Introduction to Classical Mechanics · Problem 6.37
The Lagrangian method — Morin
Physics — Mechanics · forces-of-constraint
Problem
Cartesian coordinates **
In Eq. (6.35), take two time derivatives of the x2+y2−R=0 equation to obtain
R2(xx¨+yy¨)+(xy˙−yx˙)2=0,
and then combine this with the other two equations to solve for F in terms of x, y, x˙, y˙. Convert the result to polar coordinates (with θ measured from the vertical) and show that it agrees with Eq. (6.32).