Problem 707
Question
The density of a newly discovered planet is twice that of earth. The acceleration due to gravity at the surface of the planet is equal to that at the surface of earth. If the radius of the earth is \(\mathrm{R}\), the radius of planet would be (A) \(2 \mathrm{R}\) (B) \(4 \mathrm{R}\) (C) \(1 / 4 \mathrm{R}\) (D) \(\mathrm{R} / 2\)
Step-by-Step Solution
Verified Answer
The planet's radius is half the Earth's radius, which is represented as (D) \(\mathrm{R} / 2\).
1Step 1: Write down the gravitational force formula
The formula for gravitational force between two objects is \( F = G * \frac{m_1 * m_2}{r^2}\), where G is the gravitational constant, m1 and m2 are the masses of the objects, and r is the distance between their centers.
2Step 2: Write down the density formula
The formula for density is \(ρ = \frac{m}{V}\), where ρ is the density, m is the mass, and V is the volume. Since both Earth and the planet are assumed to be spheres, their volumes can be represented by the formula for the volume of a sphere, which is \(V = \frac{4}{3}πr^3\).
3Step 3: Set up equations for Earth and the planet
Let's denote Earth's density as \(ρ_e\) and the planet's density as \(ρ_p\). We know that \(ρ_p = 2ρ_e\). We also know that the gravitational forces on their surfaces are the same. Therefore, we can set up two equations:
1. For Earth: \[F_e = G * \frac{m_e * m}{r_e^2}\]
2. For the planet: \[F_p = G * \frac{m_p * m}{r_p^2}\]
Since \(F_e = F_p\), let's set these two equations equal to each other and eliminate G and m:
\(G * \frac{m_e * m}{r_e^2} = G * \frac{m_p * m}{r_p^2}\)
4Step 4: Express the masses of Earth and the planet in terms of their densities
From the density formulas, we have:
1. \(m_e = ρ_e * V_e = ρ_e * \frac{4}{3}πr_e^3\)
2. \(m_p = ρ_p * V_p = (2ρ_e) * \frac{4}{3}πr_p^3\)
Now, substitute these expressions for the masses into the equation from Step 3:
\(\frac{\rho_e * \frac{4}{3}πr_e^3 * m}{r_e^2} = \frac{(2\rho_e) * \frac{4}{3}πr_p^3 * m}{r_p^2}\)
5Step 5: Solve for the planet's radius in terms of Earth's radius
First, cancel out the common terms from the equation:
\(\frac{r_e^3 * \rho_e}{r_e^2} = \frac{2 * r_p^3 * \rho_e}{r_p^2}\)
Next, cancel out the remaining common terms:
\(r_e = 2 * r_p\)
Now, solve for the planet's radius, \(r_p\):
\(r_p = \frac{r_e}{2}\)
So the correct answer is (D) \(\mathrm{R} / 2\). The planet's radius is half the Earth's radius.
Key Concepts
Gravitational ForceDensity FormulaSphere Volume CalculationEqual Surface Gravity Conditions
Gravitational Force
Gravitational force is a fundamental concept that describes the force of attraction between two masses. This force is given by Newton's law of universal gravitation, represented by the formula: \ \[ F = G \frac{m_1 m_2}{r^2} \] where:
- \( F \) is the gravitational force, measured in Newtons,
- \( G \) is the gravitational constant, approximately \( 6.674 \times 10^{-11} \, \text{Nm}^2/\text{kg}^2 \),
- \( m_1 \) and \( m_2 \) are the masses of the two objects,
- \( r \) is the distance between the centers of the two masses.
Density Formula
Density is a key property that relates mass to volume in a substance or object. It is defined by the formula: \ \[ \rho = \frac{m}{V} \] where:
This concept is crucial because it gives insight into the internal structure and composition of a celestial body, helping us understand surface conditions like gravity.
- \( \rho \) is the density,
- \( m \) is the mass,
- \( V \) is the volume.
This concept is crucial because it gives insight into the internal structure and composition of a celestial body, helping us understand surface conditions like gravity.
Sphere Volume Calculation
Understanding the volume of a sphere is essential for various applications, including planetary sciences. The volume of a sphere is calculated with the following formula: \ \[ V = \frac{4}{3} \pi r^3 \] where:
When solving problems involving planetary volume, it becomes possible to relate volume changes to other factors like mass and density, which are crucial in gravitational physics.
- \( V \) is the volume,
- \( r \) is the radius of the sphere.
When solving problems involving planetary volume, it becomes possible to relate volume changes to other factors like mass and density, which are crucial in gravitational physics.
Equal Surface Gravity Conditions
The concept of equal surface gravity conditions refers to having the same gravitational pull on the surface of two different celestial bodies. Here, both Earth and an unknown planet have such a condition despite having differing densities and radii.
When replacement is performed in our calculations, it involves equating the gravitational force experienced by objects on their surfaces. Normally for planets, this is equated as: \ \[ \frac{G m_e m}{r_e^2} = \frac{G m_p m}{r_p^2} \] where the subscript \( e \) denotes Earth and \( p \) denotes the planet.
By maintaining equal gravitational forces while acknowledging differences in density, you can solve for unknown planetary characteristics, such as radius, as in this example.
The example demonstrates how differing size and density can yet result in equal gravitational experiences at the surface. This understanding aids significantly in the fields of astronomy and geophysics.
When replacement is performed in our calculations, it involves equating the gravitational force experienced by objects on their surfaces. Normally for planets, this is equated as: \ \[ \frac{G m_e m}{r_e^2} = \frac{G m_p m}{r_p^2} \] where the subscript \( e \) denotes Earth and \( p \) denotes the planet.
By maintaining equal gravitational forces while acknowledging differences in density, you can solve for unknown planetary characteristics, such as radius, as in this example.
The example demonstrates how differing size and density can yet result in equal gravitational experiences at the surface. This understanding aids significantly in the fields of astronomy and geophysics.
Other exercises in this chapter
Problem 704
At what distance from the center of earth, the value of acceleration due to gravity \(g\) will be half that of the surfaces \((\mathrm{R}=\) Radius of earth \()
View solution Problem 705
The acceleration due to gravity near the surface of a planet of radius \(\mathrm{R}\) and density \(\mathrm{d}\) is proportional to (A) \(\mathrm{d} / \mathrm{R
View solution Problem 708
Density of the earth is doubled keeping its radius constant then acceleration, due to gravity will be \(-m s^{-2}\) \(\left(\mathrm{g}=9.8 \mathrm{~ms}^{2}\righ
View solution Problem 712
If the value of ' \(\mathrm{g}\) ' acceleration due to gravity, at earth surface is \(10 \mathrm{~ms}^{-2}\). its value in \(\mathrm{ms}^{-2}\) at the center of
View solution