Home / IBDP Physics- D.1 Gravitational fields- IB Style Questions For HL Paper 1A

IBDP Physics- D.1 Gravitational fields- IB Style Questions For HL Paper 1A -FA 2025

Question

Planet P has diameter 1/3 of Earth’s and mass 1/18 of Earth’s. If Earth’s surface gravity is g, what is P’s surface gravity?
(A) g/6
(B) g/2
(C) 2g
(D) 6g
▶️ Answer/Explanation
Detailed solution

Gravitational field strength g = GM/R²
For Earth: g = GM_E/R_E²
For Planet P: g_P = GM_P/R_P² = G(M_E/18)/(R_E/3)² = (G M_E/18)/(R_E²/9) = (G M_E/R_E²) × (9/18) = g × 1/2
Answer: (B) g/2

Question

The escape speed from the surface of Earth is \( v_{\mathrm{esc}} \). The radius of Earth is \( R \). A satellite of mass \( m \) is in orbit at a height \( \dfrac{R}{4} \) above the surface of Earth.
What is the energy required to move the satellite to infinity?
(A) \( \dfrac{m v_{\mathrm{esc}}^{2}}{5} \)
(B) \( \dfrac{2 m v_{\mathrm{esc}}^{2}}{5} \)
(C) \( m v_{\mathrm{esc}}^{2} \)
(D) \( 2 m v_{\mathrm{esc}}^{2} \)
▶️ Answer / Explanation
Detailed solution

The satellite is initially in a circular orbit at a distance \( r = R + \dfrac{R}{4} = \dfrac{5R}{4} \) from the centre of Earth.

The total mechanical energy of a satellite in circular orbit is:

\( E = -\dfrac{GMm}{2r} \)

Substituting \( r = \dfrac{5R}{4} \):

\( E = -\dfrac{GMm}{2 \times \dfrac{5R}{4}} = -\dfrac{2GMm}{5R} \)

At infinity, both the gravitational potential energy and kinetic energy are zero. Therefore, the energy required to move the satellite to infinity is:

\( E_{\text{required}} = \dfrac{2GMm}{5R} \)

The escape speed from the surface of Earth is given by:

\( v_{\mathrm{esc}} = \sqrt{\dfrac{2GM}{R}} \)

Squaring and substituting:

\( GM = \dfrac{v_{\mathrm{esc}}^{2} R}{2} \)

Hence,

\( E_{\text{required}} = \dfrac{2}{5} m \times \dfrac{v_{\mathrm{esc}}^{2} R}{2R} = \dfrac{m v_{\mathrm{esc}}^{2}}{5} \)

Answer: (A)

Question

Two isolated point masses, P of mass \(m\) and Q of mass \(2m\), are separated by a distance \(3d\). X is a point a distance \(d\) from P and \(2d\) from Q.
What is the net gravitational field strength at X and the net gravitational potential at X?
OptionNet gravitational field strength at XNet gravitational potential at X
A\( \dfrac{Gm}{d^{2}} \)\( 0 \)
B\( \dfrac{Gm}{d^{2}} \)\( -\dfrac{2Gm}{d} \)
C\( \dfrac{Gm}{2d^{2}} \)\( 0 \)
D\( \dfrac{Gm}{2d^{2}} \)\( -\dfrac{2Gm}{d} \)
▶️ Answer / Explanation
Detailed solution

The gravitational field strength due to a point mass is \( g = \dfrac{GM}{r^{2}} \).

At X, the field due to mass P is \( g_P = \dfrac{Gm}{d^{2}} \).

The field due to mass Q is \( g_Q = \dfrac{G(2m)}{(2d)^{2}} = \dfrac{Gm}{2d^{2}} \).

These fields act in opposite directions, so the net gravitational field strength at X is

\( g_X = g_P – g_Q = \dfrac{Gm}{2d^{2}} \).

The gravitational potential due to a point mass is \( V = -\dfrac{GM}{r} \).

Potential at X due to P is \( V_P = -\dfrac{Gm}{d} \), and due to Q is \( V_Q = -\dfrac{Gm}{d} \).

Hence, the net gravitational potential at X is \( V_X = -\dfrac{2Gm}{d} \).

Answer: D

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