/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 4 A system consisting of two block... [FREE SOLUTION] | 91Ó°ÊÓ

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A system consisting of two blocks kept onc over the other rests over a smooth horizontal surface. Somchow it is sct in motion so that the system of blocks acquires a constant velocity. Friction cocfficicnts between the two blocks is \(\mu(\mu \neq O)\) Statement-1 : Aflerwards, friction between the blocks is static in nature and non zero. Statement-2 : 'The lower block is in translational equilibrium.

Short Answer

Expert verified
Both statements are correct; static friction maintains the blocks' constant velocity and translational equilibrium.

Step by step solution

01

Identify the System and Forces Involved

We have two blocks, one on top of the other, resting on a smooth horizontal surface. The lower block experiences no horizontal forces from the surface due to the smoothness. There is a frictional force between the two blocks when they are set into motion.
02

Understanding Frictional Forces

Since the blocks are moving together at a constant velocity, the friction between them must be static. Static friction acts to prevent surfaces from sliding over each other, and it is non-zero when exerting a force to maintain equilibrium.
03

Analyzing Statement 1

Statement 1 claims that the friction between the blocks is static and non-zero. Given that the blocks move at constant velocity without relative motion between them, static friction applies, thus supporting Statement 1.
04

Analyzing Statement 2

Statement 2 claims the lower block is in translational equilibrium. For an object at constant velocity on a frictionless surface with forces balanced (including static friction between blocks), it is indeed in translational equilibrium.
05

Conclusion

Both statements are correct; static friction is present and maintains equilibrium between the moving blocks, ensuring the lower block's translational equilibrium.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Static Friction
Static friction is a type of friction that occurs when two surfaces are in contact but not moving relative to each other. It's crucial for maintaining the position of objects and ensuring they stay stationary until enough force is applied to overcome it. Unlike kinetic friction, which acts when surfaces slide over each other, static friction prevents sliding. This friction arises from the microscopic contact points between surfaces.
In the context of our exercise, the static friction between the two blocks keeps them moving together at a constant velocity without slipping. If they were not moving at the same rate, kinetic friction would arise. However, since their velocities match perfectly, only static friction is at play. This type of friction is non-zero because it acts to maintain the system's equilibrium by countering any forces trying to disrupt it. Despite the common notion that static friction is highest just before sliding begins, it is actively working, even at lower values, as seen in the blocks remaining together as a unit without slipping.
Translational Equilibrium
Translational equilibrium refers to a state where all forces acting on an object are balanced, resulting in no net force and, consequently, no acceleration of the object. When an object is in translational equilibrium, it either remains at rest or continues to move at a constant velocity. This concept is deeply rooted in Newton's first law of motion, which states that an object will remain in its current state unless acted upon by a net external force.
In the case of our block system, the lower block is in translational equilibrium because there are no unbalanced horizontal forces acting on it. The smooth surface offers no resistance, and the static friction force between the blocks balances any external force. Therefore, the lower block maintains a constant velocity, illustrating its translational equilibrium. This scenario embodies the real-world application of the concept, demonstrating how forces can be perfectly balanced to achieve equilibrium.
Newton's Laws of Motion
Newton's laws of motion are foundational principles in physics that describe the relationship between the motion of an object and the forces acting on it. There are three laws that explain this relation:
  • First Law: Also known as the law of inertia, it states that an object will remain at rest or in uniform motion unless acted upon by a net external force.
  • Second Law: It introduces the concept of force, stating that the acceleration of an object is proportional to the net force acting upon it and inversely proportional to its mass. This is expressed by the formula \( F = ma \).
  • Third Law: This law states that for every action, there is an equal and opposite reaction.
In our exercise, these laws are at play in ensuring that the system of blocks moves with constant velocity. The first law explains the constant velocity in the absence of external horizontal forces due to the smooth surface, while the second law supports the observation of balanced forces resulting in no acceleration. The presence of static friction as an internal force preventing relative motion corresponds to the interplay of these laws, showing how they govern the dynamics of motion.

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Most popular questions from this chapter

Statement-1 : \(\Lambda\) body can be pulled with the least effort if it is pulled at an angle equal to the angle of friction from the surface. Statement-2 : If coefficient of static friction is \(\mu\), the angle of friction is tan \({ }^{1}(\mu)\).

Statement-1 : When a block moves on a rough horizontal surface with some specd, it cventually slows down. Statement-2 : Friction always opposes motion.

Statement-1 : Kinctic Triction force opposes the relative motion of the body. Statement-2 : Triction forec is gencrated duc to relative slipping betwcen bodics.

The block \(A\) has mass \(m_{1}\) and is attached to a spring having a stiflness \(k .\) The natural length of the spring is \(I_{0}\). Another block \(B\) of mass \(m_{2}\) is pressed against block \(A\) so the compression in the spring is \(d\). The arrangement is released from rest from this position. The coeflicient of friction between the blocks and the ground beneath is \(\mu\). The block \(B\) will gel separated from \(A\) il (a) \(d \leq \frac{2\left(m_{1}+m_{2}\right) \mu g}{k}\) (b) \(d \leq \frac{\left(m_{1}+m_{2}\right) \mu g}{k}\) (c) \(d>\frac{2\left(m_{1}+m_{2}\right) \mu g^{1 / 2}}{k}\) (d) \(d>\frac{\left(m_{1}+m_{2}\right) \mu g}{k}\)

A block of mass \(10 \mathrm{~kg}\) is placed in a car going down an incline of inclination \(60^{\circ}\). If the coefficient of friction between the block and car floor is \(\frac{1}{\sqrt{3}}\). Find the acceleration \(a\) of car down the incline so that the block doesn't slip on the car surface. (a) \(a \geq \frac{g}{\sqrt{3}}\) (b) \(\alpha \geq \frac{2 g}{\sqrt{3}}\) (c) \(a<\frac{g}{\sqrt{3}}\) or \(a>\frac{2 g}{\sqrt{3}}\) (d) \(\frac{g}{\sqrt{3}} \leq a \leq \frac{2 g}{\sqrt{3}}\)

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