/*! 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 10 Two blocks of masses \(10 \mat... [FREE SOLUTION] | 91Ó°ÊÓ

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Two blocks of masses \(10 \mathrm{~kg}\) and \(4 \mathrm{~kg}\) are connected by a spring of negligible mass and placed on a frictionless horizontal surface. An impulsive force gives a velocity of \(14 \mathrm{~ms}^{-1}\) to the heavier block in the direction of the lighter block. The velocity of centre of mass of the system at that moment is (a) \(30 \mathrm{~ms}^{-1}\) (b) \(20 \mathrm{~ms}^{-1}\) (c) \(10 \mathrm{~ms}^{-1}\) (d) \(5 \mathrm{~ms}^{-1}\)

Short Answer

Expert verified
The velocity of the center of mass is \(10 \mathrm{~ms}^{-1}\).

Step by step solution

01

Identify the System Components

The system consists of two blocks, one with a mass of \(10 \mathrm{~kg}\) and another with a mass of \(4 \mathrm{~kg}\). They are connected by a spring on a frictionless surface.
02

Apply the Concept of Centre of Mass

The velocity of the center of mass, \(v_{\text{cm}}\), is derived from the total momentum of the system divided by the total mass. Here, the system's momentum is influenced only by the velocity of the \(10 \mathrm{~kg}\) block.
03

Calculate the Total Momentum

The initial momentum of the heavier block is \(10 \mathrm{~kg} \times 14 \mathrm{~ms}^{-1} = 140 \mathrm{~kg \cdot ms}^{-1}\). Since the lighter block is initially at rest, its momentum is \(0 \mathrm{~kg \cdot ms}^{-1}\). Thus, the total initial momentum is \(140 \mathrm{~kg \cdot ms}^{-1}\).
04

Determine the Total Mass of the System

Add the masses of the two blocks: \(10 \mathrm{~kg} + 4 \mathrm{~kg} = 14 \mathrm{~kg}\).
05

Calculate the Velocity of the Centre of Mass

Use the formula \(v_{\text{cm}} = \frac{\text{Total Momentum}}{\text{Total Mass}} = \frac{140 \mathrm{~kg \cdot ms}^{-1}}{14 \mathrm{~kg}} = 10 \mathrm{~ms}^{-1}\).

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Key Concepts

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

Impulse and Momentum
Understanding impulse and momentum is crucial when dealing with collisions and forces in physics. Impulse is the change in momentum that occurs when a force is applied over a period of time.
  • Impulse is calculated by the formula: \( J = F \cdot \, \Delta t \)
  • Momentum, on the other hand, is the product of the mass and velocity of an object: \( p = m \cdot v \)
In this exercise, an impulsive force is applied to a block. This changes the momentum of the block immediately, giving it a velocity of \(14 \, \text{ms}^{-1}\). The momentum of each part of the system affects the velocity of the center of mass. By conserving momentum, we can calculate how the velocity changes when an impulse is applied. The law of conservation of momentum states that the total momentum before any event must be equal to the total momentum after, assuming no external forces act on the system.
Frictionless Surface
A frictionless surface in physics means that no forces oppose the motion of the objects on it. This makes calculations simpler, as you don't need to account for the friction force that typically slows down moving objects.
  • Without friction, the only forces acting are those applied directly, such as the impulsive force in this exercise.
  • This results in all energy being conserved for linear motion, allowing us to focus on other forces and effects, like the spring dynamics in this system.
For the blocks, the lack of friction implies that any changes in velocity are due solely to the initial impulse, as no kinetic energy is lost to friction. The center of mass's movement purely reflects the applied impulse and spring forces, without the need to adjust for energy loss or direction changes due to surface interactions.
Spring Dynamics
Springs follow Hooke's Law, which describes how they exert forces or store energy when compressed or stretched from their rest position.
  • The force exerted by a spring is \( F = -k\Delta x \), where \( k \) is the spring constant and \( \Delta x \) is the displacement from equilibrium.
  • Potential energy stored in a spring is calculated by \( U = \frac{1}{2} k \Delta x^2 \).
In the given problem, the spring’s dynamics don't change the situation's outcome because the spring's mass is negligible. It only connects the blocks. However, if the spring compresses or stretches, it could temporarily store or release energy. This example ignores spring dynamics for simplification, focusing entirely on the direct result of the impulse.
Velocity Calculation
Velocity is a vector quantity measuring the rate of change of position and it's crucial to understanding the system's movement.
  • The center of mass velocity \( v_{\text{cm}} \) represents the system’s overall motion.
  • To calculate \( v_{\text{cm}} \), use the formula: \( v_{\text{cm}} = \frac{\text{Total Momentum}}{\text{Total Mass}} \).
In this exercise, the velocity is found by dividing the total momentum (which is dictated by the motion of the heavy block) by the sum of the masses of both blocks. This results in a center of mass velocity of \( 10 \, \text{ms}^{-1} \). Understanding how to calculate velocity helps in determining how systems behave dynamically, especially when multiple objects interact.

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Most popular questions from this chapter

A spherical hollow is made in a lead sphere of radius \(R\) such that its surface touches the outside surface of lead sphere and passes through the centre. What is the shift in the centre of mass of lead sphere as a result of this hollowing? (a) \(\frac{R}{7}\) (b) \(\frac{R}{14}\) (c) \(\frac{R}{2}\) (d) \(R\)

\((n-1)\) equal point masses each of mass \(m\) are placed at the vertices of a regular \(n\)-polygon. The vacant vertex has a position vector a with respect to the centre of the polygon. Find the positive vector of centre of mass [NCERT Exemplat] (a) \(\frac{1}{n-1} a\) (b) \(-\frac{1}{(n-1)} a\) (c) \((n-1) a\) (d) \(-\left(\frac{n-1}{a}\right)\)

A thick uniform bar lies on a frictionless horizontal surface and is free to move in any way on the surface. Its, mass is \(0.16 \mathrm{~kg}\) and length is \(1.7 \mathrm{~m} .\) Two particles each of mass \(0.08 \mathrm{~kg}\) are moving on the same surface and towards the bar in the direction perpendicular to the bar, one with a velocity of \(10 \mathrm{~ms}^{-1}\) and other with velocity \(6 \mathrm{~ms}^{-1}\). If collision between particles and bar is completely inelastic, both particles strike with the bar simultaneously. The velocity of centre of masa after collision is (a) \(2 \mathrm{~ms}^{-1}\) (b) \(4 \mathrm{~ms}^{-1}\) (c) \(10 \mathrm{~ms}^{-1}\) (d) \(167 \mathrm{~ms}^{-1}\)

The masses of five balls at rest and lying at equal distances in a straight line are in geometrical progression with ratio 2 and their coefficients of restitution are each \(2 / 3\). If the first ball be started towards the second with velocity \(u\), then the velocity communicated to 5 th ball is (a) \(\frac{5}{9} \mathrm{u}\) (b) \(\left(\frac{5}{9}\right)^{2} u\) (c) \(\left(\frac{5}{9}\right)^{7} u\) (d) \(\left(\frac{5}{9}\right)^{4} u\)

Consider a two particle system with particles having masses \(m_{1}\) and \(m_{2} .\) If the first particle is pushed towards the centre of mass through a distance \(d\), by what distance should the second particle be moved, 80 as to keep the centre of mass at the same position? IAIEEE 2006] (a) \(\frac{m_{2}}{m_{1}} d\) (b) \(\frac{m_{1}}{m_{1}+m_{2}} d\) (c) \(\frac{m_{1}}{m_{2}} d\) (d) \(d\)

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