Sticking Of A Block With Accelerated Cart

Sticking Of A Block With Accelerated Cart

Edited By Vishal kumar | Updated on Jul 02, 2025 07:42 PM IST

When driving on a level road, most drivers assume that their vehicles will maintain control and stability. However, skidding, a situation where a vehicle loses traction and slides uncontrollably, can occur even on flat surfaces. Skidding is often caused by factors such as sudden braking, sharp turns, or wet and slippery road conditions. In real life, skidding can lead to dangerous situations, especially if the driver panics or is unprepared. For example, a driver may suddenly brake to avoid a pedestrian, but if the road is wet, the vehicle might skid and lose control, potentially leading to an accident. Understanding the causes and prevention of skidding is crucial for safe driving.

This Story also Contains
  1. Skidding of Vehicle on a Level Road
  2. Solved Examples Based on Skidding of Vehicle on A Level Road
  3. Summary

Skidding of Vehicle on a Level Road

While solving with the help of the concept of pseudo-force.

When a cart moves with some acceleration toward the right then a pseudo force (ma) acts on the block toward the left.

This force (ma) is an action force by a block on the cart.


Now block will remain static w.r.t.cart. If friction force = μR ≥ mg

For equilibrium condition
$
\begin{aligned}
& \mu m a \geq m g \\
& a \geq \frac{g}{\mu} \\
& \mathrm{R}=\mathrm{ma} \\
& \therefore \quad a_{\min }=\frac{g}{\mu}
\end{aligned}
$
So, minimum force is applied on the cart so that the block will remain static w.r.t.cart.

$
F_{\min }=(M+m) \frac{g}{\mu}
$

where
$F_{\text {min }}=$ Minimum force
$a_{\text {min }}=$ minimum acceleration cart

M, m are masses of the cart and block respectively

Recommended Topic Video

Solved Examples Based on Skidding of Vehicle on A Level Road

Example 1: As shown here, in the figure, a cart C with mass M moves with acceleration 'b'. If the coefficient of friction between block A having mass m and the cart is μ, then, the acceleration of the cart and block system is independent of:

1) g

2) M

3) m

4) Both b) and c)

Solution:

If the cart is accelerated with 'b'

Pseudo force on the mass $F=m \times b=m \cdot b$
The force of friction $=\mu \mathrm{N}$
For horizontal equilibrium $\mathrm{F}=\mathrm{N}$
$f=\mu \mathrm{mb}$
The block will not fall as long as $\mathrm{f} \geq \mathrm{mg}$
$\mu \mathrm{mb} \geq \mathrm{mg}$
$\mathrm{b} \geq \mathrm{g} / \mu$

Hence, the answer is the option (4).

Example 2: As shown here, in the figure, cart C moving with acceleration 'b'. If the coefficient of friction between block A and the cart is $\mu$ then what is the maximum value of 'b' so that block A does not fall?

1) $\mu g$
2) $\mu^2 g$
3) $\frac{g}{\mu} $
4) None of these

Solution:

Sticking of a Block With Accelerated Cart

While solving with the help of the concept of pseudo-force.

When a cart moves with some acceleration toward the right then a pseudo force (ma) acts on the block toward the left.

This force (ma) is an action force by a block on the cart.

Now block will remain static w.r.t. block. If friction force= μR≥mg

For equilibrium condition

$\begin{aligned} & \mu m a \geq m g \\ & a \geq \frac{g}{\mu} \\ & \mathrm{R}=\mathrm{ma} \\ & \therefore \quad a_{\min }=\frac{g}{\mu} \\ & \quad F_{\min }=(M+m) \frac{g}{\mu}\end{aligned}$

Pseudo force (ma) acts on block towards the left
$
\begin{aligned}
& F_{\min }=\text { Minimum force } \\
& a_{\min }=\text { minimum acceleration cart }
\end{aligned}
$

$\mathrm{M}, \mathrm{m}$ are masses of the cart and block respectively
So, by using this concept -
Force acting on block $A$

$
W=f_L=m g=\mu(m b) \Rightarrow b=\frac{g}{\mu}
$

Hence, the answer is the option (3)

Summary

Skidding on a level road occurs when a vehicle loses traction, often due to sudden braking, sharp turns, or slippery conditions. The concept of pseudo-force helps explain this phenomenon, as it accounts for the forces acting on a block (or vehicle) when there is acceleration. By considering the minimum force and acceleration needed to prevent skidding, one can understand the relationship between friction, mass, and motion, helping to predict and prevent such incidents.

Frequently Asked Questions (FAQs)

1. What force prevents the block from sliding on an accelerating cart?
The force of static friction between the block and the cart's surface prevents the block from sliding. If this friction is strong enough, it will keep the block stationary relative to the cart.
2. How does the acceleration of the cart affect the likelihood of the block sliding?
As the cart's acceleration increases, the likelihood of the block sliding also increases. Higher acceleration requires a greater frictional force to keep the block in place.
3. What role does the coefficient of static friction play in this scenario?
The coefficient of static friction determines the maximum frictional force that can exist between the block and cart. A higher coefficient means more friction, making it less likely for the block to slide.
4. What is the relationship between the cart's acceleration and the frictional force needed to keep the block in place?
The frictional force needed to keep the block in place is directly proportional to the cart's acceleration. As the acceleration increases, the required frictional force increases linearly.
5. How does Newton's First Law of Motion apply to this scenario?
Newton's First Law states that an object at rest stays at rest unless acted upon by an external force. In this case, the block tends to remain at rest (relative to its surroundings) while the cart accelerates, causing the apparent backward motion.
6. What is the maximum acceleration a cart can have without causing a block to slide?
The maximum acceleration depends on the coefficient of static friction (μ) between the block and cart, and the acceleration due to gravity (g). It's given by a_max = μg, assuming a horizontal surface.
7. What happens when a block is placed on an accelerating cart?
When a block is placed on an accelerating cart, it experiences both the force of gravity and a horizontal force due to the cart's acceleration. The block will tend to move relative to the cart unless there's enough friction to keep it in place.
8. Why does a block tend to slide backwards on an accelerating cart?
A block tends to slide backwards on an accelerating cart due to inertia. The block resists changes in its motion, so as the cart accelerates forward, the block appears to move backward relative to the cart.
9. How does the mass of the block affect its tendency to slide?
The mass of the block doesn't directly affect its tendency to slide. This is because while a more massive block experiences a greater frictional force, it also requires a proportionally greater force to accelerate.
10. Can a block ever slide forward on an accelerating cart?
Yes, a block can slide forward on an accelerating cart, but only if the cart is decelerating (negative acceleration). In this case, the block's inertia would cause it to continue moving forward relative to the slowing cart.
11. How does the angle of the cart's surface affect the block's tendency to slide?
If the cart's surface is inclined, it increases the block's tendency to slide. The component of gravity parallel to the surface adds to the force trying to move the block, requiring more friction to keep it in place.
12. How would the scenario change if the block was replaced with a liquid in a container?
If the block was replaced with a liquid, the liquid's surface would tilt backwards relative to the container due to inertia. The angle of tilt would depend on the acceleration and the container's dimensions.
13. How would the scenario change if the block was connected to the cart with a spring?
If the block was connected to the cart with a spring, it would oscillate back and forth as the cart accelerates. The spring would provide a restoring force, causing the block to eventually settle at a new equilibrium position stretched back from its original position.
14. What would happen if the cart was accelerating on an inclined plane?
If the cart was accelerating on an inclined plane, the block would experience an additional component of gravity parallel to the cart's surface. This would make the block more likely to slide if the cart is accelerating uphill, and less likely if accelerating downhill.
15. How does the concept of mechanical advantage apply if the cart is part of a larger machine?
Mechanical advantage could apply if the cart's motion is part of a larger system. For example, if the cart is moved by a lever or pulley system, mechanical advantage could allow a smaller force to create the acceleration needed to move the cart and block.
16. What would happen if the block was replaced with a gyroscope?
A spinning gyroscope would resist changes to its axis of rotation due to angular momentum conservation. This could cause interesting behavior, such as precession, when the cart accelerates, depending on the orientation of the gyroscope's spin axis.
17. What is the difference between static and kinetic friction in this context?
Static friction acts to keep the block from moving relative to the cart when it's stationary. If the block starts sliding, kinetic friction (which is typically less than static friction) acts to slow its motion relative to the cart.
18. How would you calculate the frictional force acting on the block?
The frictional force (F) acting on the block is equal to the mass of the block (m) multiplied by the acceleration of the cart (a): F = ma. This force must be less than or equal to the maximum static friction force.
19. What happens if the frictional force is not strong enough to keep the block in place?
If the frictional force is not strong enough, the block will begin to slide relative to the cart. It will accelerate backwards (relative to the cart) until the kinetic friction force balances the force causing the relative motion.
20. How does the surface area of contact between the block and cart affect the friction?
Surprisingly, the surface area of contact does not affect the friction force. Friction depends on the normal force and the coefficient of friction, not on the area of contact (assuming ideal surfaces).
21. What is the normal force in this scenario, and why is it important?
The normal force is the force exerted by the cart's surface perpendicular to the contact area with the block. It's important because the maximum static friction force is proportional to this normal force.
22. How would adding weight to the top of the block affect its tendency to slide?
Adding weight to the top of the block increases the normal force between the block and cart, which in turn increases the maximum static friction force. This makes it less likely for the block to slide.
23. What would happen if the cart suddenly stopped accelerating?
If the cart suddenly stopped accelerating, the block would continue moving forward due to its inertia, potentially sliding if the deceleration is abrupt enough to overcome static friction.
24. How does the concept of relative motion apply to this scenario?
Relative motion is crucial here. While the block may appear to move backwards relative to the accelerating cart, both the cart and block are actually moving forward relative to the ground.
25. What is the difference between the real and apparent forces acting on the block?
The real forces are gravity and friction. The apparent force, often called a "fictitious force," is what seems to push the block backwards relative to the cart, but it's actually just the block's inertia resisting acceleration.
26. How would you experimentally determine the coefficient of static friction between the block and cart?
You could gradually increase the cart's acceleration until the block just starts to slip. At this point, the maximum static friction force equals ma, where m is the block's mass and a is the cart's acceleration. The coefficient of static friction μ is then a/g.
27. What would happen if the cart was accelerating vertically instead of horizontally?
If the cart was accelerating vertically upward, the block would experience an increased normal force, increasing the friction and making it less likely to slide. If accelerating downward, the normal force would decrease, potentially causing the block to lose contact with the cart.
28. How does air resistance affect the motion of the block relative to the cart?
Air resistance would have a minimal effect on the block's motion relative to the cart, as both are moving together through the air. However, it would affect the overall motion of the cart-block system relative to the ground.
29. What role does the block's moment of inertia play in this scenario?
The block's moment of inertia doesn't play a significant role in this scenario unless the block starts to rotate. If the friction is not uniform or the acceleration causes the block to tip, then the moment of inertia would affect the block's rotational motion.
30. What would happen if the cart's acceleration was not constant?
If the cart's acceleration varied, the force required to keep the block in place would also vary. Rapid changes in acceleration (jerk) could cause the block to slide even if it remained stationary under constant acceleration.
31. How does the concept of impulse relate to the sudden acceleration or deceleration of the cart?
Impulse, which is the change in momentum, is relevant when the cart suddenly accelerates or decelerates. A large impulse (rapid change in velocity) is more likely to cause the block to slide than a gradual change in velocity.
32. What would happen if there were multiple blocks stacked on top of each other on the cart?
With multiple stacked blocks, each block would exert a force on the ones below it. The bottom block would be most likely to slide first, as it experiences the sum of all the forces from the blocks above it.
33. How does the roughness of the surfaces affect the interaction between the block and cart?
Rougher surfaces generally have higher coefficients of friction, making it less likely for the block to slide. However, extremely rough surfaces might allow for mechanical interlocking, which can behave differently from pure frictional forces.
34. What would happen if the block and cart were in a friction-free environment?
In a friction-free environment, the block would immediately start sliding backwards relative to the cart as soon as the cart began to accelerate. It would continue to accelerate backwards until it fell off the back of the cart.
35. How does the elasticity of the materials affect the interaction between the block and cart?
The elasticity of the materials affects how they deform under stress. More elastic materials might "grip" each other better, potentially increasing friction. They could also absorb some of the energy from sudden accelerations, reducing the tendency for the block to slide.
36. What would happen if the cart was accelerating in a circular path instead of a straight line?
If the cart was accelerating in a circular path, the block would experience both tangential and centripetal acceleration. It would tend to slide towards the outside of the curve due to the centrifugal effect, in addition to the backward sliding tendency from the tangential acceleration.
37. How does the distribution of mass within the block affect its behavior on the accelerating cart?
The distribution of mass within the block doesn't affect its translational motion, but it can affect whether the block tips over. A block with a higher center of mass is more likely to tip when the cart accelerates.
38. What role does static equilibrium play in keeping the block stationary relative to the cart?
Static equilibrium occurs when the sum of all forces on the block is zero. This includes the friction force balancing the force due to the cart's acceleration. As long as static equilibrium is maintained, the block remains stationary relative to the cart.
39. What would happen if the cart's surface was frictionless but the block had a suction cup on its bottom?
With a suction cup, the block could remain stationary relative to the cart even on a frictionless surface. The suction force would need to overcome the force due to the cart's acceleration to prevent sliding.
40. How does the concept of work apply to the block-cart system during acceleration?
Work is done on the block-cart system by the force causing the cart's acceleration. If the block doesn't slide, no work is done in the block-cart reference frame. If the block slides, work is done against the kinetic friction force.
41. What would happen if the block was made of a magnetic material and the cart had a magnetic surface?
If both the block and cart were magnetic, there would be an additional attractive force between them. This would effectively increase the normal force and thus the maximum static friction force, making it less likely for the block to slide.
42. How does the principle of conservation of energy apply to this scenario?
Conservation of energy applies to the entire system. The work done to accelerate the cart increases the kinetic energy of the cart and block. If the block slides, some energy is converted to heat due to friction.
43. How does the humidity of the environment affect the interaction between the block and cart?
Humidity can affect friction between the block and cart. In some cases, a thin layer of moisture can increase friction through adhesion. In others, it might act as a lubricant and reduce friction. The effect depends on the materials and surface characteristics.
44. What would happen if the cart's acceleration was great enough to deform the block?
If the cart's acceleration was extreme enough to deform the block, the situation would become more complex. The deformation could change the contact area and pressure distribution, potentially affecting the friction. Elastic energy would also be stored in the deformed block.
45. How does the concept of impulse momentum theorem apply if the cart collides with another object?
If the cart collides with another object, the impulse momentum theorem would describe the change in momentum of the system. The block might continue moving forward due to its inertia, potentially sliding or tipping depending on the collision characteristics.
46. What would happen if the block was replaced with a pendulum hanging from the cart?
A pendulum hanging from the accelerating cart would swing backwards relative to the cart due to inertia. It would eventually settle at an angle where the tension in the string balances both gravity and the apparent force due to acceleration.
47. How does the concept of virtual work apply to analyzing the forces in this scenario?
Virtual work can be used to analyze the forces by considering hypothetical displacements. For example, you could use it to find the minimum coefficient of friction needed to prevent sliding by equating the virtual work done by friction to the work done by the apparent force due to acceleration.
48. What would happen if the cart was accelerating in a medium other than air, like water?
In a medium like water, both the cart and block would experience additional drag forces. This would require more force to achieve the same acceleration. The block might also experience buoyancy, which could affect the normal force and thus the friction.
49. How does the concept of stress and strain apply to the contact between the block and cart?
The contact between the block and cart involves stress (force per unit area) and strain (deformation). Even if not visibly deformed, there's microscopic deformation at the contact points. This deformation contributes to the frictional force through mechanisms like adhesion and mechanical interlocking.
50. What would happen if the block was very tall and narrow compared to its base?
A tall, narrow block would be more likely to tip over when the cart accelerates. There's a critical height-to-width ratio beyond which the block will tip before it slides. This occurs when the moment caused by the apparent horizontal force overcomes the stabilizing moment due to the block's weight.

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