Horace Lamb,
1911 Encyclopædia Britannica, Volume 17…
(1911)
“ The ellipsoids (41) and (43) are reciprocal polars with respect to a sphere having O as centre. If A = B = C, the momental ellipsoid becomes a sphere; all axes through O are then principal axes, and the moment of inertia is the same for each. The mass-system is then said to possess kinetic symmetry about O. If all the masses lie in a plane (z = 0) we have, in the notation of (25) , c2 = 0, and therefore A = Mb2, B = Ma2, C = M (a2 + b2) , so that the equation of the momental ellipsoid takes the form b2x2 + a2y2 + (a2 + b2) z2 = ε4. ”
