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1. On the Dynamical Theory of Heat. Part VII

Published online by Cambridge University Press:  15 September 2014

W. Thomson
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Extract

This paper commences with a condensed re-statement of the fundamental principles and formulæ of the Dynamical Theory of Heat, from the first six parts of the author's treatment of the subject previously communicated to the Royal Society of Edinburgh, and his articles “On the Thermo-elastic Properties of Matter,” in the “Quarterly Mathematical Journal” (April 1855), and on “Thermo-magnetism,” and “Thermo-electricity,” in Nichol's Cyclopedia (Edinburgh 1860).

Type
Proceedings 1865-66
Information
Proceedings of the Royal Society of Edinburgh , Volume 5 , 1866 , pp. 510 - 512
Copyright
Copyright © Royal Society of Edinburgh 1866

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References

page no 510 note * The amount of the force divided by the elongation produced by it, when any force within practical limits of elasticity is applied to elongate a bar rod or wire, of the substance, one square centimetre in section.

page no 511 note * Which, when the French system (unit bulk of water being of mass unity) is followed, mean the same thing

page no 511 note † The “length of the modulus” is M ÷ ρ, if M be the modulus in grammes weight per square centimetre.—Thomson and Tait's Natural Philosophy, § 689.