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

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important in his view: "to what extent can heat correspond to a force<br />

equivalent"? 168<br />

Here force equivalents should not be confused <strong>with</strong> mechanical equivalents: the<br />

firsts are theoretically identifiable "energy terms"; the second are numerical<br />

conversion factors.<br />

The caloric theory was discussed in explicit reference to the interpretation of<br />

Carnot <strong>and</strong> Clapeyron 169, for whom the force equivalent is the work produced in<br />

the passage of a certain amount of caloric from a higher to a lower temperature.<br />

Helmholtz criticised 170 W.Henry's <strong>and</strong> Berthollet's interpretation of the heat<br />

produced by friction as displacement of caloric <strong>and</strong> asserted that results from the<br />

field of electricity showed that the total amount of the heat of a body can be<br />

actually increased. Helmholtz recalled experimental evidence, entirely based on<br />

research in electricity, against the caloric theory of heat <strong>and</strong> in favour of the<br />

mechanical one. While frictional <strong>and</strong> voltaic electricity did not give<br />

unquestionable evidence, because the heat produced could be interpreted as<br />

caloric displaced, "we still have to explain in a purely mechanical way the<br />

production of electrical tensions in two processes, in which any quantity of heat<br />

that can be assumed as transferred never appears" 171 : electrical (not<br />

electromagnetic) induction <strong>and</strong> movements of magnets. Helmholtz gave the<br />

example of an electrophorus used to charge a Leyden jar for the first, <strong>and</strong> for the<br />

second the example of electromagnetic machines where "heat can be developed<br />

ad infinitum" 172. It is only at this stage that Helmholtz recalled Joule's experiments<br />

of 1843 173 <strong>and</strong> asserted that Joule "endeavoured to show directly" that the<br />

electromagnetic current produced heat <strong>and</strong> not cold even in that part which is<br />

under the actual action of the magnet (no displacement of caloric is thus<br />

conceivable in the electrical circuit). Again the minor role that Joule's results<br />

play in the exposition of <strong>Helmholtz's</strong> ideas must be noted .<br />

For Helmholtz thus the caloric theory must be rejected, because heat can be<br />

produced indefinitely through mechanical <strong>and</strong> electrical forces, <strong>and</strong> the<br />

mechanical theory must take its place. As seen in the previous section, this result<br />

168 Helmholtz Erhaltung P. 27.<br />

169 Helmholtz Erhaltung P.28.<br />

170 Helmholtz Erhaltung P.28<br />

171 Helmholtz Erhaltung P. 29.<br />

172 Helmholtz Erhaltung P.30.<br />

173 Helmholtz Erhaltung P.30 ( Joule's rezsults were wrongly dated 1844)

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