Substituting in Sec. 2 (10), we have

d dPR dPR d dPR dPR

-- ----- - ----- = Q1, -- ----- - ---- = Q2, ... (8)

dt dPq`1 dPq1 dt dPq`2 dPq2

These are Routh's forms of the modified Lagrangian equations.

Equivalent forms were obtained independently by Helmholtz at a later

date.

Kelvin's equations.

Encyclopaedia Britannica, 11th Edition, "Dyer, Sir Edward" to "Echidna" Volume 8, Slice 9 · 第 34 / 84 题