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Dr Faustus of Modern Physics - Department of Speech, Music and ...

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Chapter 22<br />

Loschmidt’s Reversibility<br />

Paradox<br />

Since a given system can never <strong>of</strong> its own accord go over into another<br />

equally probable state but into a more probable one, it is likewise<br />

impossible to construct a system <strong>of</strong> bodies that after traversing various<br />

states returns periodically to its original state, that is a perpetual<br />

motion machine. (Boltzmann)<br />

The Translators foreword to Lectures on Gas Theory by Boltzmann, confesses<br />

• There is apparently a contradiction between the law <strong>of</strong> increasing entropy<br />

<strong>and</strong> the principles <strong>of</strong> Newtonian mechanics, since the latter do<br />

not recognize any difference between past <strong>and</strong> future times. This is the<br />

so-called reversibility paradox (Umkehreinw<strong>and</strong>) which was advanced as<br />

an objection to Boltzmann’s theory by Loschmidt 1876-77.<br />

Loschmidts paradox formulated in 1876 by Johann Josef Loschmidt, compares<br />

the time-reversibility <strong>of</strong> Hamiltonian systems with the irreversibility <strong>of</strong><br />

the 2nd Law <strong>of</strong> thermodynamics:<br />

If microscopically matter consists <strong>of</strong> atoms <strong>and</strong> molecules ruled by reversible<br />

Hamiltonian mechanics, from where does the irreversibility <strong>of</strong> macroscopic<br />

physics? This was the problem Boltzmann set out to solve in his 1877<br />

article<br />

• On the Relation <strong>of</strong> a General Mechanical Theorem to the Second Law<br />

<strong>of</strong> Thermodynamics,<br />

101

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