IBDP Physics- D.1 Gravitational fields- IB Style Questions For HL Paper 1A -FA 2025
Question
Which is a statement of one of Kepler’s laws of orbital motion?
(B) A line segment joining a planet and the Sun sweeps out equal arc lengths during equal intervals of time.
(C) A planet’s orbital period is proportional to the cube of the length of the semi-major axis of its orbit.
(D) The orbit of a planet is an ellipse with the Sun positioned at the centre.
▶️ Answer/Explanation
Correct Answer: \( \boxed{\mathrm{A}} \)
Kepler’s third law states that the square of the orbital period is proportional to the cube of the semi-major axis:
\(T^2\propto a^3\)
where \(T\) is the orbital period and \(a\) is the semi-major axis of the orbit.
Option B is incorrect because Kepler’s second law refers to equal areas, not equal arc lengths, being swept out in equal intervals of time.
Option C incorrectly states \(T\propto a^3\), rather than \(T^2\propto a^3\).
Option D is incorrect because the Sun is located at one focus of the elliptical orbit, not at its centre.
Hence, the correct answer is \( \boxed{\mathrm{A}} \).
Question
Isolated planets X and Y have masses \(M_X\) and \(M_Y\) respectively and are separated by a distance \(R\).

A point P is located at a distance \(\dfrac{R}{3}\) from planet X, as shown. The gravitational field strength at P is zero.
What is \(\dfrac{M_Y}{M_X}\)?
(B) \(3\)
(C) \(4\)
(D) \(9\)
▶️ Answer/Explanation
Correct Answer: \( \boxed{\mathrm{C}} \)
At P, the gravitational fields due to X and Y are equal in magnitude and opposite in direction.
The gravitational field strength due to a mass \(M\) at distance \(r\) is
\(g=\dfrac{GM}{r^2}\)
The distance from X to P is \(\dfrac{R}{3}\), while the distance from P to Y is
\(R-\dfrac{R}{3}=\dfrac{2R}{3}\)
Since the resultant gravitational field at P is zero,
\(\dfrac{GM_X}{(R/3)^2}=\dfrac{GM_Y}{(2R/3)^2}\)
Cancelling \(G\) and \(R^2\),
\(\dfrac{M_X}{1/9}=\dfrac{M_Y}{4/9}\)
Therefore,
\(9M_X=\dfrac{9}{4}M_Y\)
\(\dfrac{M_Y}{M_X}=4\)
Hence, the correct answer is \( \boxed{\mathrm{C}} \).
Question


| Option | Net gravitational field strength at X | Net 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
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
