Edexcel A Level (IAL) Physics-5.34 Gravitational Potential for a Radial Field- Study Notes- New Syllabus
Edexcel A Level (IAL) Physics -5.34 Gravitational Potential for a Radial Field- Study Notes- New syllabus
Edexcel A Level (IAL) Physics -5.34 Gravitational Potential for a Radial Field- Study Notes -Edexcel A level Physics – per latest Syllabus.
Key Concepts:
- be able to use the equation \( V_{\text{grav}} = \dfrac{-Gm}{r} \) for a radial gravitational field
Gravitational Potential in a Radial Gravitational Field
Gravitational potential describes the energy per unit mass at a point in a gravitational field. For a radial gravitational field (around a point mass), gravitational potential depends on distance from the mass.
Definition of Gravitational Potential
Gravitational potential \( V_{\text{grav}} \) at a point is defined as:
- The work done per unit mass in bringing a small test mass from infinity to that point.
- No change in kinetic energy occurs during this process.
Reference point: Gravitational potential is taken as zero at infinity.
Gravitational Potential Due to a Point Mass
For a radial gravitational field produced by a point mass \( m \), the gravitational potential is:![]()
\( V_{\text{grav}} = \dfrac{-Gm}{r} \)
- \( V_{\text{grav}} \) = gravitational potential (J kg⁻¹)
- \( G \) = gravitational constant
- \( m \) = mass producing the field (kg)
- \( r \) = distance from the centre of the mass (m)
Meaning of the Negative Sign
- The gravitational force is attractive.
- Work must be done to move a mass away from the field.
- Potential increases (becomes less negative) as distance increases.
Key idea: At infinity, \( V_{\text{grav}} = 0 \).
Variation of Gravitational Potential with Distance
- Gravitational potential increases with distance from the mass.
- As \( r \rightarrow \infty \), \( V_{\text{grav}} \rightarrow 0 \).
- The graph of \( V_{\text{grav}} \) against \( r \) is a curve, not a straight line.
Important distinction:
- Gravitational potential is a scalar quantity.
- It has no direction.
Relation to Gravitational Field Strength
Gravitational field strength is related to the gradient of gravitational potential:![]()
\( g = -\dfrac{dV_{\text{grav}}}{dr} \)
Using \( V_{\text{grav}} = \dfrac{-Gm}{r} \):
\( g = \dfrac{Gm}{r^2} \)
This confirms consistency with Newton’s law of gravitation.
Using the Equation in Calculations
- Ensure distance is measured from the centre of the mass.
- Use SI units throughout.
- Remember potential values are negative.
Rearranged forms:
\( m = \dfrac{-V_{\text{grav}} r}{G} \)
\( r = \dfrac{-Gm}{V_{\text{grav}}} \)
Exam Tips
- Do not confuse gravitational potential with potential energy.
- Always mention “per unit mass”.
- Explain the negative sign physically.
- State reference point clearly (infinity).
Example (Easy)
What is the gravitational potential at infinity?
▶️ Answer / Explanation
Gravitational potential at infinity is defined as zero.
Example (Medium)
Calculate the gravitational potential \( 8.0\times10^{6}\,\mathrm{m} \) from the centre of the Earth \( (m = 6.0\times10^{24}\,\mathrm{kg}) \).
▶️ Answer / Explanation
\( V_{\text{grav}} = \dfrac{-(6.67\times10^{-11})(6.0\times10^{24})}{8.0\times10^{6}} \)
\( V_{\text{grav}} \approx -5.0\times10^{7}\,\mathrm{J\,kg^{-1}} \)
Example (Hard)
Explain why gravitational potential becomes less negative as distance from a planet increases.
▶️ Answer / Explanation
- The gravitational attraction weakens with distance.
- Less work is needed to move a unit mass further away.
- Potential approaches zero at infinity.
