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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principe. L’expèrience nous montre que l’ènergie d’un champ èlectromagnètique<br />
se dècompose en deux parties, l’ènergie èlectrostatique et l’ènergie<br />
èlectrodynamique. Maxwell a reconnu (que si l’on regarde) la premiére come<br />
reprèsentant l’ènergie potentielle U, la seconde comme reprèsentant l’ènergie<br />
cinètique T." 433<br />
Maxwell thus solves the problem, allowing in addition a Lagrangian derivation of<br />
the equations <strong>and</strong> so fulfills the possibility of a mechanical explanation of<br />
electromagnetism. The grounds of acceptance of Maxwell’s theory in Poincarè’s<br />
analysis are clearly the ones referring to energy. Maxwell’s (<strong>and</strong> not Poynting’s)<br />
approach is preferred in view of its links <strong>with</strong> the mechanical expression of both<br />
PCE <strong>and</strong> PLA. This judgment is explicit already in 1890 <strong>and</strong> was to be reasserted<br />
in 1902 434. Hertz’s experiments, instead, up to 1894 were considered doubtful<br />
<strong>and</strong> in 1902 were considered to lend only indirect support. The<br />
desubstantialisation of ether theory was to weaken the experimental difference<br />
between contiguous action <strong>and</strong> delayed action-at-a-distance theories, but was to<br />
strengthen the theoretical difference between the PCE’s of the latter theories <strong>and</strong><br />
a local PCE expressed by the contiguous action theory. Poincarè’s choice of<br />
Maxwell from 1890 to 1902 is not referred to Poynting’s development (second<br />
step of localisation) but to Maxwell’s substantialisation (first step). This is due to<br />
the relevance he attributed to the asserted possibility of a mechanical<br />
explanation 435. Poincarè’s approach is very different from Hertz’s axiomatic<br />
assumption of Maxwell’s equations <strong>and</strong> his rejection of both a mechanical<br />
explanation <strong>and</strong> of a Lagrangian derivation. But still PCE, <strong>and</strong> specifically<br />
<strong>Helmholtz's</strong> PCE, was the principal reason for Poincarè’s choice of Maxwell.<br />
In the important process of the emergence of theoretical physics<br />
discussions on the meaning <strong>and</strong> the role of <strong>Helmholtz's</strong> approach to energy<br />
conservation were basic. Acceptance or denial of the mechanical world view, of<br />
the sharp distinction between kinetic <strong>and</strong> potential energy <strong>and</strong> of the privileged<br />
status of the central forces depending only on the distance were among the key<br />
issues, while others, non strictly mechanical interpretations of the principle of<br />
conservation, started to become mere <strong>and</strong> more important. At the end of the<br />
century in every research programme (mechanical, electromagnetic, energetic,<br />
thermodynamic) a specific version of the principle was put forward, <strong>and</strong> new<br />
433 Poincarè La Science p. 223.<br />
434 Poincarè La Science pp.216-25.<br />
435 Poincarè La Science pp.216-25.