Question
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 fbfa by ground in situations (a) and (b).

1
109
910
none
D
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 is the same for all surfaces.
Let M be the mass of the sphere and R 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=μN, where N is the normal force.
Situation (a): Clockwise Rotation
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Forces and their directions:
- Gravity (Mg) acts downwards.
- Normal force from the ground (Ng) acts upwards.
- Normal force from the wall (Nw) 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 (fg) acts to the left.
- The point of contact with the wall moves downwards relative to the wall. So, the frictional force from the wall (fw) acts upwards.
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Equations of motion (for the center of mass, initially at rest):
- Vertical equilibrium: Ng+fw−Mg=0⟹Ng+fw=Mg
- Horizontal equilibrium: Nw−fg=0⟹Nw=fg
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Frictional forces:
- fg=μNg
- fw=μNw
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Solving for fa (frictional force from the ground): Substitute the friction equations into the equilibrium equations: Ng+μNw=Mg (1) Nw=μNg (2)
Substitute (2) into (1): Ng+μ(μNg)=Mg Ng(1+μ2)=Mg Ng=1+μ2Mg
The frictional force from the ground in situation (a) is fa=fg=μNg. fa=1+μ2μMg
Given μ=1/3: fa=1+(1/3)2(1/3)Mg=1+1/9Mg/3=10/9Mg/3=3Mg×109=103Mg
Situation (b): Counter-clockwise Rotation
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Forces and their directions:
- Gravity (Mg) acts downwards.
- Normal force from the ground (Ng′) acts upwards.
- Normal force from the wall (Nw′) 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 (fg′) acts to the right.
- The point of contact with the wall moves upwards relative to the wall. So, the frictional force from the wall (fw′) acts downwards.
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Equations of motion (for the center of mass, initially at rest):
- Vertical equilibrium: Ng′−fw′−Mg=0⟹Ng′−fw′=Mg
- Horizontal equilibrium: Nw′−fg′=0⟹Nw′=fg′
-
Frictional forces:
- fg′=μNg′
- fw′=μNw′
-
Solving for fb (frictional force from the ground): Substitute the friction equations into the equilibrium equations: Ng′−μNw′=Mg (3) Nw′=μNg′ (4)
Substitute (4) into (3): Ng′−μ(μNg′)=Mg Ng′(1−μ2)=Mg Ng′=1−μ2Mg
The frictional force from the ground in situation (b) is fb=fg′=μNg′. fb=1−μ2μMg
Given μ=1/3: fb=1−(1/3)2(1/3)Mg=1−1/9Mg/3=8/9Mg/3=3Mg×89=83Mg
Ratio of Frictional Forces
Finally, find the ratio fbfa: fbfa=83Mg103Mg=103Mg×3Mg8=108=54
Comparing this with the given options: (A) 1 (B) 109 (C) 910 (D) none
The calculated ratio is 4/5, which is not among options (A), (B), or (C).
The final answer is D.