Uniform Circular Motion — Question 10

Section 4-6 · Physics pages 570–571

Question 10 Leaving the circle preserves the instantaneous tangent velocity A point travels counterclockwise at speed 10 m/s on a circle of radius 5 m centered at the origin. At position angle 30◦it leaves the constraint. For the following 0.20 s, its acceleration is stipulated to be zero. after release The straight post-release path is tangent at the release point. (a) Find the position and velocity at release. (b) Find its position 0.20 s later and its distance from the old center. (c) Explain why continuing along the circle or moving radially outward would contradict the stated post-release acceleration.
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Question 10 - Solution Leaving the circle preserves the instantaneous tangent velocity after release (a) Take the tangent in the counterclockwise sense.⃗ r0 = 5(cos 30◦, sin 30◦) = (5 √ 3/2, 5/2) m,⃗ v0 = (−5, 5 √ 3) m/s Release position is (5 √ 3/2, 5/2) m. The unit tangent is (−sin 30◦, cos 30◦), so velocity is (−5, 5 √ 3) m/s. It is perpendicular to the radius, not parallel to it. (b) Continue with the release velocity.⃗ r =⃗r0 + .20⃗v0 = (5 √ 3/2 −1, 5/2 + √ 3) m, |⃗r| = √ 25 + 4 = √ 29 m With zero acceleration, displacement in 0.20 s is (−1, √ 3) m. New position is (5 √ 3/2 −1, 5/2 + √ 3) m. Since the displacement is perpendicular to the original radius, its distance from C is √ 52 + 22 = √ 29 ≈5.385 m. (c) Respect the velocity-change requirement.⃗ aafter =⃗0 ⇒⃗v =⃗v0; acircle = v2/R = 20 m/s2̸ = 0 Following the circle would still require inward acceleration v2/R = 20 m/s2. An immediate radial departure would require a discontinuous velocity turn. Zero post-release acceleration instead preserves the tangent velocity, producing a straight tangent path whose distance from the old center grows.

Question 10

Leaving the circle preserves the instantaneous tangent velocity

A point travels counterclockwise at speed 10 m/s on a circle of radius 5 m centered at the origin. At position angle 30∘30^\circ it leaves the constraint. For the following 0.20 s, its acceleration is stipulated to be zero.

Diagram shown in the original SVG worksheet.

  1. Find the position and velocity at release.

  2. Find its position 0.20 s later and its distance from the old center.

  3. Explain why continuing along the circle or moving radially outward would contradict the stated post-release acceleration.

Question 10 - Solution

Leaving the circle preserves the instantaneous tangent velocity

Diagram shown in the original SVG worksheet.

(a) Take the tangent in the counterclockwise sense.

r→0=5(cos⁡30∘,sin⁡30∘)=(53/2,5/2)m,v→0=(−5,53)m/s\vec r_0=5(\cos30^\circ,\sin30^\circ)=(5\sqrt3/2,5/2)\,\mathrm m,\quad\boxed{\vec v_0=(-5,5\sqrt3)\,\mathrm{m/s}} Release position is (53/2,5/2)(5\sqrt3/2,5/2) m. The unit tangent is (−sin⁡30∘,cos⁡30∘)(-\sin30^\circ,\cos30^\circ), so velocity is (−5,53)(-5,5\sqrt3) m/s. It is perpendicular to the radius, not parallel to it.

(b) Continue with the release velocity.

r→=r→0+.20v→0=(53/2−1,5/2+3)m,|r→|=25+4=29m\vec r=\vec r_0+.20\vec v_0=(5\sqrt3/2-1,5/2+\sqrt3)\,\mathrm m,\quad|\vec r|=\sqrt{25+4}=\sqrt{29}\,\mathrm m With zero acceleration, displacement in 0.20 s is (−1,3)(-1,\sqrt3) m. New position is (53/2−1,5/2+3)(5\sqrt3/2-1,5/2+\sqrt3) m. Since the displacement is perpendicular to the original radius, its distance from C is 52+22=29≈5.385\sqrt{5^2+2^2}=\sqrt{29}\approx5.385 m.

(c) Respect the velocity-change requirement.

a→after=0→⇒v→=v→0;acircle=v2/R=20m/s2≠0\vec a_{\mathrm{after}}=\vec0\ \Rightarrow\ \vec v=\vec v_0;\qquad a_{\mathrm{circle}}=v^2/R=20\,\mathrm{m/s^2}\ne0 Following the circle would still require inward acceleration v2/R=20v^2/R=20 m/s2^2. An immediate radial departure would require a discontinuous velocity turn. Zero post-release acceleration instead preserves the tangent velocity, producing a straight tangent path whose distance from the old center grows.