/*! 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 49 A body is acted upon by a force ... [FREE SOLUTION] | 91Ó°ÊÓ

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A body is acted upon by a force which is inversely proportional to the distance covered. The work done will be proportional to (a) \(s\) (b) \(s^{2}\) (c) \(s^{1 / 2}\) (d) None

Short Answer

Expert verified
(d) None.

Step by step solution

01

Understanding the Relationship

We know from the problem statement that the force \( F \) is inversely proportional to the distance \( s \). Mathematically, this can be expressed as: \[ F = \frac{k}{s} \]where \( k \) is a constant of proportionality.
02

Work Done Calculation

Work done \( W \) by a force is given by the integral of force over distance. Thus, \[ W = \int F \, ds = \int \frac{k}{s} \, ds \]
03

Integration of the Force Function

Perform the integration, \[ W = \int \frac{k}{s} \, ds = k \ln|s| + C \]where \( C \) is the integration constant. Note that work done expressed through this formula does not directly match with powers of \( s \) such as \( s \), \( s^2 \), or \( \sqrt{s} \).
04

Conclusion based on Integration Result

Since work done involves \( \ln(s) \), none of the options (\( s \), \( s^2 \), or \( s^{1/2} \)) accurately represent the proportional relationship with \( W \) from the integral. Thus, the correct answer is (d) None.

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Key Concepts

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

Integrals in Physics
In physics, integrals are used to calculate quantities that accumulate over a range, such as work done, area under curves, or even mass and charge distributions. Specifically, when dealing with the calculation of work done by a force, the integration approach enables us to consider varying force over a range of motion.
To compute work done by a varying force, we integrate the force function concerning the variable over which it acts, typically distance. For example, if a force varies with distance and is given as some function of distance, the work done can be expressed as \[ W = \int F(s) \, ds \]Here, the integration symbol \( \int \) indicates that we sum up the infinitesimal work done, \( F(s) \, ds \), over the entire path.
This approach is beneficial in real-world scenarios where force is not constant, and thus, direct multiplication is insufficient to determine work done.
Inverse Proportionality
Inverse proportionality describes a relationship where one quantity increases as the other decreases, such that their product remains constant. Mathematically, if a variable \( y \) is inversely proportional to another variable \( x \), it is expressed as \[ y = \frac{k}{x} \]where \( k \) is a constant.
This relationship is common in physics, such as in gravitational or electrostatic fields, where forces decrease as the distance between interacting bodies increases.
  • In the given problem, the force \( F \) varies inversely with distance \( s \), expressed as \( F = \frac{k}{s} \).
  • This suggests that as the body moves further away, the force acting on it reduces, holding the product \( F \times s \) constant.
This inverse relationship is crucial in deriving meaningful results when calculating work using integrals.
Force-Distance Relationship
The concept of how force relates to the distance over which it acts is foundational in understanding motion dynamics. Specifically, this relationship describes how the force applied to an object impacts the movement over distance.
In scenarios where force is constant, the work can be easily explained using the equation \[ W = F \times s \]where \( W \) is the work done, \( F \) is the constant force, and \( s \) is the distance.
  • However, when force varies with distance, as explored in the problem, integration is needed due to the changing value of \( F \).
  • In the given solution, \( F \) is inversely related to \( s \), a scenario illustrating that the force decreases as distance increases.
In practical terms, this affects how much work is done, necessitating a calculation approach that accommodates such variations, typically involving logarithmic or other complex dependencies not directly aligned with simple power relationships.

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Most popular questions from this chapter

Two particles of masses \(m_{1}\) and \(m_{2}\) are connected by an inextensible string which passes through a smooth vertical tube. The particle \(m_{1}\) is in equilibrium by the tension in the string which revolves the particle \(m_{2}\) in a horizontal circular path. Find the (a) angle \(\theta\) and (b) angular speed \(\omega\).

A particle moves in a straight line with retardation proportional to its displacement. kinetic energy during a displacement \(x\) is proportional to (a) \(x^{2}\) (b) \(e^{x}\) (c) \(x\) (d) \(\log _{e} x\)

\(\Delta\) car is moving with speed \(v\) and is taking a turn on a circular road of radius \(10 \mathrm{~m}\). The angle of banking is \(37^{\circ}\). The driver wants that car does not slip on the road. The coefficient of friction is \(0.4\left(g=10 \mathrm{~m} / \mathrm{scc}^{2}\right)\) 1\. The speed of car for which no frictional force is produced, is (a) \(5 \mathrm{~m} / \mathrm{sec}\) (b) \(5 \sqrt{3} \mathrm{~m} / \mathrm{sec}\) (c) \(3 \sqrt{5} \mathrm{~m} / \mathrm{sec}\) (d) \(10 \mathrm{~m} / \mathrm{sec}\) 2\. The friction force acting when \(v=10 \mathrm{~m} / \mathrm{scc}\) and mass of car is \(50 \mathrm{~kg}\) is (a) \(400 \mathrm{~N}\) (b) \(100 \mathrm{~N}\) (c) \(300 \mathrm{~N}\) (d) \(200 \mathrm{~N}\) 3\. If the car were moving on a llat road and distanec betwecn the front tyres is \(2 \mathrm{~m}\) and the height of the centre of the mass of the car is \(1 \mathrm{~m}\) from the ground, then the minimum velocity for which car topples is (a) \(5 \mathrm{~m} / \mathrm{sec}\) (b) \(5 \sqrt{3} \mathrm{~m} / \mathrm{scc}\) (c) \(3 \sqrt{5} \mathrm{~m} / \mathrm{scc}\) (d) \(10 \mathrm{~m} / \mathrm{scc}\)

A weightless rod of length \(2 l\) carries two equal masses \(m\), one tied at lower end \(A\) and the other at the middle of the rod at \(B\). The rod can rotate in vertical planc about a fixed horizontal axis passing through \(C\). The rod is released from rest in horizontal position. The speed of the mass \(B\) at the instant rod becomes vertical is (a) \(\sqrt{\frac{3 g l}{5}}\) (b) \(\sqrt{\frac{4 g l}{5}}\) (c) \(\sqrt{\frac{6 g l}{5}}\) (d) \(\sqrt{\frac{7 g l}{5}}\)

Statement-1: Work done by a force acting on a particle may be negative, even if kinetic energy of the body remains constant. Statement-2: Work done by conservative force equals negative of change in potential cnergy of Lhe body.

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