As shown under MECHANICS, Sec. 22, we derive from (10)

d[Tau]

------ = Q1q`1 + Q2q`2 + ..., (15)

dt

and therefore in the case of a conservative system free from

extraneous force,

d

--([Tau] + V) = 0 or [Tau] + V = const., (16)

dt

which is the equation of energy. For examples of the application of

the formula (13) see MECHANICS, Sec. 22.

Encyclopaedia Britannica, 11th Edition, "Dyer, Sir Edward" to "Echidna" Volume 8, Slice 9 · 第 18 / 84 题