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\sqrt{x^2 + y^2} - R = 0 equation to obtain R2(xx¨+yy¨)+(xy˙−yx˙)2=0,R^2(x\ddot{x} + y\ddot{y}) + (x\dot{y} - y\dot{x})^2 = 0, and then combine this with the other two equations to solve for FF in terms of xx, yy, x˙\dot{x}, y˙\dot{y}. Convert the result to polar coordinates (with θ\theta measured from the vertical) and show that it agrees with Eq. (6.32).

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