/*! 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 25 A solid uniform sphere has a mas... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

A solid uniform sphere has a mass of \(1.0 \times 10^{4} \mathrm{~kg}\) and a radius of \(1.0 \mathrm{~m}\). What is the magnitude of the gravitational force due to the sphere on a particle of mass \(m\) located at a distance of (a) \(1.5 \mathrm{~m}\) and (b) \(0.50 \mathrm{~m}\) from the center of the sphere? (c) Write a general expression for the magnitude of the gravitational force on the particle at a distance \(r \leq 1.0 \mathrm{~m}\) from the center of the sphere.

Short Answer

Expert verified
(a) Force is \(2.966 \times 10^{-7} m\text{ N}\). (b) Force is \(3.337 \times 10^{-7} m\text{ N}\). (c) \[ F = G m \times \frac{4}{3} \pi \times \rho r \].

Step by step solution

01

Understanding Gravitational Force

Gravitational force between two masses is given by the equation: \\[ F = \frac{G M m}{r^2} \]\where \(G\) is the gravitational constant \((6.674 \times 10^{-11} \text{Nm}^2/\text{kg}^2)\), \(M\) is the mass of the sphere, \(m\) is the mass of the particle, and \(r\) is the distance between the center of the sphere and the particle.
02

Calculating Force for r = 1.5 m

For part (a), since the particle is outside the sphere, use the equation: \\[ F = \frac{G M m}{1.5^2} \]\Substitute the given values: \\[ F = \frac{6.674 \times 10^{-11} \times 1.0 \times 10^4 \times m}{1.5^2} \]\\[ F = \frac{6.674 \times 10^{-7} m}{2.25} \] \Calculate the simplified force expression: \\[ F = 2.966 \times 10^{-7} m \text{ N} \]
03

Analyzing Gravitational Force Inside a Sphere

For part (b), because the particle is inside the sphere, we use a different approach. Inside a uniform sphere, the force is given by: \\[ F = \frac{G M_r m}{r^2} \]\where \(M_r = \frac{4}{3} \pi r^3 \rho\) and \(\rho = \frac{M}{V} = \frac{M}{\frac{4}{3} \pi R^3}\).
04

Substituting Parameters for r = 0.5 m

Compute \(\rho\), the density of the sphere: \\[ \rho = \frac{1.0 \times 10^4}{\frac{4}{3} \pi (1^3)} = \frac{1.0 \times 10^4}{\frac{4}{3} \pi} \]\Compute \(V_r\) (volume for \(r = 0.5\) m): \\[ M_r = \rho \times \frac{4}{3} \pi (0.5^3) \]\Substitute these in \(F\): \\[ F = \frac{G (\rho \frac{4}{3} \pi (0.5^3)) m}{0.5^2} \]}{
05

Calculating Internal Force

Substituting values for \(M_r\) and calculating: \\[ M_r = \rho \times \frac{4}{3} \pi (0.5^3) \approx 1250 \] \\[ F = \frac{6.674 \times 10^{-11} \times 1250 \times m}{0.25} \] \\[ F = 3.337 \times 10^{-7} m \text{ N} \]
06

General Expression for r ≤ 1.0 m

For distances \(r ≤ 1.0 \, \text{m}\), the force expression is: \\[ F = \frac{G m \cdot \frac{4}{3} \pi \rho r^3}{r^2} \] \Simplifying, use: \\[ F = G m \cdot \frac{4}{3} \pi \times \rho r \] \Where \( \rho \) is the sphere's density.

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 91Ó°ÊÓ!

Key Concepts

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

Uniform Sphere
A uniform sphere is a three-dimensional object where mass is evenly distributed throughout its volume. This uniformity simplifies the application of physics laws, like gravitational force calculations. When dealing with gravitational force exerted by a sphere on another object, the sphere’s mass distribution affects the calculations.

For gravitational force calculations outside the sphere, the sphere can be treated as if all its mass were concentrated at its center. However, the scenario changes if the particle is within the sphere’s radius. For points inside the sphere, the force depends only on the mass enclosed within a smaller concentric sphere whose radius is the distance from the center to the point being considered. This requires understanding both the sphere's overall density and its radius to determine the mass that contributes to the gravitational force.
Mass and Density
Mass and density are key concepts in understanding gravitational forces within spheres. The mass (M) is the measure of the amount of matter contained in the sphere. Density (\rho) is the mass per unit volume and is calculated using the formula:
  • \( \rho = \frac{M}{V} \)where \( V = \frac{4}{3} \pi R^3 \)
Here, \( R \) is the radius of the sphere. Density is crucial when calculating gravitational force for points inside the sphere. It allows us to determine the mass of a smaller sphere, with radius equal to the distance from the center, that influences gravitational force.

For the given uniform sphere, by knowing the total mass is \(1.0 \times 10^4 \text{ kg} \) and radius is \(1.0 \text{ m} \), we can calculate the overall density. This aids in understanding how much of the sphere's mass affects gravitational calculations for points within the sphere.
Inverse Square Law
The inverse square law is a fundamental principle used in calculating gravitational force. According to this law, the gravitational force between two objects is inversely proportional to the square of the distance (\( r \)) separating the objects. The equation representing this concept is:
  • \[ F = \frac{G M m}{r^2} \]
where \( G \) is the gravitational constant, \( M \) is the mass of the sphere, and \( m \) is the mass of the particle.

This principle explains why gravitational force decreases as the distance between objects increases. The gravitational pull becomes weaker the further away a particle is placed. When applied to a sphere, if the particle is outside, the force calculation takes into account the entire mass distributing from the center. Inside, only the mass within the smaller radius affects the force.
Gravitational Constant
The gravitational constant (\( G \)) is a critical factor in gravitational force calculations. Its value is \(6.674 \times 10^{-11} \text{ Nm}^2/\text{kg}^2\). This constant provides the necessary scale for forces and ensures the units match in any gravitational force equation.

It plays a pivotal role in both large-scale astronomical calculations and simple classroom physics problems. When substituting values into the gravitational force equation, \( G \) remains unchanged:
  • \[ F = \frac{G M m}{r^2} \]
This consistency helps in obtaining accurate results for forces exerted by large bodies like planets, or in this case, spherical objects. For practical problem solving, understanding \( G \) and its role ensures calculations remain precise and relevant to real-world scenarios.

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

Three identical stars of mass \(M\) form an equilateral triangle that rotates around the triangle's center as the stars move in a common circle about that center. The triangle has edge length \(L\). What is the speed of the stars?

In 1610, Galileo used his telescope to discover four prominent moons around Jupiter. Their mean orbital radii \(a\) and periods \(T\) are as follows: $$\begin{array}{lcc} {\text { Name }} & a\left(10^{8} \mathrm{~m}\right) & T \text { (days) } \\ \hline \text { Io } & 4.22 & 1.77 \\ \text { Europa } & 6.71 & 3.55 \\ \text { Ganymede } & 10.7 & 7.16 \\ \text { Callisto } & 18.8 & 16.7 \\ \hline \end{array}$$ (a) Plot \(\log a(y\) axis \()\) against \(\log T(x\) axis \()\) and show that you get a straight line. (b) Measure the slope of the line and compare it with the value that you expect from Kepler's third law. (c) Find the mass of Jupiter from the intercept of this line with the \(y\) axis.

In a shuttle craft of mass \(m=3000 \mathrm{~kg}\), Captain Janeway orbits a planet of mass \(M=9.50 \times 10^{25} \mathrm{~kg}\), in a circular orbit of radius \(r=4.20 \times 10^{7} \mathrm{~m}\). What are (a) the period of the orbit and (b) the speed of the shuttle craft? Janeway briefly fires a forwardpointing thruster, reducing her speed by \(2.00 \%\). Just then, what are (c) the speed, (d) the kinetic energy, (e) the gravitational potential energy, and (f) the mechanical energy of the shuttle craft? (g) What is the semimajor axis of the elliptical orbit now taken by the craft? (h) What is the difference between the period of the original circular orbit and that of the new elliptical orbit? (i) Which orbit has the smaller period?

(a) What is the escape speed on a spherical asteroid whose radius is \(500 \mathrm{~km}\) and whose gravitational acceleration at the surface is \(3.0 \mathrm{~m} / \mathrm{s}^{2} ?(\mathrm{~b})\) How far from the surface will a particle go if it leaves the asteroid's surface with a radial speed of \(1000 \mathrm{~m} / \mathrm{s} ?(\mathrm{c})\) With what speed will an object hit the asteroid if it is dropped from \(1000 \mathrm{~km}\) above the surface?

Assume a planet is a uniform sphere of radius \(R\) that (somehow) has a narrow radial tunnel through its center (Fig. 13-7). Also assume we can position an apple anywhere along the tunnel or outside the sphere. Let \(F_{R}\) be the magnitude of the gravitational force on the apple when it is located at the planet's surface. How far from the surface is there a point where the magnitude is \(\frac{1}{2} F_{R}\) if we move the apple (a) away from the planet and (b) into the tunnel?

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.