Are Angular Quantities Vectors? — Question 1

Section 10-2 · Physics pages 1392–1393

Question 1 Opposite viewing ends describe the same angular velocity A shaft lies along the laboratory z axis. An observer on the positive z side looking toward the origin sees counterclockwise rotation at 6 rad/s. x y + View from the positive z side toward the origin; the positive angular vector points out of the page. (a) Write the angular-velocity vector and describe what an observer on the negative z side sees. (b) If the speed decreases at 2 rad/s2, find the angular-acceleration vector.
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Question 1 - Solution Opposite viewing ends describe the same angular velocity x y + (a) Derivation and calculation Use a single laboratory axis for both observers. The right-hand rule gives⃗ ω = 6ˆz rad/s , |⃗ω| = 6 rad/s. The negative-z observer sees clockwise motion because the line of sight is reversed; the laboratory vector remains +6ˆz. (b) Result and interpretation For fixed direction ˆz,⃗ α = d⃗ω dt = d|ω| dt ˆz = −2ˆz rad/s2 . d|ω| dt =⃗ω ·⃗α |ω| = 6(−2) 6 = −2 rad/s2. Physical check The negative dot product identifies slowing independently of which end is viewed.

Question 1

Opposite viewing ends describe the same angular velocity

A shaft lies along the laboratory zz axis. An observer on the positive zz side looking toward the origin sees counterclockwise rotation at 6rad/s6\,\mathrm{rad/s}.

Diagram shown in the original SVG worksheet.

  1. Write the angular-velocity vector and describe what an observer on the negative zz side sees.

  2. If the speed decreases at 2rad/s22\,\mathrm{rad/s^2}, find the angular-acceleration vector.

Question 1 - Solution

Opposite viewing ends describe the same angular velocity

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Use a single laboratory axis for both observers. The right-hand rule gives ω→=6ẑrad/s,|ω→|=6rad/s.\boxed{\vec\omega=6\hat z\ \mathrm{rad/s}},\qquad |\vec\omega|=6\ \mathrm{rad/s}. The negative-zz observer sees clockwise motion because the line of sight is reversed; the laboratory vector remains +6ẑ+6\hat z.

(b) Result and interpretation

For fixed direction ẑ\hat z, α→=dω→dt=d|ω|dtẑ=−2ẑrad/s2.\vec\alpha=\frac{d\vec\omega}{dt}=\frac{d|\omega|}{dt}\hat z =\boxed{-2\hat z\ \mathrm{rad/s^2}}. d|ω|dt=ω→⋅α→|ω|=6(−2)6=−2rad/s2.\frac{d|\omega|}{dt}=\frac{\vec\omega\cdot\vec\alpha}{|\omega|} =\frac{6(-2)}6=-2\ \mathrm{rad/s^2}.

Physical check

The negative dot product identifies slowing independently of which end is viewed.