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Ch 13: Gravitation
Chapter 13, Problem 13.19

A planet orbiting a distant star has radius 3.24 * 10^6 m. The escape speed for an object launched from this planet’s surface is 7.65 * 10^3 m/s. What is the acceleration due to gravity at the surface of the planet?

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Identify the given values: radius of the planet (R) = 3.24 \times 10^6 \text{ m}, escape speed (v_e) = 7.65 \times 10^3 \text{ m/s}.
Recall the formula for escape speed: v_e = \sqrt{2gR}, where g is the acceleration due to gravity and R is the radius of the planet.
Rearrange the escape speed formula to solve for g: g = \frac{v_e^2}{2R}.
Substitute the given values into the rearranged formula: g = \frac{(7.65 \times 10^3 \text{ m/s})^2}{2 \times (3.24 \times 10^6 \text{ m})}.
Calculate the value of g using the substituted values to find the acceleration due to gravity at the surface of the planet.

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Key Concepts

Here are the essential concepts you must grasp in order to answer the question correctly.

Escape Velocity

Escape velocity is the minimum speed needed for an object to break free from the gravitational attraction of a celestial body without any additional propulsion. It depends on the mass of the body and the distance from its center. The formula for escape velocity (v) is given by v = √(2GM/r), where G is the gravitational constant, M is the mass of the body, and r is the radius from the center of the body.
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Gravitational Acceleration

Gravitational acceleration is the acceleration experienced by an object due to the gravitational force exerted by a massive body. On the surface of a planet, it can be calculated using the formula g = GM/r², where G is the gravitational constant, M is the mass of the planet, and r is the radius of the planet. This acceleration determines how quickly an object will fall towards the planet's surface.
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Relationship Between Escape Velocity and Gravitational Acceleration

There is a direct relationship between escape velocity and gravitational acceleration. The escape velocity can be expressed in terms of gravitational acceleration as v = √(2gr), where g is the gravitational acceleration and r is the radius of the planet. This relationship allows us to derive the gravitational acceleration at the surface of a planet if the escape velocity and radius are known.
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Related Practice
Textbook Question
On July 15, 2004, NASA launched the Aura spacecraft to study the earth's climate and atmosphere. This satellite was injected into an orbit 705 km above the earth's surface. Assume a circular orbit. (a) How many hours does it take this satellite to make one orbit?
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Textbook Question
For a satellite to be in a circular orbit 890 km above the surface of the earth, (a) what orbital speed must it be given?
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Textbook Question
Two uniform spheres, each of mass 0.260 kg, are fixed at points A and B (Fig. E13.5). Find the magnitude and direction of the initial acceleration of a uniform sphere with mass 0.010 kg if released from rest at point P and acted on only by forces of gravitational attraction of the spheres at A and B.
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Textbook Question

A uniform, solid, 1000.0-kg sphere has a radius of 5.00 m. (a) Find the gravitational force this sphere exerts on a 2.00-kg point mass placed at the following distances from the center of the sphere: (i) 5.01 m, (ii) 2.50 m.

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Textbook Question

A thin, uniform rod has length L and mass M. A small uniform sphere of mass m is placed a distance x from one end of the rod, along the axis of the rod (Fig. E13.34)<IMAGE>. (a) Calculate the gravitational potential energy of the rod–sphere system. Take the potential energy to be zero when the rod and sphere are infinitely far apart. Show that your answer reduces to the expected result when x is much larger than L.

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Textbook Question

Consider the ringshaped body of Fig. E13.35<IMAGE>. A particle with mass m is placed a distance x from the center of the ring, along the line through the center of the ring and perpendicular to its plane. (a) Calculate the gravitational potential energy U of this system. Take the potential energy to be zero when the two objects are far apart. (b) Show that your answer to part (a) reduces to the expected result when x is much larger than the radius a of the ring. (c) Use Fx = -dU>dx to find the magnitude and direction of the force on the particle (see Section 7.4). (d) Show that your answer to part (c) reduces to the expected result when x is much larger than a. (e) What are the values of U and Fx when x = 0? Explain why these results make sense.

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