Stopping Of Block Due To Friction

Stopping Of Block Due To Friction

Vishal kumarUpdated on 02 Jul 2025, 05:44 PM IST

Friction is the opposing force to the motion of one body over the surface of another body. As in the case of a ball rolling freely on the ground, the ball ultimately comes to rest, due to the frictional force that exists between the ball and the ground. Friction is a force that is around us all of the time, and it opposes relative motion between systems in contact and also allows us to move. It is parallel to the surface and opposite to the direction of the intended motion.

This Story also Contains

  1. On the Horizontal Road
  2. On the Inclined Road
  3. Solved Examples Based on Stopping of Block Due to Friction
  4. Summary
Stopping Of Block Due To Friction
Stopping Of Block Due To Friction

In this article, we will cover the concept of stopping Block Due To Friction. This concept falls under the broader category of law of motion which is a crucial chapter in Class 11 physics. It is not only essential for board exams but also for competitive exams like the Joint Entrance Examination (JEE Main), National Eligibility Entrance Test (NEET), and other entrance exams such as SRMJEE, BITSAT, WBJEE, BCECE and more. Over the last ten years of the JEE Main exam (from 2013 to 2023), a total of three questions have been asked on this concept and no direct question was asked in NEET.

On the Horizontal Road

A block of mass m is moving initially with velocity u on a rough surface and due to friction, it comes to rest after covering a distance S.

  • Distance travelled before coming to rest (S):

F=ma=μRma=μmga=μgV2=u2−2asS=u22μg=P22μm2g

Where:

a= acceleration μ= coefficient of friction S= distance travelled g= gravity u= initial velocity V= finally velocity P= initial mometum=mu

  • Time taken to come to rest:
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From equation, v=u−at⇒0=u−μgt[ As v=0,a=μg]
∴t=uμg

  • The force of friction acting on the body:

F=maF=m(v−u)tF=mut[ As v=0]F=μmg[ As t=uμg]

On the Inclined Road

a=g[sin⁡θ+μcos⁡θ]V2=u2−2aS0=u2−2g[sin⁡θ+μcos⁡θ]SS=u22g(sin⁡θ+μcos⁡θ)

Where:

S= distance travelled μ= coefficient of friction V= Final velocity u= Initial velocity

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Solved Examples Based on Stopping of Block Due to Friction

Example 1: A 2 kg mass starts from rest on an inclined smooth surface with an inclination 30∘ and a length 2 m. How much will it travel (in meters) before coming to rest on a surface with a coefficient of friction of 0.25?

1) 4

2)6

3)8

4)2

Solution:

v2=u2+2as=0+2×gsin⁡30×2

Let it travel a distance ' S ' before coming to rest on a horizontal surface
S=v22μg=202×0.25×10=4 m

Hence, the answer is option (1).

Example 2: A body is moving with a speed of 12m/s and the coefficient of friction between the ground and the body is 0.4. The distance travelled by the body (in meters) before coming to rest is.

1) 18

2)10

3)15

4)20

Solution:

f=μmg
due to retardation
μmg=ma⇒a=μg=0.4∗10=4 m/s2
now for V=0
V2=u2−2as⇒0=u2−2asS=u22×a⇒12∗122∗4=18 m

Hence, the answer is option (1).

Example 3: A block of mass 10 kg starts sliding on a surface with an initial velocity of 9.8 ms−1. The coefficient of friction between the surface and block is 0.5. The distance covered by the block before coming to rest is:
[ use g=9.8 ms−2]

1) 4.9 m
2) 9.8 m
3) 12.5 m
4) 19.6 m

Solution:

f=μN=μmga=μg=4.9 m/s2V2=u2+2as0=(9.8)2+2(−4.9)ss=9.8 m
The distance covered by the block before coming to rest is $\mathrm{ 9.8\, m}$

Hence, the correct option is (2)

Example 4: A bag is gently dropped on a conveyor belt moving at a speed of 2 m/s. The coefficient of friction between the conveyor belt and bag Initially, the bag slips on the belt before it stops due to friction. The distance travelled by the bag on the belt during the slipping motion, is : [Take g=10 m/s−2 ]

1) 2 m
2) 0.5 m
3) 3.2 m
4) 0.8 ms

Solution:

f=μmga=fm=μg

The bag comes to rest when the speed of the bag is the same as the conveyor belt ie., 4 m/s
v2=u2+2 as (4)2=0+2(0.4×10)sS=2 m

The distance travelled by the bag on the belt during slipping motion is 2 m

Hence 1 is the correct option.

Example 5: A block of mass M slides down on a rough inclined plane with constant velocity. The angle made by the inclined plane with horizontal is θ. The magnitude of the contact force will be:

1) Mg
2) Mgcos⁡θ
3) Mgsin⁡θ+Mgcos⁡θ
4) Mgsin⁡θ1+μ

Solution:

For block moving at constant velocity

∑Fx=0−mgsin⁡Θ+μMgcos⁡Θ=0tan⁡Θ=μf=Mgsin⁡Θ=μMgcos⁡Θ→(1) Contact force =f2+N2(Mgsin⁡Θ)2+(Mgcos⁡Θ)2 Contact force =Mg

Hence, the answer is option (1).

Summary

When a moving block encounters friction, the force of friction opposes its motion, gradually reducing its speed until it comes to a complete stop. The stopping distance depends on the initial speed of the block and the coefficient of friction between the block and the surface. Understanding this interaction is crucial for applications requiring precise control of motion and stopping.

Frequently Asked Questions (FAQs)

Q: Why does a block sliding down an incline eventually reach a point where it stops accelerating?
A:
A block sliding down an incline reaches a point where it stops accelerating when the component of gravity parallel to the incline exactly balances the friction force. At this point, the net force becomes zero, and the block continues at a constant velocity (its terminal velocity for that incline).
Q: What would happen to a block's motion if the friction force suddenly increased halfway through its slide?
A:
If the friction force suddenly increased halfway through the block's slide, its deceleration would increase. This would result in the block stopping more abruptly than expected. The second half of the slide would have a much shorter stopping distance compared to if the friction had remained constant.
Q: How does the stopping distance of a block relate to the impulse provided by friction?
A:
The impulse provided by friction (force integrated over time) is equal to the change in the block's momentum. The stopping distance is related to how long it takes for this impulse to reduce the block's momentum to zero. A larger friction force provides the necessary impulse over a shorter distance.
Q: How does the concept of power apply to a block stopping due to friction?
A:
Power is the rate at which work is done or energy is transferred. In the case of a block stopping due to friction, power represents the rate at which kinetic energy is being converted to thermal energy. The power decreases as the block slows because power is the product of force (constant) and velocity (decreasing).
Q: What's the relationship between a block's stopping distance and the work done by friction?
A:
The work done by friction is equal to the friction force multiplied by the stopping distance. This work is also equal to the initial kinetic energy of the block. Therefore, the stopping distance is directly related to the initial kinetic energy and inversely related to the friction force.
Q: Why does a block sliding on a surface that becomes progressively rougher stop more quickly than expected?
A:
A block on a progressively rougher surface stops more quickly because the friction force increases as it moves. The increasing coefficient of friction leads to a stronger friction force, causing greater deceleration and a shorter overall stopping distance than if the surface had a uniform roughness.
Q: How does the concept of friction relate to the idea of energy dissipation in a sliding block?
A:
Friction is a mechanism of energy dissipation. As the block slides, the friction force converts the block's kinetic energy into thermal energy (heat), dissipating the energy that was initially in the block's motion into the block and the surface.
Q: What's the difference between sliding friction and rolling friction in terms of stopping a block?
A:
Sliding friction is typically greater than rolling friction. If a block could roll instead of slide, it would generally travel farther before stopping. This is why wheels are used to reduce friction in many applications.
Q: How would the stopping distance change if a block were sliding on a surface in a vacuum?
A:
In a vacuum, the stopping distance would be slightly longer compared to in air. This is because there would be no air resistance to contribute to slowing the block. However, for most everyday scenarios, this difference would be negligible as friction with the surface is the dominant factor in stopping the block.
Q: How does the distribution of mass within a block affect its stopping distance?
A:
The distribution of mass within the block doesn't directly affect its stopping distance on a horizontal surface. What matters is the total mass and the nature of the contact with the surface. However, mass distribution could indirectly affect stopping if it changes how the block interacts with the surface or air.