Potential Energy (Gravitational)
The potential energy (positional energy) of a body of mass m at height h in the homogeneous gravitational field g.
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Formula
E_{pot} = m \cdot g \cdot hVariables & units – Potential Energy (Gravitational)
| Symbol | Meaning | Unit |
|---|---|---|
| E_pot | Potential energy | J |
| m | Mass | kg |
| g | Acceleration due to gravity (9.81 m/s²) | m/s² |
| h | Height above the reference level | m |
Derivation & background – Potential Energy (Gravitational)
Holds exactly only in homogeneous gravitational fields (an approximation at the surface of the Earth). For large heights: E_pot = -G·M·m/r (the general form). The conservation of energy: E_kin + E_pot = const. (for conservative forces).
Exam blueprint
Validity range
Applies in an approximately uniform gravitational field near Earth and relative to a chosen reference height.
Derivation steps
Potential energy is lifting work against weight.
- 1Weight force: F_G = m·g.
- 2Lifting work for constant force: W = F_G·h = m·g·h.
Rearrangements
Height from energy
The zero height is arbitrary; energy differences are physically decisive.
Task variant
What energy does a 50 kg body gain at 4 m height?
E = mgh = 50·9.81·4 ≈ 1962 J.
Common mistakes
Interpreting h as absolute rather than relative to the chosen reference level.
Define the zero level before calculating.
Exam context
- Often asked with falling motion, energy conservation and efficiency.
These mistakes cost points in real exams. The set drills them until they stick.
Formula cluster
Mechanical energy
Complements kinetic energy and gravitational force models.
Worked example
A mountaineer (m = 80 kg) at an altitude of 3,000 m: E_pot = 80 × 9.81 × 3,000 ≈ 2.35 MJ, the energy of a package of explosives.
Applications
Pumped-storage power plants, drop-tower experiments, bridge statics, spaceflight
Quanta exam set
Curated exam set for "Potential Energy (Gravitational)":
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Which formula describes Potential Energy (Gravitational)?
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Question (front)
How do you rearrange Epot = mgh for Height from energy?
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Which common mistake happens with Potential Energy (Gravitational)?
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Frequently asked questions about Potential Energy (Gravitational)
How do you calculate potential energy in a gravitational field?+
Multiply the mass in kilograms by the local factor g ≈ 9.81 m/s² and by the height h in metres: E_pot = m·g·h. The result is the positional energy in joules. A body of 50 kg at 4 m height has E_pot = 50·9.81·4 ≈ 1962 J. The height h is always understood relative to a freely chosen zero level, usually the ground or a table top. Only height differences are physically meaningful, since the absolute height depends on the chosen reference point. Insert g as 9.81 or, rounded, 10 m/s² depending on the task.
Why can you freely choose the zero level of height?+
Because only energy differences act physically, not the absolute energy value. When a body falls from one height to another, only the height difference matters for the energy converted. Whether you place the zero level at the ground or at the table edge changes the numerical value of E_pot, but the difference between start and finish stays the same. Therefore you deliberately fix the zero level before each calculation and keep it. A common mistake is to interpret h as absolute height above sea level, although the problem means the height above the ground.
How are potential and kinetic energy linked in free fall?+
Without friction the total mechanical energy stays constant, so E_pot + E_kin = constant. During the fall the body loses height and thus potential energy, but gains exactly the same amount of kinetic energy. Setting m·g·h = ½·m·v² cancels the mass and gives the impact speed v = √(2·g·h). From 5 m height, for example, v = √(2·9.81·5) ≈ 9.9 m/s, independent of the mass. This energy approach is often faster than the equations of motion, because you do not even need to know the fall time.
When does E_pot = m·g·h no longer apply?+
The formula assumes a nearly uniform gravitational field, that is a constant local factor g. This holds well near the ground as long as the height is small compared with the Earth radius. If you rise to several hundred kilometres, for example into a satellite orbit, g decreases noticeably and you need the general gravitational potential energy, E_pot = −G·m·M/r. On other celestial bodies you must also insert their own local factor, on the Moon about 1.62 m/s². For everyday heights from metres to a few kilometres, however, E_pot = m·g·h gives very accurate values.
How do you rearrange E_pot = m·g·h for the height?+
Divide the potential energy by the product of mass and local factor: h = E_pot/(m·g). The height is therefore the ratio of positional energy to weight, since m·g is exactly the weight F_G. Insert the energy in joules, the mass in kilograms and g in m/s², then h comes out in metres. Example: 1962 J at 50 kg give h = 1962/(50·9.81) = 4 m. If you want the mass instead, rearrange to m = E_pot/(g·h). Always check the result for plausibility; negative heights usually point to a sign or reference error.
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How do you calculate with Potential Energy (Gravitational)?
Here is how to work through a typical Potential Energy (Gravitational) (Epot = mgh) task step by step:
- 1
Task
What energy does a 50 kg body gain at 4 m height?
Solution path
E = mgh = 50·9.81·4 ≈ 1962 J.