Cambridge A-Level Physics 9702 – Gravitational Potential Energy and Kinetic Energy
Gravitational Potential Energy (GPE) and Kinetic Energy
Learning Objective
Derive, using the work‑energy principle \$W = F s\$, the expression
\$\Delta EP = mg\,\Delta h\$
for the change in gravitational potential energy of an object moving in a uniform gravitational field.
Key Concepts
Work: \$W = \mathbf{F}\cdot\mathbf{s}=Fs\cos\theta\$ where \$F\$ is the magnitude of a constant force, \$s\$ the displacement, and \$\theta\$ the angle between them.
Uniform gravitational field: Near the Earth’s surface the acceleration due to gravity \$g\$ is approximately constant (≈ 9.81 m s⁻²).
Potential energy change: The work done by a conservative force (gravity) is stored as potential energy.
Derivation Using \$W = Fs\$
Consider an object of mass \$m\$ moving vertically a distance \$\Delta h\$ in a uniform gravitational field.
The weight of the object is the constant force \$F_g = mg\$ acting downward.
If the object is displaced upward, the angle between the force (downward) and the displacement (upward) is \$\theta = 180^\circ\$, so \$\cos\theta = -1\$.
Apply the definition of work:
\$W{\text{gravity}} = Fg\,\Delta h \cos\theta = mg\,\Delta h (-1) = -mg\,\Delta h.\$
For a conservative force, the work done by the force equals the negative change in the associated potential energy:
\$W_{\text{gravity}} = -\Delta EP.\$
Combine the two expressions for \$W_{\text{gravity}}\$:
\$- \Delta EP = - mg\,\Delta h \quad\Longrightarrow\quad \Delta EP = mg\,\Delta h.\$
Assumptions Made
The gravitational field is uniform (constant \$g\$) over the height interval \$\Delta h\$.
Air resistance and other non‑conservative forces are neglected.
The displacement is strictly vertical; horizontal components do not affect the work done by gravity.
Table of Symbols
Symbol
Quantity
Units
\$m\$
Mass of the object
kg
\$g\$
Acceleration due to gravity (uniform)
m s⁻²
\$\Delta h\$
Vertical displacement (positive upward)
m
\$\Delta EP\$
Change in gravitational potential energy
J
\$W_{\text{gravity}}\$
Work done by the weight of the object
J
Example Problem
Question: A 2.0 kg block is lifted vertically by 0.50 m from the floor. Calculate the increase in its gravitational potential energy.
Solution:
Identify the given values: \$m = 2.0\;\text{kg}\$, \$\Delta h = 0.50\;\text{m}\$, \$g = 9.81\;\text{m s}^{-2}\$.
Apply the derived formula:
\$\Delta EP = mg\,\Delta h = (2.0\;\text{kg})(9.81\;\text{m s}^{-2})(0.50\;\text{m}) = 9.81\;\text{J}.\$
Therefore, the block’s gravitational potential energy increases by \$9.8\;\text{J}\$ (to two significant figures).
Connection to Kinetic Energy
When an object moves under gravity without non‑conservative forces, the total mechanical energy is conserved:
\$\Delta EP + \Delta KE = 0 \quad\Longrightarrow\quad \Delta KE = -\Delta EP.\$
This relationship explains why an object falling a height \$\Delta h\$ gains kinetic energy \$KE = mg\,\Delta h\$.
Suggested diagram: A block of mass \$m\$ being lifted a height \$\Delta h\$ with the weight \$mg\$ acting downward and the displacement \$s\$ upward.
Summary
The work done by a constant gravitational force over a vertical displacement \$\Delta h\$ is \$W_{\text{gravity}} = -mg\,\Delta h\$.
Because gravity is conservative, \$W_{\text{gravity}} = -\Delta EP\$, leading directly to \$\Delta EP = mg\,\Delta h\$.
This expression is valid for any motion in a uniform gravitational field, provided non‑conservative forces are negligible.