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annotate texts/XML/diverse/de/Einst_Ueber_de_1902.xml @ 6:22d6a63640c6
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1 <?xml version="1.0" encoding="utf-8" ?> |
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4 <!--http://www.w3.org/TR/xhtml1/DTD/xhtml1-transitional.dtd--> |
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5 <html> |
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7 <head><title></title> |
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8 <meta http-equiv="Content-Type" content="text/html; charset=iso-8859-1" /> |
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9 <meta name="generator" content="TeX4ht (http://www.cse.ohio-state.edu/~gurari/TeX4ht/mn.html)" /> |
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10 <meta name="originator" content="TeX4ht (http://www.cse.ohio-state.edu/~gurari/TeX4ht/mn.html)" /> |
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11 <!-- xhtml,html --> |
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12 <meta name="src" content="Einst_Ueber_de_1902.tex" /> |
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13 <meta name="date" content="2005-03-10 17:48:00" /> |
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14 <link rel="stylesheet" type="text/css" href="Einst_Ueber_de_1902.css" /> |
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15 </head><body > |
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17 <!--l. 17--><p class="noindent"><pb/></p> |
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18 <div class="center" > |
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19 |
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20 <!--l. 18--><p class="noindent"> |
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21 </p><!--l. 19--><p class="noindent"><span |
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22 class="cmr-12x-x-120">5. </span><span |
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23 class="cmbxti-10x-x-144">Ueber die thermodynamische Theorie </span> <br/><span |
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24 class="cmbxti-10x-x-144">der</span> |
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25 <span |
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26 class="cmbxti-10x-x-144">Potentialdifferenz zwischen Metallen und voll-</span> |
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27 <br/><span |
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28 class="cmbxti-10x-x-144">st</span><span |
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29 class="cmbxti-10x-x-144">ändig dissociirten L</span><span |
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30 class="cmbxti-10x-x-144">ösungen ihrer Salze und </span> <br/><span |
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31 class="cmbxti-10x-x-144">über</span> |
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32 <span |
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33 class="cmbxti-10x-x-144">eine elektrische Methode zur Erforschung der</span> |
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34 <br/><span |
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35 class="cmbxti-10x-x-144">Molecularkr</span><span |
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36 class="cmbxti-10x-x-144">üfte; von A. Einstein.</span></p></div> |
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37 <div class="center" > |
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38 |
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39 <!--l. 27--><p class="noindent"> |
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40 </p><!--l. 28--><p class="noindent">----------</p></div> |
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41 <div class="center" > |
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42 |
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43 <!--l. 32--><p class="noindent"> |
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44 </p><!--l. 33--><p class="noindent"><span |
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45 class="cmsy-10x-x-120">§ </span>1. Eine hypothetische Erweiterung des zweiten Hauptsatzes <br/>der mechanischen Wärmetheorie.</p></div> |
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46 <!--l. 38--><p class="indent"> Der zweite Hauptsatz der mechanischen Wärmetheorie <br/>kann auf solche physikalische Systeme Anwendung finden, die <br/>im stande sind, mit beliebiger Annäherung umkehrbare Kreis-<br/>processe zu durchlaufen. Gemäss der Herleitung dieses Satzes <br/>aus der Unmöglichkeit der Verwandlung latenter Wärme in |
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47 <br/>mechanische Energie, ist hierbei notwendige Voraussetzung, <br/>dass jene Processe realisirbar seien. Bei einer wichtigen An-<br/>wendung der mechanischen Wärmetheorie ist es aber zweifel-<br/>haft, ob dieses Postulat erfüllt ist, nämlich bei der Ver-<br/>mischung zweier oder mehrerer Gase mit Hülfe von semi-<br/>permeabeln Wänden. Auf der Voraussetzung der Realisirbarkeit <br/>dieses Vorganges basirt die thermodynamische Theorie der <br/>Dissociation der Gase und die Theorie der verdünnten Lösungen. |
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48 </p><!--l. 54--><p class="indent"> Die einzuführende Voraussetzung ist bekanntlich folgende: <br/>Zu je zwei Gasen <span |
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49 class="cmmi-12">A</span> |
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50 und <span |
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51 class="cmmi-12">B </span>sind zwei Scheidewände herstell-<br/>bar, sodass die eine durchlässig für <span |
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52 class="cmmi-12">A</span>, nicht aber für <span |
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53 class="cmmi-12">B</span>, die <br/>andere durchlässig für <span |
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54 class="cmmi-12">B</span>, nicht aber für <span |
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55 class="cmmi-12">A </span>ist. Besteht die |
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56 <br/>Mischung aus mehreren Componenten, so gestaltet sich diese <br/>Voraussetzung noch complicirter und unwahrscheinlicher. Da <br/>nun die Erfahrung die Resultate der Theorie vollständig be-<br/>stätigt hat, trotzdem wir mit Processen operirt haben, deren <br/>Realisirbarkeit wohl bezweifelt werden kann, so erhebt sich <br/>die Frage, ob nicht vielleicht der zweite Hauptsatz auf ideale <br/>Processe gewisser Art angewendet werden kann, ohne dass <br/>man mit der Erfahrung in Widerspruch gerät. |
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57 </p><!--l. 69--><p class="indent"> In diesem Sinne können wir auf Grund der gewonnenen <br/>Erfahrung jedenfalls den Satz aussprechen: Man bleibt im <br/>Einklang mit der Erfahrung, wenn man den zweiten Haupt-<br/><pb/> |
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58 </p><!--l. 76--><p class="indent"> |
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59 |
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60 </p><!--l. 77--><p class="noindent">satz auf physikalische Gemische ausdehnt, deren einzelne <br/>Componenten durch in gewissen Flächen wirkende conservative <br/>Kräfte auf gewisse Teilräume beschränkt werden. Diesen Satz <br/>verallgemeinern wir hypothetisch zu folgendem: |
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61 </p><!--l. 83--><p class="indent"> Man bleibt im Einklange mit der Erfahrung, wenn man <br/>den zweiten Hauptsatz auf physikalische Gemische anwendet, <br/>auf deren einzelne Componenten beliebige conservative Kräfte <br/>wirken. |
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62 </p><!--l. 88--><p class="indent"> Auf diese Hypothese werden wir uns im Folgenden stets <br/>stützen, auch wo es nicht absolut notwendig erscheint. |
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63 </p> |
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64 <div class="center" > |
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65 |
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66 <!--l. 92--><p class="noindent"> |
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67 </p><!--l. 93--><p class="noindent"><span |
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68 class="cmsy-10x-x-120">§ </span>2. Ueber die Abhängigkeit der elektrischen Potentialdifferenz <br/>einer vollkommen dissociirten Salzlösung und einer aus dem <br/>Lösungsmetall bestehenden Elektrode, von der Concentration der <br/>Lösung und vom hydrostatischen Druck.</p></div> |
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69 <!--l. 101--><p class="indent"> In einem cylindrischen Gefässe, dessen Axe zusammen-<br/>falle mit der <span |
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70 class="cmmi-12">z</span>-Axe eines cartesischen Coordinatensystems <br/>befinde sich ein vollkommen dissociirtes Salz in Lösung. <span |
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71 class="cmmi-12"><img |
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72 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /> do </span> <br/>sei die Anzahl der Grammmolecüle des Salzes, welche sich <br/>im Volumenelemente <span |
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73 class="cmmi-12">do </span>gelöst finden, <span |
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74 class="cmmi-12"><img |
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75 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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76 class="cmmi-8">m</span></sub> <span |
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77 class="cmmi-12">do </span>die Anzahl der <br/>Metallionen, <span |
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78 class="cmmi-12"><img |
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79 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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80 class="cmmi-8">s</span></sub> <span |
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81 class="cmmi-12">do </span>die Anzahl der Säureionen daselbst, wobei <br/><span |
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82 class="cmmi-12"><img |
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83 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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84 class="cmmi-8">m</span></sub> und <span |
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85 class="cmmi-12"><img |
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86 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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87 class="cmmi-8">s</span></sub> ganzzahlige Vielfache von <span |
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88 class="cmmi-12"><img |
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89 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span> |
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90 sind, sodass die Gleichungen <br/>bestehen:</p> |
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91 <center class="par-math-display" > |
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92 <img |
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93 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_19020x.png" alt="nm = nm .n , " class="par-math-display" /></center> |
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94 <!--l. 115--><p class="nopar"></p> |
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95 <center class="par-math-display" > |
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96 <img |
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97 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_19021x.png" alt="ns = ns.n . " class="par-math-display" /></center> |
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98 <!--l. 120--><p class="nopar"></p><!--l. 124--><p class="noindent">Ferner sei <span |
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99 class="cmmi-12">n.<img |
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100 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" />.E.do </span>die Grösse der gesamten positiven elektri-<br/>schen Ionenladung in <span |
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101 class="cmmi-12">do</span>, also auch, bis auf unendlich Kleines, <br/>die Grösse der negativen. <span |
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102 class="cmmi-12">n </span>ist dabei die Summe der Wertig-<br/>keiten der Metallionen des Molecüls, <span |
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103 class="cmmi-12">E</span> |
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104 die Elektricitätsmenge, <br/>welche zur elektrolytischen Ausscheidung eines Grammmolecüles <br/>eines einwertigen Ions erforderlich ist. |
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105 </p><!--l. 133--><p class="indent"> Diese Gleichungen gelten jedenfalls, da die Anzahl der <br/>überzähligen Ionen einer Gattung zu vernachlässigen sein wird. |
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106 </p><!--l. 137--><p class="indent"> Wir wollen ferner annehmen, dass auf die Metall- bez. <br/>Säureionen eine äussere conservative Kraft wirke, deren Potential <br/>pro Ion die Grösse <span |
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107 class="cmmi-12">P</span><sub ><span |
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108 class="cmmi-8">m</span></sub> bez. <span |
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109 class="cmmi-12">P</span><sub ><span |
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110 class="cmmi-8">s</span></sub> |
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111 besitze. Wir vernachlässigen <br/>ferner die Veränderlichkeit der Dichte des Lösungsmittels mit <br/>dem Druck und der Dichte des gelösten Salzes, und nehmen |
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112 <br/><pb/> |
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113 |
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114 </p><!--l. 147--><p class="indent"> |
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115 |
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116 </p><!--l. 148--><p class="noindent">an, dass auf die Teile des Lösungsmittels ebenfalls eine con-<br/>servative Kraft wirke, deren Potential pro Grammäquivalent <br/>des Lösungsmittels die Grösse <span |
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117 class="cmmi-12">P</span><sub ><span |
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118 class="cmr-8">0</span></sub> |
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119 besitze, wobei <span |
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120 class="cmmi-12"><img |
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121 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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122 class="cmr-8">0</span></sub> <span |
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123 class="cmmi-12">do </span>Gramm-<br/>molecüle des Lösungsmittels in <span |
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124 class="cmmi-12">do </span>vorhanden seien. |
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125 </p><!--l. 154--><p class="indent"> Alle die Kräftefunctionen seien lediglich von der <span |
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126 class="cmmi-12">z</span>-Coordi-<br/>nate abhängig, und das System befinde sich im elektrischen, <br/>thermischen und mechanischen Gleichgewicht. Es werden dann <br/>die Grössen: Concentration <span |
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127 class="cmmi-12"><img |
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128 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span>, das elektrische Potential <span |
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129 class="cmmi-12"><img |
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130 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-19.png" alt="p" class="12x-x-19" /></span>, <br/>osmotische Drucke der beiden Ionengattungen <span |
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131 class="cmmi-12">p</span><sub ><span |
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132 class="cmmi-8">m</span></sub> und <span |
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133 class="cmmi-12">p</span><sub ><span |
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134 class="cmmi-8">s</span></sub>, hydro-<br/>statischer Druck <span |
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135 class="cmmi-12">p</span><sub ><span |
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136 class="cmmi-8">o</span></sub> nur Functionen von <span |
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137 class="cmmi-12">z </span>sein. |
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138 </p><!--l. 163--><p class="indent"> Es müssen nun an jeder Stelle des Elektrolyten die beiden <br/>Elektronengattungen für sich im Gleichgewicht sein, was durch <br/>die Gleichungen ausgedrückt wird: |
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139 </p> |
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140 <center class="par-math-display" > |
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141 <img |
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142 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_19022x.png" alt=" dpm 1 dPm dp - -----.--- nm ------- n E ---= 0, d z n dz dz " class="par-math-display" /></center> |
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143 <!--l. 171--><p class="nopar"></p> |
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144 <center class="par-math-display" > |
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145 <img |
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146 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_19023x.png" alt="- -dps-.1-- ns-d-Ps- + nE dp-= 0, d z n dz dz " class="par-math-display" /></center> |
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147 <!--l. 179--><p class="nopar"></p><!--l. 183--><p class="noindent">dabei ist:</p> |
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148 <center class="par-math-display" > |
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149 <img |
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150 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_19024x.png" alt="pm = n .nm .R T , " class="par-math-display" /></center> |
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151 <!--l. 189--><p class="nopar"></p> |
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152 <center class="par-math-display" > |
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153 <img |
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154 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_19025x.png" alt="ps = n .ns .R T , " class="par-math-display" /></center> |
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155 <!--l. 196--><p class="nopar"></p><!--l. 200--><p class="noindent">wo <span |
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156 class="cmmi-12">R </span>eine für alle Ionenarten gemeinsame Constante ist. Die <br/>Gleichungen nehmen also die Form an:</p> |
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157 <table width="100%" |
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158 class="equation"><tr><td><a |
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159 id="x1-2r1"></a> |
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160 <center class="math-display" > |
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161 <img |
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162 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_19026x.png" alt=" n R T d-lg-n + n dPm--+ n E d-p = 0 , { m dz m dz d z d lg n dPs dp ns R T ------+ ns----- - n E --- = 0, dz d z dz " class="math-display" /></center></td><td width="5%">(1)</td></tr></table> |
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163 <!--l. 211--><p class="nopar"> |
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164 </p><!--l. 214--><p class="noindent">Sind <span |
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165 class="cmmi-12">P</span><sub ><span |
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166 class="cmmi-8">m</span></sub> und <span |
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167 class="cmmi-12">P</span><sub ><span |
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168 class="cmmi-8">s</span></sub> für alle <span |
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169 class="cmmi-12">z</span>, sowie <span |
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170 class="cmmi-12"><img |
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171 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /> </span>und <span |
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172 class="cmmi-12"><img |
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173 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-19.png" alt="p" class="12x-x-19" /> </span>für ein bestimmtes <span |
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174 class="cmmi-12">z </span> <br/>bekannt, so liefern die Gleichungen (1) <span |
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175 class="cmmi-12"><img |
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176 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /> </span>und <span |
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177 class="cmmi-12"><img |
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178 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-19.png" alt="p" class="12x-x-19" /> </span>als Functionen <br/>von <span |
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179 class="cmmi-12">z. </span>Auch ergäbe die Bedingung, dass sich die Lösung als <br/>Ganzes im Gleichgewicht befindet, eine Gleichung zur Be-<br/>stimmung des hydrostatischen Druckes <span |
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180 class="cmmi-12">p</span><sub ><span |
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181 class="cmmi-8">o</span></sub>, die nicht angeschrieben <br/>zu werden braucht. Wir bemerken nur, dass <span |
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182 class="cmmi-12">dp</span><sub ><span |
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183 class="cmmi-8">o</span></sub> von <span |
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184 class="cmmi-12">d<img |
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185 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /> </span> <br/>und <span |
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186 class="cmmi-12">d<img |
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187 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-19.png" alt="p" class="12x-x-19" /> </span>deshalb unabhängig ist, weil es uns freisteht, beliebige <br/>conservative Kräfte anzunehmen, welche auf die Molecüle des <br/>Lösungsmittels wirken. |
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188 </p><!--l. 226--><p class="indent"> Wir denken uns nun in <span |
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189 class="cmmi-12">z </span>= <span |
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190 class="cmmi-12">z</span><sub ><span |
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191 class="cmr-8">1</span></sub> und <span |
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192 class="cmmi-12">z </span>= <span |
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193 class="cmmi-12">z</span><sub ><span |
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194 class="cmr-8">2</span></sub> Elektroden in <br/>die Lösung eingeführt, welche aus dem Lösungsmetalle be-<br/>stehen, und nur einen verschwindend kleinen Teil des Quer-<br/>schnittes des cylindrischen Gefässes ausfüllen sollen. Lösung |
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195 <br/><pb/> |
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196 </p><!--l. 235--><p class="indent"> |
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197 |
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198 </p><!--l. 236--><p class="noindent">und Elektroden zusammen bilden ein physikalisches System, <br/>welches wir folgenden umkehrbaren isothermischen Kreisprocess <br/>ausführen lassen: |
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199 </p><!--l. 240--><p class="indent"> 1. Teilprocess: Wir lassen die Elektricitätsmenge <span |
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200 class="cmti-12">n E un- </span> <br/><span |
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201 class="cmti-12">endlich langsam</span> |
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202 durch die Lösung passiren, indem wir die in <br/><span |
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203 class="cmmi-12">z </span>= <span |
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204 class="cmmi-12">z</span><sub ><span |
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205 class="cmr-8">1</span></sub> bez. <span |
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206 class="cmmi-12">z </span>= <span |
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207 class="cmmi-12">z</span><sub ><span |
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208 class="cmr-8">2</span></sub> befindliche Elektrode als Anode bez. Kathode <br/>verwenden. |
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209 </p><!--l. 245--><p class="indent"> 2. Teilprocess: Wir bewegen die hierbei elektrolytisch von <br/><span |
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210 class="cmmi-12">z</span><sub ><span |
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211 class="cmr-8">1</span></sub> nach <span |
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212 class="cmmi-12">z</span><sub ><span |
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213 class="cmr-8">2</span></sub> bewegte Metallmenge mechanisch in der Lösung <br/>unendlich langsam wieder von <span |
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214 class="cmmi-12">z</span><sub ><span |
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215 class="cmr-8">2</span></sub> nach |
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216 <span |
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217 class="cmmi-12">z</span><sub ><span |
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218 class="cmr-8">1</span></sub>. |
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219 </p><!--l. 250--><p class="indent"> Man ersieht zunächst, dass der Process strenge umkehr-<br/>bar ist, da alle Vorgänge unendlich langsam vor sich gehend <br/>gedacht werden, derselbe also aus (idealen) Gleichgewichts-<br/>zuständen zusammengesetzt ist. Der zweite Hauptsatz ver-<br/>langt für einen solchen Process, dass die Summe der dem <br/>System während des Kreisprocesses zugeführten Wärmemengen <br/>verschwinde. Der erste Hauptsatz verlangt in Verbindung mit <br/>dem zweiten, dass die Summe der übrigen Energien, welche <br/>dem System während des Kreisprocesses zugeführt werden, |
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220 <br/>verschwinde. |
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221 </p><!--l. 262--><p class="indent"> Während des ersten Teilprocesses wird die elektrische <br/>Arbeitsmenge zugeführt:</p> |
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222 <center class="par-math-display" > |
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223 <img |
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224 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_19027x.png" alt="- n E (TT2 - TT1) , " class="par-math-display" /></center> |
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225 <!--l. 268--><p class="nopar"> |
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226 </p><!--l. 272--><p class="noindent">wobei <img |
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227 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmr12-5.png" alt="TT" class="12x-x-5" /><sub ><span |
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228 class="cmr-8">2</span></sub> und <img |
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229 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmr12-5.png" alt="TT" class="12x-x-5" /><sub ><span |
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230 class="cmr-8">1</span></sub> die elektrischen Potentiale der Elektroden <br/>bedeuten. |
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231 </p><!--l. 275--><p class="indent"> Während des zweiten Teilprocesses wird: |
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232 </p> |
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233 <center class="par-math-display" > |
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234 <img |
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235 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_19028x.png" alt=" z integral 1 K d z z |
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236 2 " class="par-math-display" /></center> |
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237 <!--l. 280--><p class="nopar"> |
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238 </p><!--l. 284--><p class="noindent">zugeführt, wobei <span |
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239 class="cmmi-12">K </span>die in der positiven <span |
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240 class="cmmi-12">z</span>-Richtung wirkende <br/>Kraft bedeutet, welche notwendig ist, um die zu bewegenden <span |
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241 class="cmmi-12">n</span><sub ><span |
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242 class="cmmi-8">m</span></sub> <br/>Metallionen, welche sich jetzt im metallischen Zustande be-<br/>finden, an der beliebigen Stelle <span |
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243 class="cmmi-12">z </span>in Ruhe zu erhalten. Für <span |
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244 class="cmmi-12">K </span> <br/>gilt, wie leicht ersichtlich die Gleichung: |
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245 </p> |
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246 <center class="par-math-display" > |
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247 <img |
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248 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_19029x.png" alt=" dP d p K - nm ---m-- nm vm---o = 0 . dz dz " class="par-math-display" /></center> |
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249 <!--l. 296--><p class="nopar"> |
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250 |
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251 </p><!--l. 300--><p class="noindent">Dabei bedeutet <span |
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252 class="cmmi-12">v</span><sub ><span |
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253 class="cmmi-8">m</span></sub> das Volumen eines Metallions im metalli-<br/>schen Zustande. Jene Arbeit erhält also den Wert: <pb/> |
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254 </p><!--l. 306--><p class="indent"> |
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255 |
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256 </p> |
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257 <center class="par-math-display" > |
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258 <img |
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259 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190210x.png" alt=" integral z1 integral z2( ) K .d z = - n dPm--+ n v dpo- d z m dz m m d z z0 z1 [( ) ( )] = - nm Pm - Pm + vm po - po , 2 1 2 1 " class="par-math-display" /></center> |
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260 <!--l. 315--><p class="nopar"> |
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261 </p><!--l. 318--><p class="noindent">wobei der zweite Index die Coordinate der Elektrode bezeichnet. |
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262 </p><!--l. 321--><p class="indent"> Wir erhalten also die Gleichung:</p> |
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263 <table width="100%" |
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264 class="equation"><tr><td><a |
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265 id="x1-3r2"></a> |
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266 <center class="math-display" > |
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267 <img |
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268 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190211x.png" alt="n .E .(TT2 - TT1) = - nm (Pm2 - Pm1) - nm vm(po2 - po1). " class="math-display" /></center></td><td width="5%">(2)</td></tr></table> |
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269 <!--l. 327--><p class="nopar"> |
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270 </p><!--l. 330--><p class="indent"> Bezeichnet man mit <span |
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271 class="cmmi-12"><img |
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272 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-19.png" alt="p" class="12x-x-19" /></span><sub ><span |
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273 class="cmr-8">1</span></sub> und <span |
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274 class="cmmi-12"><img |
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275 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-19.png" alt="p" class="12x-x-19" /></span><sub ><span |
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276 class="cmr-8">2</span></sub> die elektrischen Potentiale, <br/>welche in den Elektrodenquerschnitten im Innern der Lösung <br/>herrschen, so erhält man durch Integration aus der ersten <br/>Gleichung (1): |
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277 </p> |
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278 <center class="par-math-display" > |
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279 <img |
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280 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190212x.png" alt=" ( ) - n .E (p - p ) = n [P - P ] + n R T log n2- , 2 1 m m2 m1 m n1 " class="par-math-display" /></center> |
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281 <!--l. 339--><p class="nopar"> |
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282 </p><!--l. 343--><p class="noindent">wobei sich <span |
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283 class="cmmi-12"><img |
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284 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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285 class="cmr-8">1</span></sub> und <span |
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286 class="cmmi-12"><img |
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287 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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288 class="cmr-8">2</span></sub> wieder auf die Elektrodenquerschnitte <br/>beziehen. Durch Addition dieser Gleichungen erhält man:</p> |
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289 <table width="100%" |
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290 class="equation"><tr><td><a |
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291 id="x1-4r3"></a> |
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292 |
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293 <center class="math-display" > |
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294 <img |
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295 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190213x.png" alt=" (TT2 - p2)- (TT1 - p1) = (D II)2 - (D TT)1 { ( ) = nm--R-T log n2- - nm-vm-(p - p ). n E n1 nE o2 o1 " class="math-display" /></center></td><td width="5%">(3)</td></tr></table> |
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296 <!--l. 356--><p class="nopar"> |
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297 </p><!--l. 360--><p class="noindent">Da die <span |
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298 class="cmmi-12"><img |
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299 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /> </span>und <span |
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300 class="cmmi-12">p</span><sub ><span |
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301 class="cmmi-8">o</span></sub> vollständig unabhängig voneinander sind, <br/>so enthält diese Gleichung die Abhängigkeit der Potential-<br/>differenz <img |
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302 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmr12-1.png" alt="D" class="12x-x-1" /> <img |
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303 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmr12-5.png" alt="TT" class="12x-x-5" /> zwischen Metall und Lösung von Concentration <br/>und hydrostatischem Druck. Es ist zu bemerken, dass die <br/>angenommenen Kräfte im Resultat nicht mehr vorkommen. <br/>Kämen sie vor, so wäre die <span |
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304 class="cmsy-10x-x-120">§ </span>1 aufgestellte Hypothese ad |
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305 <br/>absurdum geführt. Die gefundene Gleichung lässt sich in <br/>zwei zerlegen, nämlich:</p> |
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306 <table width="100%" |
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307 class="equation"><tr><td><a |
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308 id="x1-5r4"></a> |
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309 <center class="math-display" > |
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310 <img |
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311 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190214x.png" alt=" ( ) (D TT)2 - (D TT)1 = nm-R--T log n2- beiconst.Druck, { n E n1 n v (D TT)p - (D TT)1 = - --m -m(po2 - po1)beiconst.Concentration . n E " class="math-display" /></center></td><td width="5%">(4)</td></tr></table> |
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312 <!--l. 380--><p class="nopar"> |
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313 </p><!--l. 384--><p class="noindent">Man hätte die Endformel (3) auch erhalten, ohne die in <span |
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314 class="cmsy-10x-x-120">§ </span>1 <br/>vorgeschlagene Hypothese, wenn man die äusseren Kräfte mit <br/>der Erdschwere identificirt hätte. Dann wären aber <span |
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315 class="cmmi-12"><img |
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316 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /> </span>und <span |
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317 class="cmmi-12">p</span><sub ><span |
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318 class="cmmi-8">o</span></sub> <br/>nicht unabhängig voneinander und eine Zerlegung in die <br/>Gleichungen (4) wäre nicht erlaubt. |
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319 </p><!--l. 391--><p class="indent"> Es soll noch kurz erwähnt werden, dass die Nernst’sche <br/>Theorie der elektrischen Kräfte im Innern dissociirter Elektro-<br/><pb/> |
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320 </p><!--l. 397--><p class="indent"> |
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321 |
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322 </p><!--l. 398--><p class="noindent">lyte in Verbindung mit der ersten der Gleichungen (4) die <br/>elektromotorische Kraft des Concentrationselementes zu be-<br/>rechnen gestattet. Man gelangt so zu einem bereits mehrfach <br/>geprüften Resultat, welches bis jetzt aus speciellen Annahmen |
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323 <br/>hergeleitet wurde. |
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324 </p> |
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325 <div class="center" > |
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326 |
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327 <!--l. 405--><p class="noindent"> |
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328 </p><!--l. 406--><p class="noindent"><span |
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329 class="cmsy-10x-x-120">§ </span>3. Ueber die Abhängigkeit der Grösse <img |
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330 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmr12-1.png" alt="D" class="12x-x-1" /> <img |
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331 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmr12-5.png" alt="TT" class="12x-x-5" /> von der Natur <br/>der Säure.</p></div> |
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332 Wir betrachten folgenden idealen Gleichgewichtszustand: <br/>Sei wieder ein cylindrisches Gefäss vorhanden. In den Teilen <span |
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333 class="cmmi-12">I </span> <br/>und <span |
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334 class="cmti-12">II </span>mögen sich vollstän-<br/>dig dissociirte Salzlösungen <br/>befinden mit identischem <br/>Metallion (gleiches Metall <br/>und gleiche elektrische La-<br/>dung), aber verschiedenem <br/>Säureion. Zwischen den <br/>beiden befinde sich der Ver-<br/>bindungsraum <span |
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335 class="cmmi-12">V </span>, in welchem |
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336 <br/>beide Salze gelöst vorkommen. In <span |
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337 class="cmmi-12">V </span>mögen auf die Säureionen |
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338 <br/>Kräfte wirken, deren Potentiale <span |
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339 class="cmmi-12">P</span><sub><span |
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340 class="cmmi-8">s</span></sub><sup><span |
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341 class="cmr-8">(1)</span></sup><img |
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342 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190215x.png" alt="PIC" class="graphics" width="184.9429pt" height="125.78271pt" /><!--tex4ht:graphics |
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343 name="img/Einst_Ueber_de_190215x.png" src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/Einst_Ueber_de_1902_001.EPS" |
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344 --> |
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345 und <span |
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346 class="cmmi-12">P</span><sub><span |
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347 class="cmmi-8">s</span></sub><sup><span |
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348 class="cmr-8">(2)</span></sup> nur von <span |
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349 class="cmmi-12">z </span>abhängen, <br/>welche Kräfte bewirken sollen, dass nur unendlich wenig Säure-<br/>ionen erster Art in <span |
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350 class="cmti-12">II</span>, zweiter Art in 1 gelangen. Ausserdem <br/>seien <span |
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351 class="cmmi-12">P</span><sub><span |
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352 class="cmmi-8">s</span></sub><sup><span |
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353 class="cmr-8">(1)</span></sup> und <span |
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354 class="cmmi-12">P</span><sub> |
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355 <span |
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356 class="cmmi-8">s</span></sub><sup><span |
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357 class="cmr-8">(2)</span></sup> so gewählt, dass die Concentration der |
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358 <br/>Metallionen in den beiden Teilen <span |
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359 class="cmmi-12">I </span>und <span |
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360 class="cmti-12">II </span>die gleiche sei. <br/>Ebenso sei |
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361 <span |
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362 class="cmmi-12">p</span><sub ><span |
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363 class="cmmi-8">o</span><sub ><span |
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364 class="cmr-6">1</span></sub></sub> = <span |
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365 class="cmmi-12">p</span><sub ><span |
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366 class="cmmi-8">o</span><sub ><span |
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367 class="cmr-6">2</span></sub></sub> |
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368 <!--l. 435--><p class="indent"> Es seien <span |
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369 class="cmmi-12"><img |
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370 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub><span |
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371 class="cmmi-8">m</span></sub><sup><span |
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372 class="cmr-8">(1)</span></sup> Metallionen in der Volumeneinheit, welche <br/>der ersten, <span |
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373 class="cmmi-12"><img |
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374 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub> |
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375 <span |
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376 class="cmmi-8">m</span></sub><sup><span |
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377 class="cmr-8">(2)</span></sup>, welche der zweiten Satzart entsprechen, dann ist:</p> |
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378 <table width="100%" |
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379 class="equation"><tr><td><a |
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380 id="x1-6r1"></a> |
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381 <center class="math-display" > |
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382 <img |
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383 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190216x.png" alt="n(m1)1 = n(m22), n(s21)= 0 , n(s1)2 = 0 , " class="math-display" /></center></td><td width="5%">(1)</td></tr></table> |
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384 <!--l. 445--><p class="nopar"> |
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385 |
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386 </p><!--l. 449--><p class="noindent">wobei die unteren Indices die Zugehörigkeit zu Raum <span |
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387 class="cmmi-12">I </span>bez. <br/>Raum <span |
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388 class="cmti-12">II</span> |
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389 bezeichnet. |
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390 </p><!--l. 452--><p class="indent"> In <span |
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391 class="cmmi-12">V </span>erhält man aber als Gleichgewichtsbedingung der <br/>Metallionen: |
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392 </p> |
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393 <center class="par-math-display" > |
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394 <img |
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395 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190217x.png" alt=" ( ) d log n(1) + n(2) --------m-----m--- d-p - R T d z - eE d z = 0 , " class="par-math-display" /></center> |
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396 <!--l. 460--><p class="nopar"> |
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397 </p><!--l. 464--><p class="noindent">wobei <span |
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398 class="cmmi-12"><img |
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399 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-22.png" alt="e" class="12x-x-22" /> </span>die Wertigkeit des Metallions bedeutet. <pb/> |
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400 </p><!--l. 470--><p class="indent"> |
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401 |
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402 </p><!--l. 471--><p class="indent"> Durch Integration über <span |
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403 class="cmmi-12">V </span>und Berücksichtigung der <br/>Gleichungen (1) ergiebt sich:</p> |
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404 <table width="100%" |
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405 class="equation"><tr><td><a |
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406 id="x1-7r2"></a> |
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407 <center class="math-display" > |
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408 <img |
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409 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190218x.png" alt="p2 = p1 . " class="math-display" /></center></td><td width="5%">(2)</td></tr></table> |
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410 <!--l. 477--><p class="nopar"> |
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411 </p><!--l. 480--><p class="noindent">Wir bilden ferner, nachdem wir in <span |
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412 class="cmmi-12">I </span>und <span |
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413 class="cmti-12">II </span>Elektroden aus <br/>Lösungsmetall eingesetzt denken, folgenden idealen Kreisprocess: |
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414 </p><!--l. 484--><p class="indent"> 1. Teilprocess: Wir schicken durch das System unendlich <br/>langsam die Elektricitätsmenge <span |
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415 class="cmmi-12"><img |
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416 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-22.png" alt="e" class="12x-x-22" /> E</span>, indem wir die im Raum <span |
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417 class="cmmi-12">I </span> <br/>befindliche Elektrode als Anode, die andere als Kathode be-<br/>trachten. |
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418 </p><!--l. 489--><p class="indent"> 2. Teilprocess: Wir führen das so durch Elektrolyse von <br/><span |
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419 class="cmmi-12">z </span>= <span |
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420 class="cmmi-12">z</span><sub ><span |
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421 class="cmr-8">1</span></sub> nach |
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422 <span |
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423 class="cmmi-12">z </span>= <span |
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424 class="cmmi-12">z</span><sub ><span |
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425 class="cmr-8">2</span></sub> transportirte Metall, welches die Masse <br/>eines Grammäquivalentes besitzt, mechanisch wieder nach der <br/>in <span |
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426 class="cmmi-12">z </span>= <span |
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427 class="cmmi-12">z</span><sub ><span |
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428 class="cmr-8">1</span></sub> befindlichen Elektrode zurück. |
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429 </p><!--l. 495--><p class="indent"> Durch Anwendung der beiden Hauptsätze der mechani-<br/>schen Wärmetheorie folgert man wieder, dass die Summe der <br/>dem System während des Kreisprocesses zugeführten mecha-<br/>nischen und elektrischen Energie verschwindet. Da, wie leicht |
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430 <br/>ersichtlich, der zweite Teilprocess keine Energie erfordert, so <br/>erhält man die Gleichung</p> |
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431 <table width="100%" |
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432 class="equation"><tr><td><a |
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433 id="x1-8r3"></a> |
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434 <center class="math-display" > |
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435 <img |
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436 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190219x.png" alt="TT2 = TT1 , " class="math-display" /></center></td><td width="5%">(3)</td></tr></table> |
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437 <!--l. 506--><p class="nopar"> |
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438 |
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439 </p><!--l. 510--><p class="noindent">wobei <img |
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440 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmr12-5.png" alt="TT" class="12x-x-5" /><sub ><span |
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441 class="cmr-8">2</span></sub> und <img |
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442 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmr12-5.png" alt="TT" class="12x-x-5" /><sub ><span |
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443 class="cmr-8">1</span></sub> wieder die Elektrodenpotentiale bedeuten. <br/>Durch Subtraction der Gleichungen (3) und (2) erhält man: |
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444 </p> |
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445 <center class="par-math-display" > |
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446 <img |
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447 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190220x.png" alt="(TT2 - p2) - (TT1 - p1) = (D TT)2 - (D TT)1 = 0 " class="par-math-display" /></center> |
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448 <!--l. 518--><p class="nopar"> |
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449 </p><!--l. 522--><p class="noindent">und also folgenden Satz: |
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450 </p><!--l. 525--><p class="indent"> Die Potentialdifferenz zwischen einem Metall und einer <br/>vollständig dissociirten Lösung eines Salzes dieses Metalles in <br/>einem bestimmten Lösungsmittel ist unabhängig von der Natur <br/>des elektronegativen Bestandteiles, sie hängt lediglich von der <br/>Concentration der Metallionen ab. Voraussetzung ist dabei <br/>jedoch, dass bei den Salzen das Metallion mit derselben Elek-<br/>tricitätsmenge geladen ist. |
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451 </p> |
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452 <div class="center" > |
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453 |
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454 <!--l. 535--><p class="noindent"> |
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455 </p><!--l. 536--><p class="noindent"><span |
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456 class="cmsy-10x-x-120">§ </span>4.</p></div> |
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457 <!--l. 541--><p class="indent"> Bevor wir dazu übergehen, die Abhängigkeit von (<img |
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458 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmr12-1.png" alt="D" class="12x-x-1" /> <img |
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459 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmr12-5.png" alt="TT" class="12x-x-5" />) von <br/>der Natur des Lösungsmittels zu studiren, wollen wir kurz <br/>die Theorie der conservativen Molecularkräfte in Flüssigkeiten <br/>entwickeln. Ich entnehme dabei die Bezeichnungsweise einer <br/><pb/> |
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460 </p><!--l. 549--><p class="indent"> |
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461 |
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462 </p><!--l. 550--><p class="noindent">früheren Abhandlung über diesen Gegenstand<sup ><span |
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463 class="cmr-8">1</span></sup>), welche zugleich <br/>die einzuführenden Hypothesen einstweilen rechtfertigen soll. |
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464 </p><!--l. 554--><p class="indent"> Jedem Molecüle einer Flüssigkeit oder einer in einer <br/>Flüssigkeit gelösten Substanz komme eine gewisse Constante <span |
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465 class="cmmi-12">c </span> <br/>zu, sodass der Ausdruck für das relative Potential der Molecular-<br/>kräfte zweier Molecüle, welche durch die Indices |
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466 <span |
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467 class="cmmi-12">...</span><sub ><span |
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468 class="cmr-8">1</span></sub> und <span |
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469 class="cmmi-12">...</span><sub ><span |
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470 class="cmr-8">2</span></sub> <br/>charakterisirt seien, lautet:</p> |
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471 <table width="100%" |
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472 class="equation"><tr><td><a |
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473 id="x1-9r4"></a> |
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474 <center class="math-display" > |
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475 <img |
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476 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190221x.png" alt="P = Po o - c1 c2f (r), " class="math-display" /></center></td><td width="5%">(a)</td></tr></table> |
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477 <!--l. 565--><p class="nopar"> |
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478 </p><!--l. 569--><p class="noindent">wobei <span |
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479 class="cmmi-12"><img |
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480 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-27.png" alt="f" class="cmmi-12x-x-27" align="middle" /> </span>(<span |
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481 class="cmmi-12">r</span>) eine für alle Molecülarten gemeinsame Function <br/>der Entfernung sei. Jene Kräfte sollen sich einfach super-<br/>poniren, sodass der Ausdruck des relativen Potentiales von <span |
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482 class="cmmi-12">n </span> <br/>Molecülen die Form habe:</p> |
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483 <table width="100%" |
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484 class="equation"><tr><td><a |
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485 id="x1-10r4"></a> |
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486 <center class="math-display" > |
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487 <img |
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488 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190222x.png" alt=" 1a= sum n b= sum n Const. - 2 cacb f (rab). a=1 b=1 " class="math-display" /></center></td><td width="5%">(b)</td></tr></table> |
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489 <!--l. 581--><p class="nopar"> |
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490 </p><!--l. 585--><p class="noindent">Wären speciell alle Molecüle gleich beschaffen, so erhielten <br/>wir den Ausdruck:</p> |
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491 <table width="100%" |
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492 class="equation"><tr><td><a |
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493 id="x1-11r4"></a> |
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494 |
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495 <center class="math-display" > |
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496 <img |
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497 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190223x.png" alt=" 1 2a= sum n b= sum n Const. - 2 c f (rab) a=1 b=1 " class="math-display" /></center></td><td width="5%">(c)</td></tr></table> |
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498 <!--l. 594--><p class="nopar"> |
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499 </p><!--l. 599--><p class="indent"> Ferner sei das Wirkungsgesetz und das Verteilungsgesetz <br/>der Molecüle so beschaffen, dass die Summen in Integrale <br/>verwandelt werden dürfen, dann geht dieser Ausdruck über in: |
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500 </p> |
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501 <center class="par-math-display" > |
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502 <img |
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503 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190224x.png" alt=" integral integral |
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504 Const. - 1 c2N 2 dt .d t'f (rdt,dt'). 2 " class="par-math-display" /></center> |
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505 <!--l. 610--><p class="nopar"></p><!--l. 614--><p class="noindent"><span |
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506 class="cmmi-12">N </span>bedeutet dabei die Zahl der Molecüle in der Volumeneinheit. <br/>Bszeichnet <span |
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507 class="cmmi-12">N</span><sub ><span |
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508 class="cmr-8">0</span></sub> |
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509 die Anzahl der Molecüle in einem Gramm-<br/>äquivalent, so ist <span |
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510 class="cmmi-12">N</span><sub ><span |
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511 class="cmr-8">0</span></sub><span |
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512 class="cmmi-12">/N </span>= <span |
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513 class="cmmi-12">v</span> |
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514 das Molecularvolumen der Flüssig-<br/>keit, und nehmen wir an, dass ein Grammäquivalent zur Unter-<br/>suchung vorliegt, so geht, wenn wir den Einfluss der Flüssig-<br/>keitsoberfläche vernachlässigen, unser Ausdruck über in: |
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515 </p> |
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516 <center class="par-math-display" > |
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517 <img |
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518 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190225x.png" alt=" oo |
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519 1 c2 2 integral ' Const. - 2 --N 0 d t .f (ro,dt'). v - oo |
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520 " class="par-math-display" /></center> |
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521 <!--l. 628--><p class="nopar"> |
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522 </p><!--l. 632--><p class="noindent">---------- |
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523 </p><!--l. 635--><p class="indent"> 1) A. Eiustein, Ann. d. Phys. <span |
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524 class="cmbx-12">4. </span>p. 513. 1901. <pb/> |
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525 </p><!--l. 640--><p class="indent"> |
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526 |
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527 </p><!--l. 641--><p class="noindent">Wir wollen nun die Einheit der <span |
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528 class="cmmi-12">c </span>so wählen, dass dieser Aus-<br/>druck übergeht in</p> |
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529 <table width="100%" |
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530 class="equation"><tr><td><a |
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531 id="x1-12r4"></a> |
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532 <center class="math-display" > |
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533 <img |
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534 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190226x.png" alt=" 2 integral oo |
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535 c- 1 2 ' ' Const. - v , also 2 N 0 d t .f (ro, d t) = 1. - oo |
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536 " class="math-display" /></center></td><td width="5%">(d)</td></tr></table> |
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537 <!--l. 651--><p class="nopar"> |
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538 </p><!--l. 655--><p class="noindent">Durch diese Festsetzung gewinnt man für die Grössen <span |
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539 class="cmmi-12">c </span>ein <br/>absolutes Maass. In jener Abhandlung ist gezeigt, dass man <br/>mit der Erfahrung in Uebereinstimmung bleibt, wenn man <br/>setzt <span |
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540 class="cmmi-12">c </span>= <span |
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541 class="cmex-10x-x-120"><img |
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542 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmex10-c-50.png" alt=" sum " class="10-120x-x-50" /></span> |
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543 <span |
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544 class="cmmi-12">c</span><sub ><span |
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545 class="cmmi-8"><img |
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546 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi8-b.png" alt="a" class="8x-x-b" /></span></sub> , wo sich die Grössen |
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547 <span |
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548 class="cmmi-12">c</span><sub ><span |
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549 class="cmmi-8"><img |
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550 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi8-b.png" alt="a" class="8x-x-b" /></span></sub> auf die Atome be-<br/>ziehen, aus denen das Molecül zusammengesetzt ist. |
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551 </p><!--l. 663--><p class="indent"> Wir wollen nun das relative Anziehungspotential des <br/>Grammmolecüls eines Ions in Bezug auf sein Lösungsmittel <br/>berechnen, wobei wir ausdrücklich die Annahme machen, dass <br/>die Anziehungsfelder der Molecüle des Lösungsmittels nicht <br/>auf die elektrischen Ladungen der Ionen wirken. Später zu <br/>entwickelnde Methoden werden ein Mittel an die Hand geben, <br/>welches über die Zulässigkeit dieser Voraussetzung zu ent-<br/>scheiden gestattet. |
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552 </p><!--l. 673--><p class="indent"> Sei <span |
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553 class="cmmi-12">c</span><sub ><span |
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554 class="cmmi-8">j</span></sub> die moleculare Constante des Ions, <span |
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555 class="cmmi-12">c</span><sub ><span |
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556 class="cmmi-8">l</span></sub> die des Lösungs-<br/>mittels, so hat das Potential eines Molecüles des Ions gegen <br/>das Lösungsmittel die Form: |
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557 </p> |
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558 <center class="par-math-display" > |
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559 <img |
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560 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190227x.png" alt=" sum integral |
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561 Const. - cj cl.f(r) = const. - cj .clNl dt .f (ro,dt) , l " class="par-math-display" /></center> |
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562 <!--l. 683--><p class="nopar"> |
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563 </p><!--l. 687--><p class="noindent">wobei <span |
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564 class="cmmi-12">N</span><sub ><span |
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565 class="cmmi-8">l</span></sub> die Zahl der Molecüle des Lösungsmittels pro Volumen-<br/>einheit bedeutet. Da <span |
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566 class="cmmi-12">N</span><sub ><span |
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567 class="cmr-8">0</span></sub><span |
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568 class="cmmi-12">/N</span><sub ><span |
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569 class="cmmi-8">l</span></sub> = <span |
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570 class="cmmi-12">v</span><sub ><span |
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571 class="cmmi-8">l</span></sub> ist, so geht dieser Ausdruck <br/>über in: |
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572 </p> |
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573 <center class="par-math-display" > |
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574 <img |
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575 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190228x.png" alt=" N integral |
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576 Const. - cj .cl.--0 dt .f (ro, d t). vl " class="par-math-display" /></center> |
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577 <!--l. 696--><p class="nopar"> |
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578 </p><!--l. 700--><p class="noindent">Das aber das Grammäquivalent <span |
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579 class="cmmi-12">N</span><sub ><span |
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580 class="cmr-8">0</span></sub> Molecüle des Ions enthält, <br/>so erhalten wir für das relative Potential des Grammäquivalentes <br/>des Ions: |
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581 </p> |
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582 <center class="par-math-display" > |
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583 <img |
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584 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190229x.png" alt=" integral |
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585 cj .cl 2 cj .cl Const. - ----- N 0 d t .f (ro, d t) = const.- 2----. vl vl " class="par-math-display" /></center> |
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586 <!--l. 709--><p class="nopar"> |
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587 </p><!--l. 713--><p class="noindent">Führt man die Concentration des Lösungsmittels 1<span |
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588 class="cmmi-12">/v</span><sub ><span |
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589 class="cmmi-8">l</span></sub> = <span |
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590 class="cmmi-12"><img |
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591 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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592 class="cmmi-8">l</span></sub> ein, <br/>so erhält man die Form:</p> |
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593 <table width="100%" |
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594 class="equation"><tr><td><a |
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595 id="x1-13r4"></a> |
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596 <center class="math-display" > |
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597 <img |
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598 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190230x.png" alt="Pj l = const.- 2cj .clnl. " class="math-display" /></center></td><td width="5%">(e)</td></tr></table> |
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599 <!--l. 720--><p class="nopar"> |
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600 <pb/> |
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601 </p><!--l. 727--><p class="indent"> |
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602 |
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603 </p><!--l. 728--><p class="noindent">Ist das Lösungsmittel eine Mischung mehrerer Flüssigkeiten, <br/>welche wir durch Indices unterscheiden wollen, erhalten wir</p> |
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604 <table width="100%" |
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605 class="equation"><tr><td><a |
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606 id="x1-14r4"></a> |
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607 <center class="math-display" > |
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608 <img |
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609 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190231x.png" alt=" sum |
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610 P = const.- 2 c c n , jl j l l " class="math-display" /></center></td><td width="5%">(e<sup ><span |
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611 class="cmsy-8">'</span></sup>)</td></tr></table> |
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612 <!--l. 736--><p class="nopar"> |
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613 </p><!--l. 740--><p class="noindent">wobei die <span |
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614 class="cmmi-12"><img |
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615 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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616 class="cmmi-8">l</span></sub> die Anzahl der Grammmolecüle der einzelnen <br/>Componenten des Lösungsmittels pro Volumeneinheit bedeuten. <br/>Die Formel (e<span |
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617 class="cmsy-10x-x-120">'</span>) gilt angenähert auch in dem Falle, dass die <br/>Grössen <span |
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618 class="cmmi-12"><img |
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619 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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620 class="cmmi-8">l</span></sub> mit dem Orte variiren. |
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621 </p> |
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622 <div class="center" > |
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623 |
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624 <!--l. 747--><p class="noindent"> |
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625 </p><!--l. 748--><p class="noindent"><span |
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626 class="cmsy-10x-x-120">§ </span>5. Ueber die Abhängigkeit der zwischen einem Metall und <br/>einer vollständig dissociirten Lösung eines Salzes dieses Metalles <br/>herrschenden elektrischen Potentialdifferenz von der Natur des <br/>Lösungsmittels.</p></div> |
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627 <!--l. 756--><p class="indent"> Ein cylindrisches Gefäss zerfalle wieder, wie im <span |
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628 class="cmsy-10x-x-120">§ </span>3 an-<br/>gegeben wurde, in die Räume <span |
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629 class="cmti-12">I, II </span>und den Verbindungs-<br/>raum <span |
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630 class="cmmi-12">V. </span>In <span |
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631 class="cmmi-12">I </span>befinde sich ein erstes, in <span |
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632 class="cmti-12">II </span>ein zweites <br/>Lösungsmittel, in <span |
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633 class="cmmi-12">V </span>mögen beide gemischt vorkommen und es <br/>mögen in diesem Raume auf die Lösungsmittel Kräfte wirken, <br/>welche eine Diffusion verhindern. In dem Gefässe befinde <br/>sich ein gelöstes Salz im Zustande vollständiger Dissociation. <br/>Auf die Säureionen desselben sollen in <span |
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634 class="cmmi-12">V </span>Kräfte wirken, deren <br/>Potential <span |
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635 class="cmmi-12">P</span><sub ><span |
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636 class="cmmi-8">s</span></sub> heisse und so gewählt sei, dass das Salz in <span |
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637 class="cmmi-12">I </span> <br/>und <span |
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638 class="cmti-12">II</span> |
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639 gleiche Concentration besitze. Wir stellen nun die <br/>Bedingung für das Gleichgewicht der Metallionen auf. Die <br/><span |
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640 class="cmmi-12">z</span>-Axe führen wir wieder <span |
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641 class="cmsy-10x-x-120">|| </span>der Cylinderaxe von <span |
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642 class="cmmi-12">I </span>nach <span |
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643 class="cmti-12">II</span>. |
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644 </p><!--l. 772--><p class="indent"> Als Ausdruck der auf das Grammäquivalent wirkenden <br/>Kraft elektrischen Ursprunges ergiebt sich: |
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645 </p> |
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646 <center class="par-math-display" > |
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647 <img |
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648 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190232x.png" alt=" n d p - --- E --- . nm d z " class="par-math-display" /></center> |
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649 <!--l. 778--><p class="nopar"> |
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650 </p><!--l. 782--><p class="noindent">Die auf das Aequivalent vom osmotischen Druck ausgeübte <br/>Kraft ist: |
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651 </p> |
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652 <center class="par-math-display" > |
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653 <img |
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654 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190233x.png" alt=" d-log-n - R T d z . " class="par-math-display" /></center> |
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655 <!--l. 789--><p class="nopar"> |
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656 </p><!--l. 793--><p class="noindent">Die auf das Aequivalent ausgeübte Wirkung der Molecular-<br/>kräfte ist: |
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657 </p> |
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658 <center class="par-math-display" > |
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659 <img |
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660 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190234x.png" alt=" d { (1) (1) (2) (2)} - --- - 2 cm cl nl - 2 cm cl nl , dz " class="par-math-display" /></center> |
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661 <!--l. 800--><p class="nopar"> <pb/> |
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662 </p><!--l. 807--><p class="indent"> |
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663 |
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664 </p><!--l. 808--><p class="noindent">wobei sich die oberen Indices auf die Lösungsmittel beziehen. <br/>Die gesuchte Gleichgewichtsbedingung ist also:</p> |
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665 <center class="par-math-display" > |
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666 <img |
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667 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190235x.png" alt=" n d p d log n d { } - ---E --- - R T -------+ --- 2 cm c(l1)n(l1)+ 2 cm c(l2)n(l2) = 0. nm d z dz dz " class="par-math-display" /></center> |
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668 <!--l. 817--><p class="nopar"> |
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669 </p><!--l. 821--><p class="noindent">Integrirt man durch <span |
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670 class="cmmi-12">V </span>hindurch und berücksichtigt, dass <span |
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671 class="cmmi-12"><img |
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672 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /> </span> <br/>in <span |
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673 class="cmmi-12">I </span>und <span |
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674 class="cmti-12">II </span>identisch ist, und dass <span |
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675 class="cmmi-12"><img |
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676 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub><span |
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677 class="cmmi-8">l</span></sub><sup><span |
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678 class="cmr-8">(2)</span></sup> in <span |
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679 class="cmmi-12">I </span>und <span |
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680 class="cmmi-12"><img |
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681 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub> |
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682 <span |
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683 class="cmmi-8">l</span></sub><sup><span |
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684 class="cmr-8">(1)</span></sup> in <span |
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685 class="cmti-12">II </span>nach <br/>unserer Voraussetzung verschwindet, so erhält man: |
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686 </p> |
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687 <center class="par-math-display" > |
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688 <img |
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689 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190236x.png" alt=" { } p2- p1 = nm--2-cm- c(2)n(2)- c(1)n(1) , n E l l l l " class="par-math-display" /></center> |
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690 <!--l. 832--><p class="nopar"> |
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691 </p><!--l. 836--><p class="noindent">wobei sich die oberen Indices auf Raum <span |
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692 class="cmmi-12">I </span>bez. <span |
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693 class="cmti-12">II </span>beziehen. |
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694 </p><!--l. 839--><p class="indent"> Wir denken uns nun in <span |
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695 class="cmmi-12">I </span>und <span |
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696 class="cmti-12">II </span>Elektroden angebracht, <br/>welche aus dem gelösten Metall bestehen, und bilden einen <br/>Kreisprocess, indem wir die Electricitätsmenge <span |
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697 class="cmmi-12">n/n</span><sub ><span |
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698 class="cmmi-8">m</span></sub> <span |
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699 class="cmmi-12">E </span>durch <br/>das System schicken, und dann die transportirte Metallmenge <br/>mechanisch wieder zurückbewegen, was keine Arbeit erfordert, <br/>wenn wir annehmen, dass in <span |
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700 class="cmmi-12">I </span>und <span |
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701 class="cmti-12">II </span>der hydrostatische <br/>Druck der nämliche sei. Durch Anwendung der beiden Haupt-<br/>sätze der Wärmetheorie erhält man: |
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702 </p> |
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703 <center class="par-math-display" > |
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704 <img |
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705 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190237x.png" alt="TT2 - TT1 = 0 . " class="par-math-display" /></center> |
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706 <!--l. 853--><p class="nopar"> |
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707 </p><!--l. 857--><p class="noindent">Durch Subtraction beider Resultate ergiebt sich:</p> |
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708 <center class="par-math-display" > |
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709 <img |
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710 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190238x.png" alt="(TT2 - p2)- (TT1 - p1) = (D TT)(2)- (D TT)(1) { } = - nm--2-cm- c(2)l n(2l)- c(1l)n(1l) . n E " class="par-math-display" /></center> |
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711 <!--l. 868--><p class="nopar"> |
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712 </p><!--l. 872--><p class="indent"> Ist jedes der beiden Lösungsmittel eine Mischung mehrerer <br/>nichtleitender |
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713 Flüssigkeiten, so erhält man etwas allgemeiner:</p> |
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714 <center class="par-math-display" > |
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715 <img |
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716 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190239x.png" alt=" nm 2 cm { sum (2) (2) sum (1) (1)} (D TT)(2) - (D TT)(1) = - --------- c l n l - c l n l , n E " class="par-math-display" /></center> |
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717 <!--l. 882--><p class="nopar"> |
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718 </p><!--l. 886--><p class="noindent">in welcher Formel <span |
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719 class="cmmi-12"><img |
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720 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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721 class="cmmi-8">l</span></sub> die Zahl der Grammmolecüle einer <br/>Componente des Lösungsmittels in einem Volumelemente des <br/>gemischten Lösungsmittels bezeichnet. |
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722 </p><!--l. 891--><p class="indent"> Die Potentialdifferenz <img |
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723 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmr12-1.png" alt="D" class="12x-x-1" /> <img |
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724 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmr12-5.png" alt="TT" class="12x-x-5" /> ist also von der Natur des <br/>Lösungsmittels abhängig. Auf diese Abhängigkeit lässt sich <br/>eine Methode zur Erforschung der Molecularkräfte gründen. |
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725 </p> |
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726 <div class="center" > |
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727 |
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728 <!--l. 897--><p class="noindent"> |
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729 </p><!--l. 898--><p class="noindent"><span |
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730 class="cmsy-10x-x-120">§ </span>6. Methode zur Bestimmung der Constanten <span |
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731 class="cmmi-12">c </span>für Metallionen <br/>und Lösungsmittel.</p></div> |
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732 <!--l. 903--><p class="indent"> In einem cylindrischen Gefässe seien zwei vollständig <br/>dissociirte Salzlösungen in Diffusion begriffen; diese Salze <br/><pb/> |
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733 </p><!--l. 909--><p class="indent"> |
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734 |
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735 </p><!--l. 910--><p class="noindent">seien durch untere Indices bezeichnet. Das Lösungsmittel sei <br/>im ganzen Gefäss dasselbe und werde durch den oberen Index <br/>bezeichnet. Das Gefäss zerfalle wieder in die Räume <span |
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736 class="cmti-12">I, II </span> <br/>und den Verbindungsraum <span |
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737 class="cmmi-12">V. </span>Im Raume <span |
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738 class="cmmi-12">I </span>sei nur das erste, <br/>im Raume <span |
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739 class="cmti-12">II </span>nur das zweite Salz vorhanden; im Raume <span |
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740 class="cmmi-12">V </span> <br/>finde Diffusion beider Salze statt. In die Räume <span |
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741 class="cmmi-12">I </span>und <span |
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742 class="cmti-12">II </span> <br/>seien Elektroden eingeführt, welche aus dem betreffenden <br/>Lösungsmetalle bestehen und die elektrischen Potentiale <span |
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743 class="cmti-12">II</span><sub ><span |
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744 class="cmr-8">1</span></sub> <br/>bez. <span |
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745 class="cmmi-12">II</span><sub><span |
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746 class="cmr-8">2</span></sub><sup> <span |
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747 class="cmsy-8">'</span></sup> besitzen; an die zweite Elektrode sei ein Stück des <br/>ersten Elektrodenmetalles angelötet, dessen Potential <span |
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748 class="cmmi-12">II</span><sub ><span |
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749 class="cmr-8">2</span></sub> |
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750 sei. <br/>Wir bezeichnen ausserdem die elektrischen Potentiale im <br/>Innern der unvermischten, in <span |
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751 class="cmmi-12">I </span>und <span |
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752 class="cmti-12">II </span>befindlichen Lösungen, <br/>mit <span |
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753 class="cmmi-12"><img |
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754 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-19.png" alt="p" class="12x-x-19" /></span><sub ><span |
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755 class="cmr-8">1</span></sub> und <span |
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756 class="cmmi-12"><img |
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757 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-19.png" alt="p" class="12x-x-19" /></span><sub ><span |
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758 class="cmr-8">2</span></sub>, dann ist:</p> |
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759 <center class="par-math-display" > |
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760 <img |
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761 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190240x.png" alt=" (1) ' ' (1) (1) (1) (II2 - TT1) = (TT2 - II2) + (TT2 - p2) + (p2- p1) - (TT1 - p1) . " class="par-math-display" /></center> |
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762 <!--l. 932--><p class="nopar"> |
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763 </p><!--l. 936--><p class="indent"> Stellt man ganz dieselbe Anordnung her, mit dem einzigen <br/>Unterschiede, dass man ein anderes Lösungsmittel benutzt, das <br/>durch den oberen Index<sup ><span |
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764 class="cmr-8">(2)</span></sup> bezeichnet werde, so hat man:</p> |
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765 <center class="par-math-display" > |
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766 <img |
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767 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190241x.png" alt="(TT2 - TT1)(2) = (TT2 - TT2') + (TT2' - p2)(2) + (p2 - p1)(2)- (TT1 - p1)(2). " class="par-math-display" /></center> |
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768 <!--l. 946--><p class="nopar"></p><!--l. 950--><p class="noindent">Durch Subtraction dieser beiden Ausdrücke erhält man mit <br/>Berücksichtigung des in <span |
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769 class="cmsy-10x-x-120">§ </span>5 gefundenen Resultates:</p> |
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770 <center class="par-math-display" > |
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771 <img |
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772 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190242x.png" alt=" { } (TT2 - TT1)(2)- (TT2 - TT1)(1) = (p2 - p1)(2)- (p2 - p1)(1) 2 { (c n ) (c n ) } { } - -- -m---m - -m--m- . c(2)l n(2)l- c(1)l n(1l) . E n 2 n 1 " class="par-math-display" /></center> |
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773 <!--l. 965--><p class="nopar"> |
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774 </p><!--l. 969--><p class="indent"> Die erforderliche Erweiterung für den Fall, dass die <br/>Lösungsmittel Mischungen sind, erhält man leicht wie in <span |
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775 class="cmsy-10x-x-120">§ </span>5. |
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776 </p><!--l. 973--><p class="indent"> Die Werte der linken Seite dieser Gleichung ergeben sich <br/>unmittelbar durch das Experiment. Mit der Bestimmung des <br/>ersten Gliedes der rechten Seite werden wir uns im folgenden <br/>Paragraph beschäftigen; es sei einstweilen gesagt, dass man |
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777 <br/>dies Glied aus den angewandten Concentrationen und den <br/>molecularen Leitfähigkeiten der betreffenden Ionen für das <br/>betreffende Lösungsmittel |
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778 berechnen kann, wenn man die An-<br/>ordnung in geeigneter Weise wählt. Die Gleichung erlaubt <br/>daher die Berechnung des zweiten Gliedes der rechten Seite. |
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779 </p><!--l. 985--><p class="indent"> Dies benutzen wir zur Bestimmung der Constanten <span |
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780 class="cmmi-12">c </span>für <br/>Metallionen und zur Prüfung unserer Hypothesen. Wir be-<br/>nutzen zu einer Reihe von Experimenten der geschilderten <br/><pb/> |
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781 </p><!--l. 992--><p class="indent"> |
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782 |
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783 </p><!--l. 993--><p class="noindent">Art immer dieselben beiden Lösungsmittel. Für die ganze <br/>Untersuchungsreihe ist dann die Grösse |
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784 </p> |
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785 <center class="par-math-display" > |
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786 <img |
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787 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190243x.png" alt="2 { } -- c(2l)n(2l)- c(1l)n(1)l = k = const. E |
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788 " class="par-math-display" /></center> |
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789 <!--l. 1001--><p class="nopar"> |
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790 </p><!--l. 1005--><p class="indent"> Setzt man <span |
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791 class="cmmi-12">n</span><sub ><span |
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792 class="cmr-8">1</span></sub><span |
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793 class="cmmi-12">/n</span><sub ><span |
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794 class="cmmi-8">m</span><sub ><span |
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795 class="cmr-6">1</span></sub></sub> = <span |
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796 class="cmmi-12">E</span><sub ><span |
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797 class="cmr-8">1</span></sub> etc. gleich der Wertigkeit des <br/>ersten etc. Metallions, so ist also das berechnete letzte Glied <br/>der rechten Seite ein relatives Maass für die Grösse |
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798 </p> |
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799 <center class="par-math-display" > |
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800 <img |
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801 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190244x.png" alt="( ) cm2-- cm1-- e - e . 2 1 " class="par-math-display" /></center> |
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802 <!--l. 1014--><p class="nopar"> |
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803 </p><!--l. 1018--><p class="indent"> Untersucht man so Combinationen aller Elektrodenmetalle <br/>zu Paaren, so erhält man in relativem Maass die Grössen |
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804 </p> |
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805 <center class="par-math-display" > |
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806 <img |
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807 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190245x.png" alt="{ c } -mj-- cmk-- . ej ek " class="par-math-display" /></center> |
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808 <!--l. 1025--><p class="nopar"> |
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809 </p><!--l. 1029--><p class="indent"> Man erhält in demselben Maasse die Grössen <span |
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810 class="cmmi-12">c</span><sub ><span |
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811 class="cmmi-8">m</span></sub><span |
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812 class="cmmi-12">/<img |
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813 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-22.png" alt="e" class="12x-x-22" /> </span>selbst, <br/>wenn man bei einem Metall eine analoge Untersuchung in der <br/>Weise ausführt, dass man Salze und Elektroden in <span |
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814 class="cmmi-12">I </span>und <span |
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815 class="cmti-12">II </span> <br/>von demselben Metall wählt, sodass jedoch <span |
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816 class="cmmi-12"><img |
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817 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-22.png" alt="e" class="12x-x-22" /></span>, d. h. die Wertig-<br/>keit (elektrische Ladung) des Metallions auf beiden Seiten <br/>verschieden ist. Es sind dann in jenem Maasse die Werte für <br/>die Grössen <span |
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818 class="cmmi-12">c</span><sub ><span |
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819 class="cmmi-8">m</span></sub> der einzelnen Metalle selbst ermittelbar. Eine <br/>Reihe von solchen Untersuchungen führt also auf die Ver-<br/>hältnisse der <span |
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820 class="cmmi-12">c</span><sub ><span |
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821 class="cmmi-8">m</span></sub>, d. h. der Constanten für die Molecularattraction <br/>der Metallionen. Diese Reihe der <span |
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822 class="cmmi-12">c</span><sub ><span |
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823 class="cmmi-8">m</span></sub> muss unabhängig sein <br/>von der Natur der benutzten Salze, und die Verhältnisse der <br/>so erhaltenen <span |
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824 class="cmmi-12">c</span><sub ><span |
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825 class="cmmi-8">m</span></sub> unabhängig von der Natur der beiden <br/>Lösungsmittel, welche wir für die Untersuchung zu Grunde <br/>legten. Ferner muss verlangt werden, dass <span |
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826 class="cmmi-12">c</span><sub ><span |
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827 class="cmmi-8">m</span></sub> unabhängig von |
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828 <br/>der elektrischen Ladung (Wertigkeit), in welcher ein Ion auf-<br/>tritt, sich herausstelle. Ist dies der Fall, so ist die oben ge-<br/>machte Voraussetzung richtig, dass die Molecularkräfte nicht <br/>auf die elektrischen Ladungen der Ionen wirken. |
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829 </p><!--l. 1052--><p class="indent"> Will man den Wert der Grössen <span |
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830 class="cmmi-12">c</span><sub ><span |
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831 class="cmmi-8">m</span></sub> wenigstens angenähert <br/>absolut bestimmen, so kann man dies, indem man die Grösse <span |
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832 class="cmmi-12">k </span> <br/>angenähert für die beiden Lösungsmittel aus den Resultaten <br/>der oben angeführten Abhandlung entnimmt, indem man die <br/>Formel <span |
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833 class="cmmi-12">c </span>= <span |
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834 class="cmex-10x-x-120"><img |
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835 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmex10-c-50.png" alt=" sum " class="10-120x-x-50" /></span> |
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836 <span |
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837 class="cmmi-12">c</span><sub ><span |
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838 class="cmmi-8"><img |
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839 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi8-b.png" alt="a" class="8x-x-b" /></span></sub> anwendet. Freilich ist hier zu bemerken, <br/>dass sich gerade für die als Lösungsmittel am meisten nahe-<br/>liegenden Flüssigkeiten, Wasser und Alkohol, die Gültigkeit <br/><pb/> |
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840 </p><!--l. 1064--><p class="indent"> |
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841 |
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842 </p><!--l. 1065--><p class="noindent">des Attractionsgesetzes aus den Erscheinungen der Capillarität, <br/>Verdampfung und Compressibilität nicht hat darthun lassen. |
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843 </p><!--l. 1069--><p class="indent"> Es lässt sich auf Grund unseres Ergebnisses aber ebenso-<br/>gut eine Erforschung der Constanten <span |
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844 class="cmmi-12">c</span><sub ><span |
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845 class="cmmi-8">l</span></sub> von Lösungsmitteln <br/>gründen, indem man der Untersuchung zwei Metallionen zu <br/>Grunde legt und das Lösungsmittel variiren lässt, sodass nun |
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846 <br/>die Grösse |
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847 </p> |
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848 <center class="par-math-display" > |
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849 <img |
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850 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190246x.png" alt=" {( ) ( ) } -2 cm-nm- - cm-nm- E n 2 n 1 " class="par-math-display" /></center> |
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851 <!--l. 1080--><p class="nopar"> |
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852 </p><!--l. 1084--><p class="noindent">als constant zu betrachten ist. Indem man auch Mischungen <br/>als Lösungsmittel zulässt, kann so die Untersuchung auf alle <br/>elektrisch nicht leitenden Flüssigkeiten ausgedehnt werden. <br/>Es lassen sich aus solchen Versuchen relative Werte für die |
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853 <br/>Grössen <span |
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854 class="cmmi-12">c</span><sub ><span |
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855 class="cmmi-8"><img |
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856 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi8-b.png" alt="a" class="8x-x-b" /></span></sub> herausrechnen, welche den die Flüssigkeitsmolecüle <br/>bildenden Atomen zukommen. Auch hier bietet sich eine Fülle <br/>von Prüfungen für die Theorie, indem die <span |
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857 class="cmmi-12">c</span><sub ><span |
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858 class="cmmi-8">a</span></sub> beliebig über-<br/>bestimmt werden können. Ebenso muss das Resultat unab-<br/>hängig sein von der Wahl der Metallionen. |
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859 </p> |
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860 <div class="center" > |
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861 |
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862 <!--l. 1098--><p class="noindent"> |
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863 </p><!--l. 1099--><p class="noindent"><span |
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864 class="cmsy-10x-x-120">§ </span>7. Berechnung von (<span |
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865 class="cmmi-12"><img |
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866 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-19.png" alt="p" class="12x-x-19" /></span><sub ><span |
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867 class="cmr-8">2</span></sub> <span |
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868 class="cmsy-10x-x-120">- </span><span |
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869 class="cmmi-12"><img |
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870 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-19.png" alt="p" class="12x-x-19" /></span><sub ><span |
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871 class="cmr-8">1</span></sub>)<span |
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872 class="cmmi-12">.</span></p></div> |
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873 <!--l. 1103--><p class="indent"> Wir haben nun noch den Diffusionsvorgang im Raume <span |
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874 class="cmmi-12">V </span> <br/>genauer zu studiren. Die variabeln Grössen seien nur von <span |
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875 class="cmmi-12">z </span> <br/>abhängig, wobei die <span |
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876 class="cmmi-12">z</span>-Axe des von uns gewählten cartesischen <br/>Coordinatensystems mit der Richtung der Axe unseres Ge-<br/>fässes zusammenfalle. <span |
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877 class="cmmi-12"><img |
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878 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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879 class="cmmi-8">m</span><sub ><span |
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880 class="cmr-6">1</span></sub></sub>, <span |
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881 class="cmmi-12"><img |
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882 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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883 class="cmmi-8">s</span><sub ><span |
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884 class="cmr-6">1</span></sub></sub>, <span |
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885 class="cmmi-12"><img |
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886 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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887 class="cmmi-8">m</span><sub ><span |
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888 class="cmr-6">2</span></sub></sub>, <span |
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889 class="cmmi-12"><img |
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890 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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891 class="cmmi-8">s</span><sub ><span |
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892 class="cmr-6">2</span></sub></sub> seien die von <span |
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893 class="cmmi-12">z </span>ab-<br/>hängigen Concentrationen (Grammäquivalente pro Volumen-<br/>einheit) der vier Ionengattungen, <span |
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894 class="cmmi-12"><img |
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895 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-22.png" alt="e" class="12x-x-22" /></span><sub ><span |
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896 class="cmmi-8">m</span><sub ><span |
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897 class="cmr-6">1</span></sub></sub> <span |
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898 class="cmmi-12">E, </span><span |
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899 class="cmsy-10x-x-120">-</span><span |
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900 class="cmmi-12"><img |
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901 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-22.png" alt="e" class="12x-x-22" /></span><sub ><span |
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902 class="cmmi-8">s</span><sub ><span |
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903 class="cmr-6">1</span></sub></sub> <span |
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904 class="cmmi-12">E, <img |
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905 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-22.png" alt="e" class="12x-x-22" /></span><sub ><span |
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906 class="cmmi-8">m</span><sub ><span |
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907 class="cmr-6">2</span></sub></sub> <span |
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908 class="cmmi-12">E, </span><span |
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909 class="cmsy-10x-x-120">-</span><span |
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910 class="cmmi-12"><img |
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911 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-22.png" alt="e" class="12x-x-22" /></span><sub ><span |
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912 class="cmmi-8">s</span><sub ><span |
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913 class="cmr-6">2</span></sub></sub> <span |
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914 class="cmmi-12">E </span> <br/>die elektrischen Ladungen, welche dieselben tragen; <span |
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915 class="cmmi-12"><img |
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916 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-19.png" alt="p" class="12x-x-19" /></span>; sei das <br/>elektrische Potential. Da nirgends beträchtliche elektrische <br/>Ladungen auftreten, so ist für alle <span |
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917 class="cmmi-12">z</span> |
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918 nahezu:</p> |
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919 <table width="100%" |
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920 class="equation"><tr><td><a |
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921 id="x1-15r4"></a> |
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922 <center class="math-display" > |
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923 <img |
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924 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190247x.png" alt="nm1 em1 - ns1 es1 + nm2 em2 - ns2 es2 = 0. " class="math-display" /></center></td><td width="5%">(<span |
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925 class="cmmi-12"><img |
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926 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-b.png" alt="a" class="12x-x-b" /></span>)</td></tr></table> |
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927 <!--l. 1124--><p class="nopar"> |
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928 </p><!--l. 1127--><p class="indent"> Ausserdem erhalten wir für jede Ionenart eine Gleichung, <br/>welche ausdrückt, dass die Vermehrung der Zahl der in einem <br/>Volumenelement befindlichen Ionen bestimmter Gattung pro <br/>Zeiteinheit gleich ist der Differenz der in dieser Zeit ins |
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929 <br/>Volumenelement eintretenden und der in derselben Zeit aus <br/>ihm austretenden Molecüle: <pb/> |
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930 </p><!--l. 1137--><p class="indent"> |
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931 |
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932 </p> |
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933 <table width="100%" |
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934 class="equation"><tr><td><a |
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935 id="x1-16r4"></a> |
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936 <center class="math-display" > |
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937 <img |
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938 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190248x.png" alt=" { } v .@-- R T -@ nm-1-+ e n E -@-p = -@-nm1-, m 1 @ z @ z m 1 m 1 @ z @ t { } { vs1 .@-- R T @-ns1-- es1 ns 1 E @-p = @-ns1-, @ z @ z @ z @ t . . . . . . . . . . . . . . . . . |
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939 . . . . . . . . . . . . . . . . . " class="math-display" /></center></td><td width="5%">(<span |
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940 class="cmmi-12"><img |
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941 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-c.png" alt="b" class="cmmi-12x-x-c" align="middle" /></span>)</td></tr></table> |
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942 <!--l. 1158--><p class="nopar"> |
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943 </p><!--l. 1161--><p class="noindent">wobei <span |
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944 class="cmmi-12">v </span>mit dem betreffenden Index die constante Ge-<br/>schwindigkeit bedeutet, welche die mechanische Krafteinheit <br/>dem Grammäquivalent des betreffenden Ions in der Lösung <br/>erteilt. |
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945 </p><!--l. 1166--><p class="indent"> Diese vier Gleichungen bestimmen im Verein mit den <br/>Grenzbedingungen den stattfindenden Vorgang vollständig, da <br/>sie für jeden Zeitmoment die fünf Grössen |
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946 </p> |
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947 <center class="par-math-display" > |
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948 <img |
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949 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190249x.png" alt="@-p- @-nm1- @-ns2 @ z , @ t ... @ t " class="par-math-display" /></center> |
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950 <!--l. 1175--><p class="nopar"> |
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951 </p><!--l. 1179--><p class="noindent">in eindeutiger Weise zu berechnen gestatten. Die allgemeine <br/>Behandlung des Problemes wäre aber mit sehr grossen <br/>Schwierigkeiten verknüpft, zumal Gleichungen (<span |
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952 class="cmmi-12"><img |
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953 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-c.png" alt="b" class="cmmi-12x-x-c" align="middle" /></span>) nicht linear <br/>in den Unbekannten sind. Uns kommt es aber nur auf die <br/>Bestimmung von <span |
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954 class="cmmi-12"><img |
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955 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-19.png" alt="p" class="12x-x-19" /></span><sub ><span |
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956 class="cmr-8">2</span></sub> <span |
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957 class="cmsy-10x-x-120">- </span><span |
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958 class="cmmi-12"><img |
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959 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-19.png" alt="p" class="12x-x-19" /></span><sub ><span |
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960 class="cmr-8">1</span></sub> an. Wir multipliciren daher die <br/>Gleichungen (<span |
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961 class="cmmi-12"><img |
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962 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-c.png" alt="b" class="cmmi-12x-x-c" align="middle" /></span>) der Reihe nach mit <span |
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963 class="cmmi-12"><img |
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964 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-22.png" alt="e" class="12x-x-22" /></span><sub ><span |
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965 class="cmmi-8">m</span><sub ><span |
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966 class="cmr-6">1</span></sub></sub>, <span |
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967 class="cmsy-10x-x-120">-</span><span |
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968 class="cmmi-12"><img |
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969 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-22.png" alt="e" class="12x-x-22" /></span><sub ><span |
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970 class="cmmi-8">s</span><sub ><span |
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971 class="cmr-6">1</span></sub></sub>, <span |
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972 class="cmmi-12"><img |
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973 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-22.png" alt="e" class="12x-x-22" /></span><sub ><span |
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974 class="cmmi-8">m</span><sub ><span |
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975 class="cmr-6">2</span></sub></sub>, <span |
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976 class="cmsy-10x-x-120">-</span><span |
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977 class="cmmi-12"><img |
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978 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-22.png" alt="e" class="12x-x-22" /></span><sub ><span |
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979 class="cmmi-8">s</span><sub ><span |
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980 class="cmr-6">2</span></sub></sub> und <br/>erhalten mit Rücksicht auf (<span |
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981 class="cmmi-12"><img |
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982 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-b.png" alt="a" class="12x-x-b" /></span>) |
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983 </p> |
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984 |
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985 <center class="par-math-display" > |
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986 <img |
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987 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190250x.png" alt="@-f- @ z = 0 , " class="par-math-display" /></center> |
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988 <!--l. 1193--><p class="nopar"> |
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989 </p><!--l. 1197--><p class="noindent">wobei</p> |
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990 <center class="par-math-display" > |
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991 <img |
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992 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190251x.png" alt=" { } f = R T v e @-nm1-- v e @-ns1 + .- . m1 m1 @ z s1 s1 @ z { } @ p + vm1 e2m1 nm1 + vs1 e21ns1 + .+ . ---. @ z " class="par-math-display" /></center> |
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993 <!--l. 1211--><p class="nopar"> |
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994 </p><!--l. 1215--><p class="indent"> Durch Integration dieser Gleichung nach <span |
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995 class="cmmi-12">z </span>ergiebt sich <br/>unter Berücksichtigung des Umstandes, dass überall, wo keine <br/>Diffusion stattfindet, |
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996 </p> |
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997 <center class="par-math-display" > |
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998 <img |
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999 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190252x.png" alt="@-nm1-, @-ns1...@-p-- @ z @ z @ z " class="par-math-display" /></center> |
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1000 <!--l. 1223--><p class="nopar"> |
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1001 </p><!--l. 1227--><p class="noindent">verschwinden:</p> |
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1002 <center class="par-math-display" > |
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1003 <img |
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1004 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190253x.png" alt="f = 0 . " class="par-math-display" /></center> |
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1005 <!--l. 1233--><p class="nopar"> <pb/> |
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1006 </p><!--l. 1240--><p class="indent"> |
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1007 |
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1008 </p><!--l. 1241--><p class="indent"> Da die Zeit als constant zu betrachten ist, lässt sich <br/>schreiben:</p> |
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1009 <center class="par-math-display" > |
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1010 <img |
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1011 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190254x.png" alt=" R T {vm1 em1 d nm1 - vs1 .es1 .d ns1 + vm2 em2 d nm2- vs2 es2 dns2} d p = - ------------2-------------2-----------2--------------2---------- . vm1 em1 nm1 + vs1 es1 ns1 + vm2 em2 nm2 + vs2 .e s2 ns2 " class="par-math-display" /></center> |
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1012 <!--l. 1254--><p class="nopar"> |
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1013 </p><!--l. 1258--><p class="indent"> Der Ausdruck rechts ist im allgemeinen kein vollständiges <br/>Differential, was bedeutet, dass <img |
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1014 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmr12-1.png" alt="D" class="12x-x-1" /> <img |
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1015 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmr12-5.png" alt="TT" class="12x-x-5" /> nicht nur durch die an <br/>den diffusionslosen Bereichen herrschenden Concentrationen, <br/>sondern auch durch den Charakter des Diffusionsvorganges <br/>bestimmt wird. Es gelingt indessen durch einen Kunstgriff <br/>in der Anordnung, die Integration zu ermöglichen. |
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1016 </p><!--l. 1266--><p class="indent"> Wir denken uns den Raum <span |
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1017 class="cmmi-12">V </span>in drei Teile, Raum (1), <br/>Raum (2) und Raum (3) eingeteilt und dieselben vor Beginn <br/>des Experimentes durch zwei Scheidewände voneinander ge-<br/>trennt. (1) communicire mit <span |
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1018 class="cmmi-12">I</span>, (3) mit <span |
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1019 class="cmti-12">II</span>, in (2) seien beide <br/>Salze gleichzeitig gelöst, mit genau denselben Concentrationen <br/>wie in <span |
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1020 class="cmmi-12">I </span>bez. <span |
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1021 class="cmti-12">II</span>. Vor Beginn des Experimentes befindet sich <br/>also in <span |
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1022 class="cmmi-12">I </span>und (1) nur das erste, in <span |
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1023 class="cmti-12">II </span>und (3) nur das zweite <br/>Salz in Lösung, in (2) eine Mischung beider. Die Concentration |
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1024 <br/>ist dabei allenthalben constant. Bei Beginn des Experimentes <br/>werden die Scheidewände weggenommen und gleich darauf die <br/>Potentialdifferenz zwischen den Elektroden gemessen. Für <br/>diese Zeit ist aber die Integration über die diffundirenden <br/>Schichten möglich, da in der ersten diffundirenden Schicht |
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1025 <br/><span |
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1026 class="cmmi-12"><img |
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1027 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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1028 class="cmmi-8">m</span><sub ><span |
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1029 class="cmr-6">1</span></sub></sub> und <span |
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1030 class="cmmi-12"><img |
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1031 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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1032 class="cmmi-8">s</span><sub ><span |
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1033 class="cmr-6">1</span></sub></sub>, in der zweiten <span |
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1034 class="cmmi-12"><img |
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1035 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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1036 class="cmmi-8">m</span><sub ><span |
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1037 class="cmr-6">2</span></sub></sub> und <span |
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1038 class="cmmi-12"><img |
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1039 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-17.png" alt="n" class="12x-x-17" /></span><sub ><span |
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1040 class="cmmi-8">s</span><sub ><span |
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1041 class="cmr-6">2</span></sub></sub> constant sind. Die <br/>Integration liefert:</p> |
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1042 <center class="par-math-display" > |
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1043 <img |
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1044 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190255x.png" alt=" { vm - vs [ vm1 e2m nm1 + ns1 e2s ns1] p2 - p1 = R T ------1-----1--- lg 1 + -----21-----------21--- vm1 em1 + vs1 es1 vm2 em2 nm2 + ns2 es2 ns2 [ 2 2 ]} - ---vm2---vs2----lg 1 + vm2-em2-nm2-+-vs2 es2 ns2 . vm2 em2 + vs2 es2 vm1 e2m1 nm1 + vs1 e2s1 ns1 " class="par-math-display" /></center> |
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1045 <!--l. 1303--><p class="nopar"> |
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1046 </p><!--l. 1307--><p class="indent"> Eine Vereinfachung der Methode lässt sich erzielen, wenn <br/>es möglich ist, in <span |
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1047 class="cmmi-12">I</span> |
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1048 und <span |
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1049 class="cmti-12">II </span>gleiches Säureion von gleicher <br/>Concentration zu wählen. Verbindet man nämlich in diesem <br/>Falle Raum <span |
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1050 class="cmmi-12">I </span>mit Raum <span |
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1051 class="cmti-12">II </span>direct, so ist für den Anfang des |
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1052 <br/>Diffusionsvorganges zu setzen: |
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1053 </p> |
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1054 <center class="par-math-display" > |
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1055 <img |
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1056 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190256x.png" alt="@-(ns1 +-ns2) = 0 ; ns1 + ns2 = ns = const. @ z " class="par-math-display" /></center> |
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1057 <!--l. 1318--><p class="nopar"> <pb/> |
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1058 </p><!--l. 1325--><p class="indent"> |
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1059 |
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1060 </p><!--l. 1326--><p class="noindent">Ebenso ist nach Voraussetzung:</p> |
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1061 <center class="par-math-display" > |
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1062 <img |
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1063 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190257x.png" alt="es1 = es2 = es und vs1 = vs2 = vs . " class="par-math-display" /></center> |
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1064 <!--l. 1332--><p class="nopar"> |
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1065 </p><!--l. 1336--><p class="noindent">Gleichung (1) geht dann über in</p> |
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1066 <table width="100%" |
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1067 class="equation"><tr><td><a |
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1068 id="x1-17r4"></a> |
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1069 <center class="math-display" > |
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1070 <img |
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1071 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190258x.png" alt="nm1 em1 + nm2 em2 - ns es = 0. " class="math-display" /></center></td><td width="5%">(1<sup ><span |
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1072 class="cmsy-8">'</span></sup>)</td></tr></table> |
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1073 <!--l. 1343--><p class="nopar"> |
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1074 </p><!--l. 1347--><p class="indent"> Von den Gleichungen (2) bleibt die erste und dritte un-<br/>verändert bestehen, aus der zweiten und vierten ergiebt sich <br/>durch Addition: |
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1075 </p> |
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1076 <center class="par-math-display" > |
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1077 <img |
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1078 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190259x.png" alt=" @ { @ ns @ p } @ ns vs---- R T ------ esns E ---- = -----. @ z @ z @ z @ t " class="par-math-display" /></center> |
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1079 <!--l. 1357--><p class="nopar"> |
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1080 </p><!--l. 1361--><p class="indent"> Eliminirt man aus den so veränderten Gleichungen (2) <br/>vermittelst der Gleichung (1<span |
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1081 class="cmsy-10x-x-120">'</span>) die Ableitungen nach der Zeit, <br/>so erhält man wie vorhin einen Ausdruck für <span |
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1082 class="cmmi-12">d<img |
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1083 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/cmmi12-19.png" alt="p" class="12x-x-19" /></span>, welcher ein <br/>vollständiges Differential ist. Durch Integration desselben er-<br/>hält man: |
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1084 </p> |
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1085 <center class="par-math-display" > |
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1086 <img |
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1087 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190260x.png" alt=" 2 2 p2 - p1 = - R-T---vm2---vm1----lg em2-vm2-nm2-+-es vsns-, E vm2 e2- vm1 e1 e2m1 vm1 nm1 + e2s vsns " class="par-math-display" /></center> |
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1088 <!--l. 1375--><p class="nopar"> |
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1089 </p><!--l. 1379--><p class="noindent">wobei sich jetzt die Zahlenindices auf die Integrationsgrenzen <br/>beziehen. Infolge der Beziehung |
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1090 </p> |
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1091 |
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1092 <center class="par-math-display" > |
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1093 <img |
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1094 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190261x.png" alt="em nm = esns = em nm 1 1 2 2 " class="par-math-display" /></center> |
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1095 <!--l. 1386--><p class="nopar"> |
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1096 </p><!--l. 1390--><p class="noindent">erhalten wir noch einfacher |
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1097 </p> |
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1098 <center class="par-math-display" > |
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1099 <img |
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1100 src="http://foxridge.mpiwg-berlin.mpg.de/permanent/einstein/annalen/Einst_Ueber_de_1902/fulltext/img/Einst_Ueber_de_190262x.png" alt=" R T vm2 - vm1 em2 vm2 + esvs p2- p1 = - -------------------lg ---------------. E vm2 e2- vm1 e1 em1 vm1 + esvs " class="par-math-display" /></center> |
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1101 <!--l. 1399--><p class="nopar"> |
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1102 </p> |
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1103 <div class="center" > |
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1104 |
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1105 <!--l. 1403--><p class="noindent"> |
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1106 </p><!--l. 1404--><p class="noindent">----------</p></div> |
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1107 <!--l. 1408--><p class="indent"> Zum Schlusse empfinde ich noch das Bedürfnis, mich zu <br/>entschuldigen, dass ich hier nur einen dürftigen Plan für eine <br/>mühevolle Untersuchung entwerfe, ohne selbst zur experi-<br/>mentellen Lösung etwas beizutragen; ich bin jedoch dazu nicht |
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1108 <br/>in der Lage. Doch hat diese Arbeit ihr Ziel erreicht, wenn <br/>sie einen Forscher veranlasst, das Problem der Molecularkräfte <br/>von dieser Seite her in Angriff zu nehmen. |
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1109 </p><!--l. 1418--><p class="indent"> Bern, April 1902. </p> |
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1110 <div class="center" > |
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1111 |
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1112 <!--l. 1420--><p class="noindent"> |
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1113 </p><!--l. 1421--><p class="noindent">(Eingegangen 30. April 1902.)</p></div> |
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1114 <div class="center" > |
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1115 |
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1116 <!--l. 1424--><p class="noindent"> |
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1117 </p><!--l. 1425--><p class="noindent">----------</p></div> |
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1118 |
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1119 </body></html> |
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1120 |
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1121 |
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1122 |