JEE Challenger
More from System of Particles and Rotational Motion

Ratio of Acceleration of Rolling Solid Sphere and Spherical Shell

A solid sphere (A)(A) of mass 5m5m and a spherical shell (B)(B) of mass mm, both having same radius, are placed on a rough surface. When a force of same magnitude is applied tangentially at the highest points of AA and BB, they start rolling without slipping with an acceleration of aAa_A and aBa_B, respectively. The ratio of aAa_A and aBa_B is ________.

Options

A

5:215 : 21

Correct
B

6:106 : 10

C

21:2521 : 25

D

1:51 : 5

Step-by-Step Solution

To find the ratio of the linear accelerations aAa_A and aBa_B of the solid sphere and the spherical shell respectively, we analyze the dynamics of rolling without slipping for a general body subjected to a tangential force applied at its highest point.

General Derivation for Rolling Acceleration

Consider a body of mass MM, radius RR, and moment of inertia about its center of mass Icm=kMR2I_{\text{cm}} = k M R^2, where kk is a dimensionless constant depending on the geometric shape of the body.

A horizontal force FF is applied tangentially at the top of the body. Let ff be the force of friction acting at the contact point with the rough surface.

  1. Translational Motion: Applying Newton's second law for the center of mass motion: F+f=MaF + f = M a

  2. Rotational Motion: Taking torque about the center of mass: τ=FRfR=Icmα\tau = F \cdot R - f \cdot R = I_{\text{cm}} \alpha Ff=IcmαRF - f = \frac{I_{\text{cm}} \alpha}{R}

  3. Condition for Pure Rolling: Since the body rolls without slipping: a=αR    α=aRa = \alpha R \implies \alpha = \frac{a}{R}

Substituting α\alpha into the rotational equation gives: Ff=IcmR2aF - f = \frac{I_{\text{cm}}}{R^2} a

Adding the translational and rotational equations eliminates the friction force ff: (F+f)+(Ff)=Ma+IcmR2a(F + f) + (F - f) = M a + \frac{I_{\text{cm}}}{R^2} a 2F=(M+IcmR2)a2F = \left(M + \frac{I_{\text{cm}}}{R^2}\right) a

Since Icm=kMR2I_{\text{cm}} = k M R^2, this simplifies to: 2F=M(1+k)a    a=2FM(1+k)2F = M(1 + k)a \implies a = \frac{2F}{M(1 + k)}


Acceleration of Solid Sphere (AA)

For a solid sphere of mass MA=5mM_A = 5m:

  • Moment of inertia IA=25MAR2    kA=25I_A = \frac{2}{5} M_A R^2 \implies k_A = \frac{2}{5}

Substituting the values into the acceleration formula: aA=2F5m(1+25)=2F5m(75)=2F7ma_A = \frac{2F}{5m \left(1 + \frac{2}{5}\right)} = \frac{2F}{5m \left(\frac{7}{5}\right)} = \frac{2F}{7m}


Acceleration of Spherical Shell (BB)

For a spherical shell of mass MB=mM_B = m:

  • Moment of inertia IB=23MBR2    kB=23I_B = \frac{2}{3} M_B R^2 \implies k_B = \frac{2}{3}

Substituting the values into the acceleration formula: aB=2Fm(1+23)=2Fm(53)=6F5ma_B = \frac{2F}{m \left(1 + \frac{2}{3}\right)} = \frac{2F}{m \left(\frac{5}{3}\right)} = \frac{6F}{5m}


Ratio of Accelerations

Taking the ratio of aAa_A to aBa_B: aAaB=2F7m6F5m=27×56=1042=521\frac{a_A}{a_B} = \frac{\frac{2F}{7m}}{\frac{6F}{5m}} = \frac{2}{7} \times \frac{5}{6} = \frac{10}{42} = \frac{5}{21}

Thus, the ratio aA:aBa_A : a_B is 5:215 : 21.

Ratio of Acceleration of Rolling Solid Sphere and Spherical Shell | Physics PYQ Solution - JEE Challenger