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Conservation and Innovation : Helmholtz's Struggle with Energy ...

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histories cites these (Hirn's) articles <strong>and</strong> even recognizes the existence of Hirn's<br />

claim" 500.<br />

In my view, for a correct grouping of the "pioneers", the acceptance of a<br />

principle of conversion <strong>with</strong> constant coefficients or of a principle of<br />

conservation of "energy" must be kept separate from the specific model adopted<br />

for "energy", from the experimental determination of the work equivalent <strong>and</strong>,<br />

finally, from the mathematical representation of the quantity conserved.<br />

Helmholtz in fact thought possible to formulate the principle of conservation in<br />

the Erhaltung <strong>with</strong> either heat models (caloric <strong>and</strong> mechanical), <strong>and</strong> the choice<br />

in favour of the mechanical one was made on experimental grounds. I want also<br />

to underline that the Erhaltung was largely independent from the experimental<br />

determination of the work-heat equivalent: as I am going to show, Helmholtz did<br />

not give much importance to Joule's (wrongly-translated) values. Finally,<br />

mechanical theory is not the only route to the work-heat equivalence: Mayer<br />

denied the first <strong>and</strong> determined the second.<br />

The need for these distinctions is shown in Carnot's case. Kuhn asserts<br />

that Sadi Carnot's Réflexions "are incompatible <strong>with</strong> energy conservation" <strong>and</strong><br />

"Carnot's version of the conservation hypothesis is scattered through a notebook<br />

written between the publication of his memoir in 1824 <strong>and</strong> his death in 1832." 501.<br />

Thus he considers Carnot as a pioneer of energy conservation for his<br />

posthumously published acceptance of the mechanical model of heat <strong>and</strong> of the<br />

relative determination of the work-heat equivalent (370Kgm) 502. But this result,<br />

while obviously placing Carnot among the pioneers of the mechanical theory of<br />

heat <strong>and</strong> of the determination of the work-heat equivalence, was not needed in<br />

order to consider him among the followers of "energy conservation". Given that<br />

Carnot correctly based his theory on the impossibility of perpetual motion, even<br />

his published results do not contradict the principle of "energy" conservation.<br />

They contradict the mechanical model of heat: Carnot's assumed an interpretation<br />

of "energy" (heat by temperature variation, <strong>and</strong> this "energy" equals work) that<br />

later was ab<strong>and</strong>oned because the conceptual model of heat adopted (heat as a<br />

substance) was shown to be experimentally wrong. The soundness of Carnot's<br />

500 Kuhn Sim Disc P.68 n.2.<br />

501 Kuhn Sim Disc P.93 <strong>and</strong> 67 respectively.<br />

502 At the same time Kuhn asserts that, strictly speaking, Holtzmann, who also used<br />

the caloric theory, should not be included in the list. However Kuhn includes him because he<br />

made a determination similar to Mayer's one. Ibid p.67, n.2.

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