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A uniform solid sphere of radius \(R\) produces a gravitational acceleration of \(a_{g}\) on its surface. At what distance from the sphere's center are there points (a) inside and (b) outside the sphere where the gravitational acceleration is \(a_{g} / 3\) ?

Short Answer

Expert verified
Inside: \(r = \frac{R}{3}\) and outside: \(r = \sqrt{3} R\).

Step by step solution

01

Understanding the Problem

We are given a uniform solid sphere that has a gravitational acceleration of \(a_{g}\) on its surface. We need to find two distances, one inside the sphere and one outside, where the gravitational acceleration is \(a_{g}/3\).
02

Gravitational field inside a sphere

For a point inside a sphere at a distance \(r\) from its center, the gravitational acceleration is given by \(g(r) = \frac{G M(r)}{r^2}\). The mass \(M(r)\) is the mass inside a radius \(r\) and is \(\frac{M}{R^3}r^3\), where \(M\) is the total mass of the sphere and \(R\) is its radius.
03

Determine the acceleration inside

Substitute the expression for \(M(r)\) into the formula for \(g(r)\) to get: \[g(r) = \frac{G}{r^2}\bigg(\frac{M}{R^3}r^3\bigg) = \frac{G M r}{R^3}\]. Set this equal to \(\frac{a_g}{3}\) to find the distance from the center where the acceleration is \(\frac{a_g}{3}\).
04

Solve for distance inside

We know that at the surface, \(G M / R^2 = a_{g}\). Hence, inside the sphere, the equation \(\frac{G M r}{R^3} = \frac{a_g}{3}\) simplifies to \( r = \frac{R}{3} \). This means the acceleration is \(\frac{a_g}{3}\) at \(r = \frac{R}{3}\) from the center.
05

Gravitational field outside a sphere

At a distance \(r\) outside the sphere, the acceleration is \(g(r) = \frac{G M}{r^2}\). Since the gravitational acceleration on the surface is \(a_g = \frac{G M}{R^2}\), set \(\frac{G M}{r^2} = \frac{a_g}{3}\) to find the external distance.
06

Solve for distance outside

From the equation \(\frac{G M}{r^2} = \frac{G M}{3 R^2}\), simplify to \(r^2 = 3 R^2\). Taking the square root, you find \(r = \sqrt{3} R\). This is the distance at which the gravitational acceleration is \(a_g / 3\) outside the sphere.

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Key Concepts

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

Uniform Solid Sphere
A uniform solid sphere is an object that has the same density throughout its volume. Each small part has the same amount of mass per unit volume. This uniformity means the mass is evenly spread across the sphere.

When discussing gravitational fields, we often assume spheres to be uniform to simplify calculations. This model helps in predicting how gravity behaves in various points inside and outside the sphere.

In the context of gravitational studies:
  • Each part of the sphere pulls gravitationally.
  • Gravity at any point is due to the combined effect of the entire mass.
The uniform solid sphere is vital for calculations in planetary physics and understanding Earth, which is approximately a uniform sphere itself.
Gravitational Acceleration
Gravitational acceleration is the rate at which an object accelerates due to the gravitational force exerted on it by a mass, like a planet or star. For Earth, we often refer to it as "g," approximately 9.81 m/s².

It measures how much velocity an object gains every second as it falls freely. For a sphere, gravitational acceleration depends on its mass and how far you are from its center.

Key aspects to remember include:
  • Gravitational acceleration on the surface of a sphere is constant when the sphere is uniform.
  • Inside the sphere, it varies depending on your distance from the center.
  • Outside the sphere, the decrease of gravitational acceleration follows the square of the distance from its center.
Distance from Center
The concept of distance from the center refers to how far a point is located from the center of a sphere, like a planet or moon. This distance affects how strongly you feel the gravitational pull.

Within the sphere, as you travel further inside from the center, gravitational acceleration begins at zero and increases as you move towards the surface. However, beyond the sphere, as the distance increases, the gravitational acceleration decreases.

For a uniform solid sphere:
  • Inside, gravitational acceleration is proportional to distance from the center.
  • Outside, gravitational acceleration decreases with the inverse square of the distance.
  • Understanding the impact of distance helps calculate gravitational effects at various points near or within massive bodies.
Inside and Outside a Sphere
When discussing gravitational acceleration, it's important to differentiate between being inside or outside a sphere.

Inside the sphere, gravitational force behaves differently compared to outside because all mass contributes to the force in a unique way:

For points inside:
  • Gravitational effects come only from the mass enclosed by your position.
  • Acceleration increases linearly with distance from the center.
For points outside:
  • All mass of the sphere contributes to gravitational force as if concentrated at the center.
  • Acceleration decreases with the square of the distance.
Understanding these differences helps solve problems involving gravitational fields and explain real-world phenomena, like how objects orbiting outside the Earth feel its gravity.

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Most popular questions from this chapter

The mean diameters of Mars and Earth are \(6.9 \times 10^{3} \mathrm{~km}\) and \(1.3 \times 10^{4} \mathrm{~km}\), respectively. The mass of Mars is \(0.11\) times Earth's mass. (a) What is the ratio of the mean density (mass per unit volume) of Mars to that of Earth? (b) What is the value of the gravitational acceleration on Mars? (c) What is the escape speed on Mars?

An asteroid, whose mass is \(2.0 \times 10^{-4}\) times the mass of Earth, revolves in a circular orbit around the Sun at a distance that is twice Earth's distance from the Sun. (a) Calculate the period of revolution of the asteroid in years. (b) What is the ratio of the kinetic energy of the asteroid to the kinetic energy of Earth?

The mean distance of Mars from the Sun is \(1.52\) times that of Earth from the Sun. From Kepler's law of periods, calculate the number of years required for Mars to make one revolution around the Sun; compare your answer with the value given in Appendix C.

The Sun's center is at one focus of Earth's orbit. How far from this focus is the other focus, (a) in meters and (b) in terms of the solar radius, \(6.96 \times 10^{8} \mathrm{~m}\) ? The eccentricity is \(0.0167\), and the semimajor axis is \(1.50 \times 10^{11} \mathrm{~m}\).

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?

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