3.2.4Work, Energy, and Power
Gravitational Potential Energy Near a Surface — AP PHYSICS 1 Revision Notes & Topical Questions
5 min read 9 parts Lesson 7 of 14 1 quiz
Lesson summary
3.2.4 Gravitational Potential Energy Near a Surface — AP PHYSICS 1 notes: Calculate changes in gravitational potential energy near a planet's surface with ΔUg = mgΔy and use them with kinetic energy.ΔUg = mgΔy — the change for the object–planet system when the object's height cha…
- Uniform field
- Reference level
- Lifting and lowering
- Scalar and path-independent
- Lifting at constant speed
- Work by gravity
Part 1 of 7The equation
ΔUg
ΔUg mgΔy
- the change for the object–planet system when the object's height changes by Δy.
- ΔUg in J, m in kg, g the field strength in N/kg (9.8 m/s2 on Earth), Δy the vertical change in m.
Uniform field
- Uniform field g is approximately constant near a planet's surface.
Reference level
- Reference level at height y above a chosen zero, Ug = mgy; zero points are relative.
Lifting and lowering
- Lifting and lowering lifting stores energy in the system, lowering releases it.
Scalar and path-independent
- Scalar and path-independent only the vertical change matters because gravity is conservative.
Part 2 of 7Link to work
Link to work
Lifting at constant speed
- Lifting at constant speed applied work mgΔy equals ΔUg.
Work by gravity
- −mgΔy.
Incline
- Incline gravity's work is −(mg sinθ)d, and d sinθ = Δy, giving the same −mgΔy.
Part 3 of 7Conservation of mechanical energy
1Condition
- Condition gravity is the only force doing work.
- (no friction or drag, normal forces perpendicular to motion)
2Equation
- Ki + Ui = Kf + Uf, or ½mvi2 + mgyi = ½mvf2 + mgyf.
3Mass cancels
- Mass cancels speed at a given height is independent of mass.
4Release from rest through height h
- Release from rest through height h v = √(2gh), as in free fall.
5Track shape
- Track shape only the vertical drop matters for a roller coaster or pendulum.
6With friction
- Ki + Ui + Wf = Kf + Uf with Wf negative.
Part 4 of 7Graphs and bar charts
Bar charts
- K and U at different positions with constant total height when energy is conserved.
Ball thrown upward
- U against height is a straight line through the origin with gradient mg.
K against height
- K against height a straight line falling to zero at the top; K and U mirror each other and sum to a constant.
K against time
- K against time parabolic.
Part 5 of 7Limits
Limits
Small height changes only
- Small height changes only the formula needs height change small compared with the planet's radius.
Large distances
- Large distances use U = −GMm/r instead.
System
- System the energy belongs to the object–Earth system.
Part 6 of 7Energy methods versus kinematics
Energy methods versus kinematics
Use energy
- Use energy when heights and speeds are given but not times, or the path is curved or unknown.
Use kinematics
- Use kinematics when time is asked for or acceleration is constant and known.
Pendulum released at angle θ
- Pendulum released at angle θ drop is L(1 − cosθ), so v = √(2gL(1 − cosθ)).
Projectile launched at v from height y0
- Projectile launched at v from height y0 impact speed is √(v2 + 2gy0) whatever the launch angle.
Resistive forces
- Resistive forces include friction or drag as a negative work term.
Part 7 of 7More from the specification
1Potential energy and reference frames
- Potential energy and reference frames gravitational potential energy depends on relative vertical separation, remaining consistent across uniform inertial reference frames.
2Observer
- Person or instrument measuring from within a frame.
3Driver
- The external system supplying the periodic force.
4Scalar quantity
- A quantity with magnitude only, such as potential
5Reference frame
- Coordinate system used by an observer.
6Spring constant
- Stiffness k in N/m.
7Elastic
- Returns to original shape when force is removed.
8Velocity
- Rate of change of displacement.
9Satellite
- A body that orbits a larger one; the Moon is the Earth's natural satellite.
10Stationary
- Not moving.
Key terms
| Term | Meaning |
|---|---|
| Gravitational potential energy | Energy stored by position in a gravitational field, mgΔy near a surface. |
| Reference level | Height chosen as zero potential energy. |
| Conservation of mechanical energy | K + U constant when only conservative forces do work. |
| Vertical drop | Change in height used in energy calculations. |
| System | Objects considered together, such as ball and Earth. |
Avoid these mistakes
1
Using the length along a ramp instead of the vertical height.
2
Thinking speed depends on mass in a frictionless problem.
3
Using an inconsistent zero level.
4
Using mgΔy for very large altitudes.
5
Applying energy conservation when friction does work without including its term.
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