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Question: A sphere is placed rotating with its centre initially at rest in a corner as shown in figure (a) and...

A sphere is placed rotating with its centre initially at rest in a corner as shown in figure (a) and (b). Coefficient of friction between all surfaces and the sphere is 1/3. Find the ratio of the frictional force fafb\frac{f_a}{f_b} by ground in situations (a) and (b).

A

1

B

910\frac{9}{10}

C

109\frac{10}{9}

D

none

Answer

D

Explanation

Solution

The problem asks for the ratio of the frictional force by the ground in two situations (a) and (b). In both situations, a sphere is placed in a corner, rotating with its center initially at rest. The coefficient of friction μ=1/3\mu = 1/3 is the same for all surfaces.

Let MM be the mass of the sphere and RR be its radius. Since the center of the sphere is initially at rest, the net force on the sphere in both horizontal and vertical directions must be zero at that instant. Since the sphere is rotating, there is relative motion (slipping) at the contact points, so kinetic friction acts. The magnitude of kinetic friction is f=μNf = \mu N, where NN is the normal force.

Situation (a): Clockwise Rotation

  1. Forces and their directions:

    • Gravity (MgMg) acts downwards.
    • Normal force from the ground (NgN_g) acts upwards.
    • Normal force from the wall (NwN_w) acts horizontally to the right (pushing the sphere away from the wall).
    • The sphere rotates clockwise.
      • The point of contact with the ground moves to the right relative to the ground. So, the frictional force from the ground (fgf_g) acts to the left.
      • The point of contact with the wall moves downwards relative to the wall. So, the frictional force from the wall (fwf_w) acts upwards.
  2. Equations of motion (for the center of mass, initially at rest):

    • Vertical equilibrium: Ng+fwMg=0    Ng+fw=MgN_g + f_w - Mg = 0 \implies N_g + f_w = Mg
    • Horizontal equilibrium: Nwfg=0    Nw=fgN_w - f_g = 0 \implies N_w = f_g
  3. Frictional forces:

    • fg=μNgf_g = \mu N_g
    • fw=μNwf_w = \mu N_w
  4. Solving for faf_a (frictional force from the ground): Substitute the friction equations into the equilibrium equations: Ng+μNw=MgN_g + \mu N_w = Mg (1) Nw=μNgN_w = \mu N_g (2)

    Substitute (2) into (1): Ng+μ(μNg)=MgN_g + \mu (\mu N_g) = Mg Ng(1+μ2)=MgN_g (1 + \mu^2) = Mg Ng=Mg1+μ2N_g = \frac{Mg}{1 + \mu^2}

    The frictional force from the ground in situation (a) is fa=fg=μNgf_a = f_g = \mu N_g. fa=μMg1+μ2f_a = \frac{\mu Mg}{1 + \mu^2}

    Given μ=1/3\mu = 1/3: fa=(1/3)Mg1+(1/3)2=Mg/31+1/9=Mg/310/9=Mg3×910=3Mg10f_a = \frac{(1/3)Mg}{1 + (1/3)^2} = \frac{Mg/3}{1 + 1/9} = \frac{Mg/3}{10/9} = \frac{Mg}{3} \times \frac{9}{10} = \frac{3Mg}{10}

Situation (b): Counter-clockwise Rotation

  1. Forces and their directions:

    • Gravity (MgMg) acts downwards.
    • Normal force from the ground (NgN_g') acts upwards.
    • Normal force from the wall (NwN_w') acts horizontally to the right.
    • The sphere rotates counter-clockwise.
      • The point of contact with the ground moves to the left relative to the ground. So, the frictional force from the ground (fgf_g') acts to the right.
      • The point of contact with the wall moves upwards relative to the wall. So, the frictional force from the wall (fwf_w') acts downwards.
  2. Equations of motion (for the center of mass, initially at rest):

    • Vertical equilibrium: NgfwMg=0    Ngfw=MgN_g' - f_w' - Mg = 0 \implies N_g' - f_w' = Mg
    • Horizontal equilibrium: Nwfg=0    Nw=fgN_w' - f_g' = 0 \implies N_w' = f_g'
  3. Frictional forces:

    • fg=μNgf_g' = \mu N_g'
    • fw=μNwf_w' = \mu N_w'
  4. Solving for fbf_b (frictional force from the ground): Substitute the friction equations into the equilibrium equations: NgμNw=MgN_g' - \mu N_w' = Mg (3) Nw=μNgN_w' = \mu N_g' (4)

    Substitute (4) into (3): Ngμ(μNg)=MgN_g' - \mu (\mu N_g') = Mg Ng(1μ2)=MgN_g' (1 - \mu^2) = Mg Ng=Mg1μ2N_g' = \frac{Mg}{1 - \mu^2}

    The frictional force from the ground in situation (b) is fb=fg=μNgf_b = f_g' = \mu N_g'. fb=μMg1μ2f_b = \frac{\mu Mg}{1 - \mu^2}

    Given μ=1/3\mu = 1/3: fb=(1/3)Mg1(1/3)2=Mg/311/9=Mg/38/9=Mg3×98=3Mg8f_b = \frac{(1/3)Mg}{1 - (1/3)^2} = \frac{Mg/3}{1 - 1/9} = \frac{Mg/3}{8/9} = \frac{Mg}{3} \times \frac{9}{8} = \frac{3Mg}{8}

Ratio of Frictional Forces

Finally, find the ratio fafb\frac{f_a}{f_b}: fafb=3Mg103Mg8=3Mg10×83Mg=810=45\frac{f_a}{f_b} = \frac{\frac{3Mg}{10}}{\frac{3Mg}{8}} = \frac{3Mg}{10} \times \frac{8}{3Mg} = \frac{8}{10} = \frac{4}{5}

Comparing this with the given options: (A) 1 (B) 910\frac{9}{10} (C) 109\frac{10}{9} (D) none

The calculated ratio is 4/54/5, which is not among options (A), (B), or (C).

The final answer is D.