Relating the Linear and Angular Variables — Question 10

Section 10-4 · Physics pages 1450–1451

Question 10 Release removes the inward acceleration constraint A small pellet is carried at the rim of a disk of radius 0.50 m, rotating counterclockwise at 4 rad/s in a horizontal plane. It is released at (0.50, 0) with no impulse. After release neglect all horizontal forces. x y + released path Viewed along the fixed axis; counterclockwise is positive. (a) Find its horizontal position 0.20 s later. (b) Compare with the position it would have occupied if still attached.
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Question 10 - Solution Release removes the inward acceleration constraint x y + released path (a) Derivation and calculation No impulse means velocity is continuous across release:⃗ v0 = 4ˆz × 0.50ˆx = 2ˆy m/s. With zero horizontal force after release,⃗ r(t) =⃗r0 +⃗v0t ⇒⃗r(0.20) = (0.50, 0.40) m . (b) Result and interpretation If attached, the point would remain on the circle: ∆θ = ωt = 4(0.20) = 0.80 rad.⃗ rattached = (0.50 cos 0.80, 0.50 sin 0.80) = (0.3484, 0.3587) m . The released path is the tangent line because the inward acceleration constraint is removed. Physical check The released point has distance √ 0.502 + 0.402 > 0.50 m from the axis.

Question 10

Release removes the inward acceleration constraint

A small pellet is carried at the rim of a disk of radius 0.50m0.50\,\mathrm m, rotating counterclockwise at 4rad/s4\,\mathrm{rad/s} in a horizontal plane. It is released at (0.50,0)(0.50,0) with no impulse. After release neglect all horizontal forces.

Diagram shown in the original SVG worksheet.

  1. Find its horizontal position 0.20s0.20\,\mathrm s later.

  2. Compare with the position it would have occupied if still attached.

Question 10 - Solution

Release removes the inward acceleration constraint

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

No impulse means velocity is continuous across release: v→0=4ẑ×0.50x̂=2ŷm/s.\vec v_0=4\hat z\times0.50\hat x=2\hat y\ \mathrm{m/s}. With zero horizontal force after release, r→(t)=r→0+v→0t⇒r→(0.20)=(0.50,0.40)m.\vec r(t)=\vec r_0+\vec v_0t\Rightarrow \boxed{\vec r(0.20)=(0.50,0.40)\ \mathrm m}.

(b) Result and interpretation

If attached, the point would remain on the circle: Δθ=ωt=4(0.20)=0.80rad.\Delta\theta=\omega t=4(0.20)=0.80\ \mathrm{rad}. r→attached=(0.50cos⁡0.80,0.50sin⁡0.80)=(0.3484,0.3587)m.\boxed{\vec r_{\mathrm{attached}}=(0.50\cos0.80,0.50\sin0.80) =(0.3484,0.3587)\ \mathrm m}. The released path is the tangent line because the inward acceleration constraint is removed.

Physical check

The released point has distance 0.502+0.402>0.50\sqrt{0.50^2+0.40^2}>0.50 m from the axis.