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Question: A disc of radius $R$ rolls without slipping on a horizontal surface with velocity $v_0$ as shown in ...

A disc of radius RR rolls without slipping on a horizontal surface with velocity v0v_0 as shown in figure. Match the entries of List-I with those of List-II. [FIGURE]

List-I: (P) Acceleration of point is zero (Q) Acceleration of point is v02R\frac{v_0^2}{R} (R) Radius of curvature of the path of point is 22R2\sqrt{2}R at given instant (S) Radius of curvature of the path of point is 4R4R at given instant

List-II: (1) Point A (2) Point B (3) Point C (4) Point D (5) Point O

A

(P)-(5), (Q)-(1), (2), (3), (4), (R)-(2), (4), (S)-(3)

B

(P)-(5), (Q)-(1), (R)-(2), (S)-(3)

C

(P)-(1), (Q)-(5), (R)-(2), (S)-(3)

D

(P)-(5), (Q)-(1), (2), (3), (4), (R)-(2), (S)-(3)

Answer

(P)-(5), (Q)-(1), (2), (3), (4), (R)-(2), (4), (S)-(3)

Explanation

Solution

For a disc rolling without slipping, the velocity of the center vc=v0v_c = v_0 and angular velocity ω=v0/R\omega = v_0/R. Assuming constant v0v_0, angular acceleration α=0\alpha = 0.

Velocities:

  • Point O (center): vO=v0v_O = v_0 (horizontal)
  • Point A (bottom): vA=0v_A = 0
  • Point B (left): vB=v02+(v0)2=2v0v_B = \sqrt{v_0^2 + (-v_0)^2} = \sqrt{2}v_0
  • Point C (top): vC=v0+ωR=v0+v0=2v0v_C = v_0 + \omega R = v_0 + v_0 = 2v_0 (horizontal)
  • Point D (right): vD=v02+v02=2v0v_D = \sqrt{v_0^2 + v_0^2} = \sqrt{2}v_0

Accelerations: The acceleration of any point P on the rim relative to the center is centripetal: aP/O=ω2R=(v0/R)2R=v02/Ra_{P/O} = \omega^2 R = (v_0/R)^2 R = v_0^2/R. The acceleration of the center is zero.

  • Point O: aO=0a_O = 0 (constant velocity)
  • Point A: aA=aA/Oa_A = a_{A/O} (upwards) =v02/R= v_0^2/R
  • Point B: aB=aB/Oa_B = a_{B/O} (rightwards) =v02/R= v_0^2/R
  • Point C: aC=aC/Oa_C = a_{C/O} (downwards) =v02/R= v_0^2/R
  • Point D: aD=aD/Oa_D = a_{D/O} (leftwards) =v02/R= v_0^2/R

Radius of Curvature of Cycloid: The path of a point on the rim is a cycloid. The radius of curvature ρ\rho is given by ρ=4Rsin(θ/2)\rho = 4R \sin(\theta/2), where θ\theta is the angle of rotation from the lowest point.

  • Point A (lowest): θ=0    ρ=4Rsin(0)=0\theta = 0 \implies \rho = 4R \sin(0) = 0.
  • Point D (rightmost): θ=π/2    ρ=4Rsin(π/4)=4R(1/2)=22R\theta = \pi/2 \implies \rho = 4R \sin(\pi/4) = 4R(1/\sqrt{2}) = 2\sqrt{2}R.
  • Point C (topmost): θ=π    ρ=4Rsin(π/2)=4R\theta = \pi \implies \rho = 4R \sin(\pi/2) = 4R.
  • Point B (leftmost): θ=3π/2    ρ=4Rsin(3π/4)=4R(1/2)=22R\theta = 3\pi/2 \implies \rho = 4R \sin(3\pi/4) = 4R(1/\sqrt{2}) = 2\sqrt{2}R.

Matching: (P) Acceleration of point is zero: Point O (5). (Q) Acceleration of point is v02R\frac{v_0^2}{R}: Points A (1), B (2), C (3), D (4). (R) Radius of curvature is 22R2\sqrt{2}R: Points B (2), D (4). (S) Radius of curvature is 4R4R: Point C (3).