Unformatted text preview: Physics 601 Homework 10
Due Friday November 12 Goldstein
4.22, 4.24, 4.25 0 1. This problem concerns rotations about the z axis. ȹ cos(θ ) sin(θ ) 0ȹ ȹ ȹ
a. Show that the rotation about the z axis: R = ȹ − sin(θ ) cos(θ ) 0ȹ can be ȹ ȹ
0
1Ⱥ
ȹ 0
ȹ0 −1 0ȹ ȹ ȹ
written as R = exp( −θM z ) where M z = ȹ1 0 0ȹ . ȹ ȹ
€
ȹ
0 0 0Ⱥ
1
b. Show that cos(ϑ ) = 1 tr ( R) − 2 2
2. There is € general theorem by Euler that any rotation matrix can be represented as a
a rotation about one given axis. Thus by analogy to problem 3a. it can be written €
ȹ n x ȹ €
ȹ ȹ
ˆ
ˆ
as R = exp −Φn ⋅ M = exp −Φ n x M x + n y M y + n z M z where n = ȹ n y ȹ is the unit ȹ ȹ
ȹ n z Ⱥ
vector specify the axis of rotation and Φ is the angle specifying the rotation. The purpose of this problem is to find the explicit of the rotation matrix for such a €
ˆ
rotation. As a first step note that n is completely specified by a polar angle θ and €
azimuthal angle φ. Define Rnˆ ≡ Rz (φ ) Ry (θ ) . T
ˆ
a. As a first step show that n ⋅ M = Rnˆ M z Rnˆ . T
€
ˆ
b. Show that R = exp( −Φ n ⋅ M ) = Rnˆ exp( − ΦM z ) Rnˆ €
c. Express the nine matrix elements of R in terms of the polar and azimuthal angles defining n and the rotation angle Φ. €ˆ
Not that this description of the rotation matrices is alternative parameterization to €
the Euler angles. €
€
3. For the general rotation of the form given in 2: ˆ
a. Show that n is an eignevector of R with eigenvalue one. b. Show that cos(Φ) = 1 Tr ( R) − 1 . 2
2
4. Suppose we have a rotation specified by the Euler angles ( π , π , π ) (that is 333 πππ
R = Rz ( 3€Rx ( 3 ) Rz ( 3 ) ) . Find the angle of rotation about the single axis and the axis )
€
ˆ
n . €
€ ( €
€ ) (( )) ...
View
Full
Document
This note was uploaded on 12/29/2011 for the course PHYSICS 601 taught by Professor Hassam during the Fall '11 term at Maryland.
 Fall '11
 Hassam
 mechanics, Work

Click to edit the document details