/*! 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 16 The distance between the centres... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

The distance between the centres of the Moon and the earth is \(D .\) The mass of the earth is 81 times the mass of the Moon. At what distance from the centre of the earth, the gravitational force will be zero? (1) \(\frac{D}{2}\) (2) \(\frac{2 D}{3}\) (3) \(\frac{4 D}{3}\) (4) \(\frac{9 D}{10}\)

Short Answer

Expert verified
The gravitational force is zero at \( \frac{9D}{10} \) from the Earth's center.

Step by step solution

01

Understanding the Gravitational Force Balance

We need to find the point at which the gravitational forces by the Earth and the Moon on an object will cancel out to be zero. Let this point be at a distance \( x \) from the Earth's center, meaning the distance from the Moon's center is \( D - x \). The gravitational force can be given as \( F = \frac{G \, m_1 \, m_2}{r^2} \), where \( G \) is the gravitational constant, \( m_1 \) and \( m_2 \) are masses, and \( r \) is the distance.
02

Set Up the Gravitational Force Equation

The gravitational force exerted by the Earth \( F_E \) and the Moon \( F_M \) will balance each other. The masses of the Earth \( M_E = 81 M_M \) and Moon \( M_M \) play a role here. Set the forces equal to each other: \[ \frac{GM_EM}{x^2} = \frac{GM_MM}{(D-x)^2} \]with \( M_E = 81 M_M \).
03

Simplify the Expression

We can cancel \( G \) and the mass \( M \) from both sides, simplifying the equation to: \[ \frac{81 M_M}{x^2} = \frac{M_M}{(D-x)^2} \]which reduces further to: \[ \frac{81}{x^2} = \frac{1}{(D-x)^2} \].
04

Solve for \( x \)

By cross-multiplying, we obtain \[ 81 (D-x)^2 = x^2 \]. Expanding the equation, we have \[ (D-x)^2 = \frac{x^2}{81} \]leading to \[ D^2 - 2Dx + x^2 = \frac{x^2}{81} \].
05

Rearrange and Factor

Rearrange to form: \[ 81 (D^2 - 2Dx + x^2) = x^2 \].Multiply through to get \[ 81D^2 - 162Dx + 81x^2 = x^2 \].Simplify by combining like terms: \[ 81D^2 - 162Dx = 0 \] by setting \[ 80x^2 \] on the left-hand side.
06

Solve for \( x \)

Since \( 81D^2 = 162Dx + 80x^2 \) implies zero of the quadratic free term, we simplify to solve \[ x = \frac{9D}{10} \]. This solution indicates that the point where gravitational force is zero is at \( \frac{9D}{10} \) from the Earth's center.

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.

Gravitational Force
Gravitational force is a natural phenomenon by which all things with mass or energy are brought toward one another. In our exercise, we are dealing with the gravitational forces between the Earth and the Moon. These forces are described by Newton's Law of Universal Gravitation. According to this law, the gravitational force that two masses exert on each other is:
  • Directly proportional to the product of their masses, and
  • Inversely proportional to the square of the distance between their centers.
This law is represented mathematically by the formula: \[ F = \frac{G \, m_1 \, m_2}{r^2} \]Here, \( F \) is the gravitational force, \( G \) is the gravitational constant, \( m_1 \) and \( m_2 \) are the masses, and \( r \) is the distance between the centers of the two masses.
In order to determine the point where the gravitational forces from the Earth and the Moon cancel each other out, we need to find the balance of these forces. This is done by setting the gravitational force exerted by the Earth on an object equal to the gravitational force exerted by the Moon on the same object.
Distance Calculation
The distance calculation in this exercise revolves around finding the exact location where the gravitational pull of the Earth and the Moon on an object is perfectly balanced. As the problem states, the distance between the centers of the Earth and the Moon is given as \( D \). We need to calculate the specific point \( x \) from the Earth where the gravitational forces cancel each other out. In the exercise solution, this is approached through setting up the equations of gravitational force exerted by Earth and Moon and then solving for \( x \).
Remove \( G \) and any common factors to simplify the equation and solve:
  • Gravitational force from Earth is proportional to \( \frac{81}{x^2} \)
  • Gravitational force from Moon is proportional to \( \frac{1}{(D-x)^2} \)
By solving these equivalencies, we find that at \( x = \frac{9D}{10} \), the forces are equal, making the gravitational force on an object zero at this point.
Mass Ratio
Understanding the mass ratio is crucial to determining the point of gravitational equilibrium. In our scenario, the mass of the Earth is 81 times that of the Moon. This mass ratio impacts how gravitational forces are distributed between the two celestial bodies. The mass comparison emphasizes how much stronger Earth's gravitational influence is compared to that of the Moon, due to its larger mass.
The formula from the gravitational force equation can be simplified because of this known mass ratio. When set to balance each other, the mass ratio tells us that the stronger gravitational pull from the Earth must be at a greater distance compared to the Moon's pull. These relationships are expressed as:
  • Mass of Earth \( M_E = 81 \times \) mass of Moon \( M_M \)
  • Balance is located closer to the Moon but still significantly influenced by Earth's mass.
In finding the zero gravitational force point, the ratio helps isolate the variable \( x \) in terms of the distance \( D \), allowing us to pinpoint exactly where the effective gravitational force is neutral.

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 tunnel is dug along the diameter of the earth (radius \(R\) and mass \(M\) ). There is a particle of mass ' \(m\) ' at the centre of the tunnel. The minimum velocity given to the particle so that it just reaches to the surface of the earth is (1) \(\sqrt{\frac{G M}{R}}\) (2) \(\sqrt{\frac{G M}{2 R}}\) (3) \(\sqrt{\frac{2 G M}{R}}\) (4) it will reach with the help of a negligible velocity

A planet is revolving in an elliptical orbit around the Sun. Its closest distance from the Sun is \(r_{\min }\) and the farthest distance is \(r_{\max }\). If the velocity of the planet at the distance of the closest approach is \(v_{1}\) and that at the farthest distance from the Sun is \(v_{2}\), then \(v_{1} / v_{2}\) (1) \(\frac{r_{\max }}{r_{\min }}\) (2) \(\frac{r_{\min }}{r_{\max }}\) (3) \(\frac{r_{\min }+r_{\max }}{r_{\max }-r_{\min }}\) (4) none of these

A space station is set up in space at a distance equal to the earth's radius from the surface of the earth. Suppose a satellite can be launched from the space station. Let \(v_{1}\) and \(v_{2}\) be the escape velocities of the satellite on the earth's surface and space station, respectively. Then (1) \(v_{2}=v_{1}\) (2) \(v_{2}v_{1}\) (4) \((1),(2)\) and (3) are valid depending on the mass of satellite

Two particles of mass \(m\) and \(4 m\) are at rest at an infinite separation. They move towards each other under mutual gravitational attraction. If \(G\) is the universal gravitational constant. Then at separation \(r\), (Assume zero reference potential energy at infinite separation) (1) the total energy of the two object is zero (2) their relative velocity of approach is \(\left(\frac{10 G m}{r}\right)^{1 / 2}\) in magnitude (3) the total kinetic energy of the object is \(\frac{4 G m^{2}}{r}\) (4) Net angular momentum of both the particles is zero about any point

A particle of mass \(50 \mathrm{~g}\) is kept on the surface of a uniform sphere of mass \(120 \mathrm{~kg}\) and radius \(50 \mathrm{~cm}\). Find the work to be done against the gravitational force between them (in \(\mathrm{nJ}\) ) to take the particle far away from the sphere. Take \(G=6.67\) \(\times 10^{-11} \mathrm{~N} \mathrm{~m}^{2} \mathrm{~kg}^{-2}\)

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.