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The density of a newly discovered planet is twice that of the earth. The acceleration due to gravity at the surface of the planet is equal to that at the surface of the earth. If the radius of the earth is \(R\) and the radius of the planet is \(R^{\prime}\). Then wat is the value of \(R / R^{\prime}\) ?

Short Answer

Expert verified
\( \frac{R}{R^{\prime}} = \sqrt[3]{2} \)

Step by step solution

01

Understanding the given problem

We are given that the density of the planet is twice the density of Earth, and the acceleration due to gravity at the planet's surface equals that at Earth's surface. We need to find the relationship between the radius of Earth \(R\) and the radius of the planet \(R^{\prime}\).
02

Recall formulas for density and gravity

Density \( \rho \) is mass \( M \) over volume \( V \), \( \rho = \frac{M}{V} \), and volume \( V \) of a sphere is \( \frac{4}{3}\pi R^3 \). The acceleration due to gravity \( g \) on the surface is \( g = \frac{GM}{R^2} \), where \( G \) is the gravitational constant, and \( M \) is the mass of the body.
03

Set-up equations for Earth and the planet

For Earth, \( g = \frac{GM}{R^2} \) and for the planet, \( g = \frac{GM'}{(R^{\prime})^2} \). Given that \( \rho' = 2\rho \) (density of planet is twice Earth's), we express the planet's mass \( M' \) as \( M' = 2 \cdot \frac{\rho V'}{V} \cdot M \) since density relates to volume and hence \( M = \rho V \).
04

Express planetary radius using densities

By rearranging, \( \rho' = \frac{M'}{V'} = 2\rho \Rightarrow \frac{M}{\frac{4}{3}\pi (R^{\prime})^3} = 2\cdot\frac{M}{\frac{4}{3}\pi R^3}\). Cancelling out constants and expressing volumes gives \( R^3 = 2 (R^{\prime})^3 \).
05

Simplify the radius ratio

From \( R^3 = 2 (R^{\prime})^3 \), take the cube root to solve for \( R \) and \( R^{\prime} \). This yields \( R = \sqrt[3]{2} \cdot R^{\prime} \). Therefore, the ratio \( \frac{R}{R^{\prime}} = \sqrt[3]{2} \).

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Key Concepts

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

Density
Density is a fundamental concept when examining the characteristics of celestial bodies in planetary physics. It is defined as the mass of an object divided by its volume, expressed in the formula \[ \rho = \frac{M}{V} \] where \( \rho \) stands for density, \( M \) is mass, and \( V \) is volume. For spherical objects like planets, the volume \( V \) can be calculated using \( \frac{4}{3} \pi R^3 \), with \( R \) being the radius of the sphere.
  • For Earth, this relation helps us determine its density and subsequently, its gravitational pull.
  • In the given problem, the planets' density is twice that of Earth's, meaning the mass per unit volume must be significantly higher or the volume (due to radius) is adjusted accordingly to maintain this relationship.
Understanding density is crucial because it directly influences the planet's ability to exert gravitational forces, a key aspect in understanding how planets operate within their solar systems.
Gravitational Acceleration
Gravitational acceleration is the force of gravity acting on an object at the surface of a planet, which determines how strongly an object is pulled toward the planet. The standard formula for calculating this is \[ g = \frac{GM}{R^2} \] where \( g \) is the gravitational acceleration, \( G \) is the universal gravitational constant, \( M \) is the planet's mass, and \( R \) is its radius.
  • This formula shows that the force of gravity increases with an increase in mass and decreases with an increase in radius.
  • Since the gravitational acceleration of the new planet equals that of Earth, this means the mass-to-radius squared ratio of the two planets is similar.
Through this relationship, even if a planet is denser, it can maintain the same gravitational pull as Earth if it has a suitable radius proportional to its density.
Radius Ratio
The concept of radius ratio is pivotal in this problem as it connects density and gravitational acceleration to the size of a planet's radius. In the exercise, we need to find the value of the ratio between Earth's radius \( R \) and the new planet's radius \( R^{\prime} \).
When we say the new planet has twice the density of Earth, the equation rearranges to show a relationship between volumes, resulting in \[ R^3 = 2 (R^{\prime})^3 \]Taking the cube root gives us \[ R = \sqrt[3]{2} \cdot R^{\prime} \]Thus, the ratio is \[ \frac{R}{R^{\prime}} = \sqrt[3]{2} \]
  • Effectively, a denser planet achieves the same gravitational pull with a smaller radius if its density compensates effectively for its smaller size.
  • This understanding helps us realize how planets can differ in size and density yet exhibit similar surface gravity forces, demonstrating the interconnectedness of these concepts in planetary physics.
The notion of radius ratio emphasizes the delicate balance between mass distribution and gravitational influence, key for understanding planetary sizes and structures.

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Most popular questions from this chapter

A small mass \(m\) is moved slowly from the surface of the earth to a height \(h\) above the surface. The work done (by an external agent) in doing this is (1) \(m g h\), for all values of \(h\) (2) \(m g h\), for \(h \ll R\) (3) \(1 / 2 m g R\), for \(h=R\) (4) \(-1 / 2 m g R\), for \(h=R\)

Which of the following statements are true for a particle on the surface of the earth? (1) The linear speed is minimum at the equator. (2) The angular speed is maximum at the equator. (3) The linear speed is minimum at the poles. (4) The angular speed is \(7.3 \times 10^{-5} \mathrm{rad} \mathrm{s}^{-1}\) at the equator.

The small dense stars rotate about their common centre of mass as a binary system, each with a period of 1 year. One star has mass double than that of the other, while mass of the lighter star is one-third the mass of the Sun. The distance between the two stars is \(r\) and the distance of the earth from the Sun is \(R\); find the ratio \(r / R\).

If both the mass and radius of the earth decrease by \(1 \%\), the value of (1) acceleration due to gravity would decrease by nearly \(1 \%\) (2) acceleration due to gravity would increase by \(1 \%\) (3) escape velocity from the earth's surface would decrease by \(1 \%\) (4) the gravitational potential energy of a body on earth's surface will remain unchanged

The escape velocity for a body projected vertically upwards from the surface of the earth is \(11.2 \mathrm{~km} \mathrm{~s}^{-1}\). If the body is projected in a direction making an angle \(45^{\circ}\) with the vertical, the escape velocity will be (1) \(\frac{11.2}{\sqrt{2}} \mathrm{~km} \mathrm{~s}^{-1}\) (2) \(11.2 \times \sqrt{2} \mathrm{~km} \mathrm{~s}^{-1}\) (3) \(11.2 \times 2 \mathrm{~km} \mathrm{~s}^{-1}\) (4) \(11.2 \mathrm{~km} \mathrm{~s}^{-1}\)

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