Classical Mechanics (Goldstein) · Problem 19

The Kinematics of Rigid Body Motion — Herbert Goldstein, Charles Poole, John Safko

Physics — Mechanics · finite-rotation-order-dependence

Problem

Figures 4.9 and 4.10 show that the order of finite rotations leads to different results. Use the notation that A(α,1n)\mathbf{A}(\alpha, \mathbf{1}_n) where A\mathbf{A} is a rotation in the direction of 1n\mathbf{1}_n through an angle α\alpha. Let n1n_1 and n2n_2 be two orthogonal directions. (a) If x\mathbf{x} is the position vector of a point on a rigid body, which is then rotated by an angle θ\theta around the origin, show that the new value of x\mathbf{x} is x′=(1n⋅x)1n+[x−1n(1n⋅x)]cos⁡θ−1n×xsin⁡θ.\mathbf{x}' = (\mathbf{1}_n \cdot \mathbf{x})\mathbf{1}_n + [\mathbf{x} - \mathbf{1}_n(\mathbf{1}_n \cdot \mathbf{x})]\cos\theta - \mathbf{1}_n \times \mathbf{x}\sin\theta. From this, obtain the formula for A(π/2,1n)\mathbf{A}(\pi/2, \mathbf{1}_n) and derive the two rotations in the figures. (b) Discuss these two rotations. [*Hint:* The answer will involve a rotation by the angle 23π\frac{2}{3}\pi in a direction (1/3)(1,1,1)(1/\sqrt{3})(1, 1, 1).]

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