D.1.9 (HL)—Potential gradient

Syllabus
First assessment 2025
Objective
Level
HL

Read the Gravitational Potential Gradient

HL only

Use the gradient relationship

Gravitational field strength is the negative spatial gradient of gravitational potential. For a graph, use the tangent gradient at the required point; the negative sign makes the field point toward decreasing potential.

g=-\frac{\Delta V_g}{\Delta r}

Worked example — graph gradient

If a tangent changes by 3.8×108Jkg13.8\times10^8\,\mathrm{J\,kg^{-1}} over 4.2×107m4.2\times10^7\,\mathrm{m}, then g=(3.8×108)/(4.2×107)=9.0Jkg1m1=9.0Nkg1|g|=(3.8\times10^8)/(4.2\times10^7)=9.0\,\mathrm{J\,kg^{-1}m^{-1}}=9.0\,\mathrm{N\,kg^{-1}}. Direction comes from the negative gradient.

Read a potential–distance graph

The gradient is ΔVg/Δr\Delta V_g/\Delta r, with units Jkg1m1=Nkg1\mathrm{J\,kg^{-1}m^{-1}}=\mathrm{N\,kg^{-1}}. A negative slope gives a positive outward radial magnitude only after the vector direction and sign convention are interpreted. Near a source, the potential changes more rapidly with distance, so the field is stronger.

Connect to work

For a mass mm moved between two points, W=mΔVgW=m\Delta V_g is the work done on the mass by the external agent under the stated sign convention. The field strength relation is local; potential difference and work compare endpoints.

Common trap

Do not use the average slope over a wide curved section as the field at one point unless the question’s graph is effectively linear there. Do not drop the negative sign without stating whether you are reporting a vector component or a magnitude.

D.1.9 (HL) Exam Analysis

HL only

Assessment in practice

1–2 marks
How it is assessed

Questions read field strength from a potential–distance graph or connect an equipotential spacing to the acceleration of a test mass.

Command terms

Determine / What is

What earns marks

Find the local tangent gradient of Vg against r, apply g=−ΔVg/Δr, keep units consistent, and interpret the sign as field direction.

Watch for

Using the graph’s height instead of its gradient, or reporting the slope sign without interpreting the negative in g=−ΔVg/Δr.

Representative question

Question 1

[Maximum number: 1]

A point mass of 5 kg is placed at point P located on one of three gravitational equipotential lines, each separated by a distance of 100 km , as shown.

What is the initial acceleration of the point mass?

A

4 m s24 \mathrm{~m} \mathrm{~s}^{-2} to the left

B

4 m s24 \mathrm{~m} \mathrm{~s}^{-2} to the right

C

20 m s220 \mathrm{~m} \mathrm{~s}^{-2} to the left

D

20 m s220 \mathrm{~m} \mathrm{~s}^{-2} to the right

Retrieve the HL D.1 Gravitational Fields Model

HL only

The HL gravitational-fields model is secure when you can move between energy, potential, gradients and orbital consequences.

  • Ep=−Gm1m2/r and Vg=−GM/r, zero at infinity
  • g=−ΔVg/Δr and W=mΔVg
  • Equipotentials are perpendicular to field lines
  • vesc=√(2GM/r) and vorbital=√(GM/r)
  • Atmospheric drag lowers orbital energy and radius while increasing the speed of the new lower orbit