In one dimension, the magnitude of the gravitational force of attraction between a particle of mass \(m_{1}\) and one of mass \(m_{2}\) is given by $$F_{x}(x)=G \frac{m_{1} m_{2}}{x^{2}}$$ where \(G\) is a constant and \(x\) is the distance between the particles. (a) What is the potential energy function \(U(x) ?\) Assume that \(U(x) \rightarrow 0\) as \(x \rightarrow \infty,(b)\) How much work is required to increase the separation of the particles from \(x=x_{1}\) to \(x=\) \(x_{1}+d ?\)

Short Answer

Expert verified
The potential energy function is \(U(x)=-\frac{Gm_1m_2}{x}\). And the work done to increase the separation of particles from \(x=x_1\) to \(x=x_1+d\) is \(W = U(x_1+d) - U(x_1) = \[-\frac{Gm_1m_2}{x_1+d} + \frac{Gm_1m_2}{x_1}\]\)

Step by step solution

01

Identifying the Potential Energy Function

From the physics of gravitation, we know that the potential energy in a gravity field is given by \(-\frac{Gm_1m_2}{r}\). Since, gravity is always attractive and the force of gravity does work on the particles to decrease the separation. Therefore, the potential energy is negative. Also, it is customary to choose the potential energy to be 0 at infinite separation. So, in this case the potential energy function will be \(U(x)=-\frac{Gm_1m_2}{x}\)
02

Calculating Work Done

To determine the work done, we need to calculate the potential energy difference between two positions. Work is defined as the change in kinetic energy and also we know from the conservation laws of physics that total energy (kinetic + potential) in a closed system is conserved. Hence, work done to move the particles from \(x = x_1\) to \(x = x_1+d\) is: \(W = U(x_1+d) - U(x_1) = \[-\frac{Gm_1m_2}{x_1+d} + \frac{Gm_1m_2}{x_1}\]\)

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A projectile with a mass of \(2.40 \mathrm{~kg}\) is fired from a cliff \(125 \mathrm{~m}\) high with an initial velocity of \(150 \mathrm{~m} / \mathrm{s}\), directed \(41.0^{\circ}\) above the horizontal. What are \((a)\) the kinetic energy of the projectile just after firing and \((b)\) its potential energy? \((c)\) Find the speed of the projectile just before it strikes the ground. Which answers depend on the mass of the projectile? Ignore air drag.

An object falls from rest from a height \(h\). Determine the kinetic energy and the potential energy of the object as a function \((a)\) of time and \((b)\) of height. Graph the expressions and show that their sum - the total mechanical energy - is constant in each case.

A car is fitted with an energy-conserving flywheel, which in operation is geared to the driveshaft so that it rotates at 237 rev/s when the car is traveling at \(86.5 \mathrm{~km} / \mathrm{h}\). The total mass of the car is \(822 \mathrm{~kg}\), the flywheel weighs \(194 \mathrm{~N}\), and it is a uniform disk \(1.08 \mathrm{~m}\) in diameter. The car descends a \(1500-\mathrm{m}\) long, \(5.00^{\circ}\) slope, from rest, with the flywheel engaged and no power supplied from the motor. Neglecting friction and the rotational inertia of the wheels, find \((a)\) the speed of the car at the bottom of the slope, \((b)\) the angular acceleration of the flywheel at the bottom of the slope, and \((c)\) the power being absorbed by the rotation of the flywheel at the bottom of the slope.

The potential energy corresponding to a certain two-dimensional force is given by \(U(x, y)=\frac{1}{2} k\left(x^{2}+y^{2}\right) .(a)\) Derive \(F_{x}\) and \(F_{y}\) and describe the vector force at each point in terms of its coordinates \(x\) and \(y .(b)\) Derive \(F_{r}\) and \(F_{\theta}\) and describe the vector force at each point in terms of the polar coordinates \(r\) and \(\theta\) of the point. ( \(c\) ) Can you think of a physical model of such a force?

To disable ballistic missiles during the early boost phase of their flight, an "electromagnetic rail gun," to be carried in low-orbit Earth satellites, has been proposed. The gun might fire a \(2.38-\mathrm{kg}\) maneuverable projectile at \(10.0 \mathrm{~km} / \mathrm{s}\). The kinetic energy carried by the projectile is sufficient on impact to disable a missile even if it carries no explosive. (A weapon of this kind is a "kinetic energy" weapon.) The projectile is accelerated to muzzle speed by electromagnetic forces. Suppose instead that we wish to fire the projectile using a spring (a "spring" weapon). What must the force constant be in order to achieve the desired speed after compressing the spring \(1.47 \mathrm{~m} ?\)

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free