Rolling as Translation and Rotation Combined — Question 6

Section 11-1 · Physics pages 1562–1563

Question 6 A marked tire traces a cycloid rather than a circle A radius-R wheel rolls right without slip. A mark starts at the ground origin. After a clockwise angle ϕ, its coordinates are x = R(ϕ −sin ϕ) and y = R(1 −cos ϕ). The center speed is constant V . x/R y/R 2π One cycloid arch; axes use the same scale. (a) Find the mark velocity and evaluate it at ϕ = π. (b) Locate the mark after a full revolution and explain the cusp at ϕ = 0.
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Question 6 - Solution A marked tire traces a cycloid rather than a circle x/R y/R 2π (a) Derivation and calculation The clockwise angle grows at ˙ϕ = V/R. Differentiating the given cycloid, vx = R(1 −cos ϕ) ˙ϕ = V (1 −cos ϕ) , vy = R sin ϕ ˙ϕ = V sin ϕ . At ϕ = π,⃗v = 2V ˆx : the mark is at the top. (b) Result and interpretation After one complete turn, (x, y) = (2πR, 0) . Near contact, the Taylor expansions give x ≃Rϕ3/6, y ≃Rϕ2/2. Both velocity components vanish at ϕ = 0. Since x changes cubically while y rises quadratically on either side, the trajectory has a cusp with a vertical limiting tangent. Physical check One turn advances the center and successive contact points by the circumference 2πR.

Question 6

A marked tire traces a cycloid rather than a circle

A radius-RR wheel rolls right without slip. A mark starts at the ground origin. After a clockwise angle ϕ\phi, its coordinates are x=R(ϕ−sin⁡ϕ)x=R(\phi-\sin\phi) and y=R(1−cos⁡ϕ)y=R(1-\cos\phi). The center speed is constant VV.

Diagram shown in the original SVG worksheet.

  1. Find the mark velocity and evaluate it at ϕ=π\phi=\pi.

  2. Locate the mark after a full revolution and explain the cusp at ϕ=0\phi=0.

Question 6 - Solution

A marked tire traces a cycloid rather than a circle

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The clockwise angle grows at ϕ̇=V/R\dot\phi=V/R. Differentiating the given cycloid, vx=R(1−cos⁡ϕ)ϕ̇=V(1−cos⁡ϕ),v_x=R(1-\cos\phi)\dot\phi=\boxed{V(1-\cos\phi)}, vy=Rsin⁡ϕϕ̇=Vsin⁡ϕ.v_y=R\sin\phi\dot\phi=\boxed{V\sin\phi}. At ϕ=π\phi=\pi, v→=2Vx̂\boxed{\vec v=2V\hat x}: the mark is at the top.

(b) Result and interpretation

After one complete turn, (x,y)=(2πR,0).\boxed{(x,y)=(2\pi R,0)}. Near contact, the Taylor expansions give x≃Rϕ3/6,y≃Rϕ2/2.x\simeq R\phi^3/6,\qquad y\simeq R\phi^2/2. Both velocity components vanish at ϕ=0\phi=0. Since xx changes cubically while yy rises quadratically on either side, the trajectory has a cusp with a vertical limiting tangent.

Physical check

One turn advances the center and successive contact points by the circumference 2πR2\pi R.