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

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apply it to acoustics (1859), hydrodynamics (1859 <strong>and</strong> 1868) <strong>and</strong><br />

electrodynamics (1861, but mainly from 1869-1870 on) in works that became<br />

masterpieces in their fields.<br />

_______________________<br />

In the German-speaking world the mathematical potential (potential<br />

function) <strong>and</strong> the physical potential (potential) spread rapidly <strong>and</strong> were widely<br />

used. Clausius had a prominent role in this, through the different editions of his<br />

treatise on "Potential <strong>and</strong> Potential function", but already F.Neumann in 1845,<br />

Weber <strong>and</strong> Kirchhoff in 1848 <strong>and</strong> Riemann had made various use of these<br />

concepts. C.Neumann too followed this line of thought; in the sixties <strong>and</strong><br />

seventies delayed potentials <strong>and</strong> generalised potentials were also introduced.<br />

Given the now generally applied identification of potential <strong>with</strong> the work done, in<br />

this tradition all that was required to satisfy energy conservation was to show that<br />

the force in question (the problems were mainly connected <strong>with</strong> the attempt to<br />

formulate a general electrodynamic force) admitted a potential, that is that the<br />

work done by the force was a total differential. This in fact is equivalent to<br />

admitting the impossibility of perpetual motion.<br />

In Britain the situation was somewhat different. Despite the early <strong>and</strong><br />

important contributions to potential theory by Green, Hamilton, W.Thomson <strong>and</strong><br />

Stokes, priority was in general given to the "classic" concept of energy, implying<br />

the clear distinction between potential <strong>and</strong> kinetic parts. Of these two the kinetic<br />

was to be seen as basic : J.J.Thomson among others attempted to show this<br />

supposed priority, while Maxwell in 1873 had defined the idea of a delayed<br />

potential as "inconceivable".<br />

An energy battlefield for the electrodynamic debate (1870-75)<br />

In Electrodynamics Helmholtz opposed the views of Weber, who since<br />

1846 had given a force law depending not only on distances but also on velocities<br />

<strong>and</strong> accelerations, <strong>and</strong> of Clausius who in 1875-6 published a contribution along<br />

similar lines. Various physicists contributed to various aspects of the debate, but<br />

here we will only refer to the role of the energy principle. Not a minor one<br />

indeed, but rather the main battleground. Given the mathematical equivalence of<br />

the competing theories <strong>and</strong> the difficulties in experimenting <strong>with</strong> open currents,<br />

the acceptance of one law or the other began to be evaluated in relation to the

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