Are Angular Quantities Vectors? — Question 6

Section 10-2 · Physics pages 1402–1403

Question 6 A turning angular-velocity vector has acceleration at constant speed A rigid body has instantaneous angular velocity⃗ω(t) = 4[cos(2t)ˆx + sin(2t)ˆy] rad/s, with time in seconds. ωx ωy⃗ ω(0)⃗ α(0) Angular-velocity space; the acceleration arrow is tangent, with its own magnitude scale. (a) Find angular acceleration and its magnitude. (b) At t = 0, compare the directions of⃗ω and⃗α. Does constant angular speed imply zero angular acceleration?
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Question 6 - Solution A turning angular-velocity vector has acceleration at constant speed ωx ωy⃗ ω(0)⃗ α(0) (a) Derivation and calculation Differentiate the Cartesian components:⃗ α = 8[−sin(2t)ˆx + cos(2t)ˆy] rad/s2 . |⃗α| = 8 √ sin2(2t) + cos2(2t) = 8 rad/s2 . (b) Result and interpretation At the specified instant,⃗ ω(0) = 4ˆx,⃗ α(0) = 8ˆy . At every time,⃗ ω ·⃗α = 32[−cos(2t) sin(2t) + sin(2t) cos(2t)] = 0. Thus d|ω|/dt = 0 while d⃗ω/dt̸ = 0: the axis turns at constant angular speed magnitude. Physical check In angular-velocity space the derivative is tangent to the circle, perpendicular to its radius.

Question 6

A turning angular-velocity vector has acceleration at constant speed

A rigid body has instantaneous angular velocity ω→(t)=4[cos⁡(2t)x̂+sin⁡(2t)ŷ]rad/s\vec\omega(t)=4[\cos(2t)\hat x+\sin(2t)\hat y]\,\mathrm{rad/s}, with time in seconds.

Diagram shown in the original SVG worksheet.

  1. Find angular acceleration and its magnitude.

  2. At t=0t=0, compare the directions of ω→\vec\omega and α→\vec\alpha. Does constant angular speed imply zero angular acceleration?

Question 6 - Solution

A turning angular-velocity vector has acceleration at constant speed

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Differentiate the Cartesian components: α→=8[−sin⁡(2t)x̂+cos⁡(2t)ŷ]rad/s2.\boxed{\vec\alpha=8[-\sin(2t)\hat x+\cos(2t)\hat y]\ \mathrm{rad/s^2}}. |α→|=8sin⁡2(2t)+cos⁡2(2t)=8rad/s2.|\vec\alpha|=8\sqrt{\sin^2(2t)+\cos^2(2t)}=\boxed{8\ \mathrm{rad/s^2}}.

(b) Result and interpretation

At the specified instant, ω→(0)=4x̂,α→(0)=8ŷ.\boxed{\vec\omega(0)=4\hat x,\qquad\vec\alpha(0)=8\hat y}. At every time, ω→⋅α→=32[−cos⁡(2t)sin⁡(2t)+sin⁡(2t)cos⁡(2t)]=0.\vec\omega\cdot\vec\alpha=32[-\cos(2t)\sin(2t)+\sin(2t)\cos(2t)]=0. Thus d|ω|/dt=0d|\omega|/dt=0 while dω→/dt≠0d\vec\omega/dt\ne0: the axis turns at constant angular speed magnitude.

Physical check

In angular-velocity space the derivative is tangent to the circle, perpendicular to its radius.