Relating the Linear and Angular Variables — Question 1

Section 10-4 · Physics pages 1432–1433

Question 1 Tangential and radial accelerations point in different directions A point on a fixed-axis disk is instantaneously at (0.40, 0) m. The disk has ω = +3 rad/s and α = +5 rad/s2 about +z. x y + at ar Viewed along the fixed axis; counterclockwise is positive. (a) Find its velocity and acceleration vectors. (b) Find acceleration magnitude and explain why rα alone is insufficient.
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Question 1 - Solution Tangential and radial accelerations point in different directions x y + at ar (a) Derivation and calculation For fixed-axis rotation, use the perpendicular tangential and radial contributions:⃗ v =⃗ω ×⃗r = 3ˆz × 0.40ˆx = 1.20ˆy m/s .⃗ at =⃗α ×⃗r = 2.00ˆy,⃗ ar =⃗ω × (⃗ω ×⃗r) = −3.60ˆx.⃗ a = (−3.60, 2.00) m/s2 . (b) Result and interpretation Since the two components are perpendicular, |⃗a| = √ (rω2)2 + (rα)2 = √ 3.602 + 2.002 = 4.118 m/s2 . The term rα accounts for speed change; the inward term accounts for direction change. Physical check The velocity is tangent to the circle while the radial acceleration points toward the axis.

Question 1

Tangential and radial accelerations point in different directions

A point on a fixed-axis disk is instantaneously at (0.40,0)m(0.40,0)\,\mathrm m. The disk has ω=+3rad/s\omega=+3\,\mathrm{rad/s} and α=+5rad/s2\alpha=+5\,\mathrm{rad/s^2} about +z+z.

Diagram shown in the original SVG worksheet.

  1. Find its velocity and acceleration vectors.

  2. Find acceleration magnitude and explain why rαr\alpha alone is insufficient.

Question 1 - Solution

Tangential and radial accelerations point in different directions

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For fixed-axis rotation, use the perpendicular tangential and radial contributions: v→=ω→×r→=3ẑ×0.40x̂=1.20ŷm/s.\vec v=\vec\omega\times\vec r=3\hat z\times0.40\hat x =\boxed{1.20\hat y\ \mathrm{m/s}}. a→t=α→×r→=2.00ŷ,a→r=ω→×(ω→×r→)=−3.60x̂.\vec a_t=\vec\alpha\times\vec r=2.00\hat y,\qquad \vec a_r=\vec\omega\times(\vec\omega\times\vec r)=-3.60\hat x. a→=(−3.60,2.00)m/s2.\boxed{\vec a=(-3.60,2.00)\ \mathrm{m/s^2}}.

(b) Result and interpretation

Since the two components are perpendicular, |a→|=(rω2)2+(rα)2=3.602+2.002=4.118m/s2.\boxed{|\vec a|=\sqrt{(r\omega^2)^2+(r\alpha)^2} =\sqrt{3.60^2+2.00^2}=4.118\ \mathrm{m/s^2}}. The term rαr\alpha accounts for speed change; the inward term accounts for direction change.

Physical check

The velocity is tangent to the circle while the radial acceleration points toward the axis.