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Suppose we could shrink the earth without changing its mass. At what fraction of its current radius would the free-fall acceleration at the surface be three times its present value?

Short Answer

Expert verified
The free-fall acceleration at the surface would be three times its present value if the earth's radius were shrunk to approximately 0.577 (or \(\frac{1}{\sqrt{3}}\)) of its current radius.

Step by step solution

01

Identify the Formula for Gravitational Acceleration

The acceleration due to gravity on the surface of a planet or any spherical body is given by the formula: \(g = \frac{GM}{r^2}\), where \(G\) is the gravitational constant, \(M\) is the mass of the body, and \(r\) is the radius of the body.
02

Set Up the Equation

We are told that the acceleration due to gravity becomes three times if the radius is reduced to a fraction x of the original radius. Substituting these changes in the formula and setting them equal gives: \(3g = \frac{GM}{(xr)^2}\)
03

Solve for the Fraction x

To find the fraction 'x', we will solve the equation from Step 2. We get \(x = \frac{1}{\sqrt{3}} \) or approximately 0.577

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Key Concepts

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

Gravitational Acceleration
Gravitational acceleration refers to the acceleration that a falling object experiences due to the gravitational pull of a planet. This is a result of the gravitational force that acts on the object. On the surface of the Earth, this acceleration is approximately 9.8 m/s². But why exactly 9.8 m/s²? The answer lies in the mass of the Earth and the distance of the object from its center.
Gravitational acceleration is mathematically expressed as follows:
  • \( g = \frac{GM}{r^2} \)
In this formula:
  • \( g \) stands for gravitational acceleration
  • \( G \) is the gravitational constant
  • \( M \) is the mass of the planet
  • \( r \) is the radius of the planet
This formula implies that gravitational acceleration is directly influenced by the planet's mass and inversely proportional to the square of its radius. Thus, changes to these elements will affect the strength of the gravitational pull experienced at the surface.
Gravitational Constant
The gravitational constant, denoted as \( G \), is a key player in understanding gravitational forces. It's a constant value that is used in the calculation of gravitational forces between two bodies.
Introduced by Sir Isaac Newton, the gravitational constant is approximately valued at \( 6.674 \times 10^{-11} \, \text{m}^3 \, \text{kg}^{-1} \, \text{s}^{-2} \) and is central to the law of universal gravitation.
The presence of \( G \) in the formula for gravitational acceleration \( g = \frac{GM}{r^2} \) means that regardless of how massive a planet is, the rate of free fall is proportional to the same constant. This is why gravitational calculations on planets or other celestial bodies maintain consistency and predictability. Understanding the gravitational constant is crucial in planetary physics as it provides the necessary foundation to solve complex gravity-related problems.
Radius Reduction
Radius reduction is an important concept when contemplating changes in gravitational acceleration. In our exercise, we reduced the Earth’s radius to observe how it affects gravitational pull.
Since gravitational acceleration is inversely proportional to the square of the radius (\( g = \frac{GM}{r^2} \)), a decrease in the radius of a planet will result in an increase in gravitational acceleration. Conversely, increasing the radius can decrease gravitational pull.
  • When the radius is reduced to a fraction of its original size, the gravitational pull increases.
  • This is evident in the formula adjustment, where reducing the Earth’s radius by a factor of \( x \) increases the gravitational force experienced on the surface.
In practical terms, shrinking a planet without changing its mass implies that the planet becomes denser, making the gravitational field more intense at the surface.
Planetary Physics
Planetary physics is the field of science concerned with the study of planets and celestial objects. It examines how various physical principles apply to these bodies.
This includes understanding gravitational forces, atmospheres, and the properties of celestial bodies. A key focus is on how gravity—the force that pulls objects toward each other—affects these celestial bodies and their surroundings.
  • Gravitational forces determine orbital paths, surface gravity conditions, and even atmospheric composition.
  • These principles are fundamental to predicting the behavior of planets and planning space missions.
Our Earth serves as an ideal model for studying these concepts, as altering parameters like radius or mass can provide insight into how fundamental physics impacts a planet's environment. Through problem-solving exercises such as the one detailed, we deepen our understanding of the intricate balance that governs celestial mechanics.

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Most popular questions from this chapter

What is the escape speed from Jupiter?

A projectile is fired from the earth in the direction of the earth's motion around the sun. What minimum speed must the projectile have relative to the earth to escape the solar system? Ignore the earth's rotation. Hint: This is a three-part problem. First find the speed a projectile at the earth's distance needs to escape the sun. Transform that speed into the earth's reference frame, then determine how fast the projectile must be launched to have this speed when far from the earth.

The solar system is 25.000 light years from the center of our Milky Way galaxy. One light year is the distance light travels in one year at a speed of \(3.0 \times 10^{8} \mathrm{m} / \mathrm{s}\). Astronomers have delermined that the solar system is orbiting the center of the galaxy at a speed of \(230 \mathrm{km} / \mathrm{s}\). a. Assuming the orbit is circular, what is the period of the solar system's orbit? Give your answer in years. b. Our solar system was formed roughly 5 billion years ago. How many orbits has it completed? c. The gravitational force on the solar system is the net force due to all the matter inside our orbit. Most of that matter is concentrated near the center of the galaxy. Assume that the matter has a spherical distribution, like a giant star. What is the approximate mass of the galactic center? d. Assume that the sun is a typical star with a typical mass. If galactic matter is made up of stars, approximately how many stars are in the center of the galaxy? Astronomers have spent many years trying to determine how many stars there are in the Milky Way. The number of stars seems to be only about \(10 \%\) of what you found in part d. In other words, about \(90 \%\) of the mass of the galaxy appears to be in some form other than stars. This is called the dark matter of the universe. No one knows what the dark matter is. This is one of the outstanding scientific questions of our day.

A \(1.0 \mathrm{kg}\) object is released from rest \(500 \mathrm{km}\) ( \(\sim 300\) miles) above the earth. a. What is its impact speed as it hits the ground? Ignore air resistance. b. What would the impact speed be if the earth were flat? c. By what percentage is the flat-earth calculation in error?

You are the science officer on a visit to a distant solar system. Prior to landing on a planet you measure its diameter to be \(1.8 \times 10^{7} \mathrm{m}\) and its rotation period to be 22.3 hours. You have previously determined that the planet orbits \(2.2 \times 10^{11} \mathrm{m}\) from its star with a period of 402 carth days. Once on the surface you find that the free-fall acceleration is \(12.2 \mathrm{m} / \mathrm{s}^{2}\). What are the mass of (a) the planet and (b) the star?

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