Conservation and Innovation : Helmholtz's Struggle with Energy ...
Conservation and Innovation : Helmholtz's Struggle with Energy ...
Conservation and Innovation : Helmholtz's Struggle with Energy ...
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<strong>and</strong> unaware of Green's results190, introduced the concept of electric potential. He<br />
defined the quantity<br />
⎛ eieii − ⎝ r ⎠ ⎞<br />
corresponding to the sum of the tension forces consumed, <strong>and</strong> also of course to<br />
the living forces acquired in the motion of the two charges from an infinite<br />
distance to the distance r, as the potential of the two electrical elements for the<br />
distance r 191.<br />
The principle of conservation can thus be expressed in a new way: "the increase<br />
of vis viva in whichever movement must be considered equal to the difference of<br />
the potential at the end of the trajectory respect to the potential at the<br />
beginning" 192 (the sign of the potential is opposite to that of modern convention).<br />
The potential as defined by Helmholtz is equivalent but for the sign to what later<br />
was to be called potential energy. He showed a good grasp in setting the<br />
relations between potential <strong>and</strong> work, for instance in the case of the potential of<br />
one body <strong>with</strong> respect to another193. Here in fact he precisely stated the<br />
equivalence between potential <strong>and</strong> work. But problems occur in the definition of<br />
the potential of a body on itself (the sum of the potentials of an electric element<br />
of a body <strong>with</strong> respect to all the other electrical elements of the same body): in<br />
this case <strong>Helmholtz's</strong> definition is double the modern convention, but what mostly<br />
matters, does not correspond to the work done194 (the potential is supposed to be<br />
double the work done). This shows the "independence" of the two concepts in<br />
<strong>Helmholtz's</strong> approach. In the original 1847 edition of the Erhaltung there is a<br />
final correction (the only one) referring exactly to these problems. This is a clear<br />
indication of the incertitudes <strong>and</strong> difficulties faced by Helmholtz <strong>with</strong> concepts<br />
that in 1847 were by no means common195. Helmholtz in 1882 196 acknowledged<br />
190 According to Koenigsberger, Helmholtz knew of Green's theorem later, in<br />
Koenigsberg, partially through F.Neumann: Koenigsberger H v H P.100.<br />
Erhaltung<br />
191 Helmholtz Erhaltung P.38.<br />
192 Helmholtz Erhaltung P.39.<br />
193 Helmholtz Erhaltung Pp.39-40<br />
194 Helmholtz Erhaltung Pp.42-3. Clausius was the first to criticise this part of the<br />
195 In the 1882 reprint of the Erhaltung in WA 1 the correction is incorporated in the<br />
text (as in the English translations of Tyndall, Kahl <strong>and</strong> Lindsay), <strong>and</strong> Helmholtz warned the