3.2.5Work, Energy, and Power
Gravitational Potential Energy Between Objects — AP PHYSICS 1 Revision Notes & Topical Questions
5 min read 9 parts Lesson 8 of 14 1 quiz
Lesson summary
3.2.5 Gravitational Potential Energy Between Objects — AP PHYSICS 1 notes: Use UG = −Gm1m2/r for two masses at any separation, including orbital and escape problems.Limit of mgΔy — it works only near a planet's surface where g is nearly constant.Far from a planet — the gravitatio…
- Resemblance to Fg
- Zero level
- Negative values
- Closer objects
- Bound system
- Sum over pairs
Section 1 of 9Why a new formula
Limit of mgΔy
- Limit of mgΔy it works only near a planet's surface where g is nearly constant.
Far from a planet
- Far from a planet the gravitational field strength is no longer constant, so a general expression is needed.
UG
−Gm1m2/r
- absolute gravitational potential energy of two approximately spherical masses.
- G = 6.67 × 10−11 N·m2/kg2.
- m1 and m2 are the masses in kg.
- r is the centre-to-centre separation in m.
Resemblance to Fg
- Resemblance to Fg the form is like Fg = Gm1m2/r2, with Fg multiplied by r for the potential energy.
Section 2 of 9Meaning of the minus sign
Zero level
- Zero level potential energy is zero at infinite separation, where the field strength tends to zero.
Negative values
- Negative values attraction means bringing masses together releases energy, so UG is always negative.
Closer objects
- Closer objects the smaller r is, the more negative UG becomes.
Bound system
- Bound system energy must be added to separate the masses to infinity.
Graph
- UG against r starts very negative and rises toward zero from below, never positive.
- The gradient magnitude at any r is Gm1m2/r2, the gravitational force.
Section 3 of 9Several objects
Several objects
Scalar
- Scalar gravitational potential energy is a scalar.
Sum over pairs
- Sum over pairs for more than two objects the total is the sum over each pair.
Central body with two satellites
- Ug,sys = Ug1 + Ug2.
Section 4 of 9Changes and conservation
Changes and conservation
Change from r1 to r2
- ΔUG = −GMm(1/r2 − 1/r1).
- Moving away (r2 > r1) gives a positive change.
Agreement near the surface
- Agreement near the surface for small Δy it reduces to mgΔy, because −GMm/(R + h) + GMm/R ≈ GMmh/R2 = mgh.
Conservation
- Conservation with only gravity doing work, ½mv12 − GMm/r1 = ½mv22 − GMm/r2.
Section 5 of 9Escape speed
Condition
- Condition the object reaches r → ∞ with speed that can be zero, so the total energy at launch is zero.
Equation
- ½mvesc2 − GMm/R = 0, so vesc = √(2GM/R).
Earth
- Earth about 11.2 km/s, independent of the object's mass and ignoring air resistance.
Total energy sign
- Total energy sign negative means bound; zero or positive means it escapes.
- (returns or orbits)
Section 6 of 9Energy in circular orbits
Kinetic energy
- GMm/r2 = mv2/r gives K = GMm/(2r).
Total energy
- E = K + UG = −GMm/(2r), negative with magnitude equal to K.
Potential energy
- UG = −GMm/r has twice the magnitude of K.
Higher orbit
- Higher orbit total energy is less negative though speed decreases, so raising an orbit needs positive work.
Changing orbits
- ΔE = (GMm/2)(1/r1 − 1/r2).
Section 7 of 9More from the specification
1Gravitational binding and reference frames
- Gravitational binding and reference frames radial distance between interacting celestial masses defines mutual gravitational potential, independent of external observer 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.
9Distance
- Total length of path travelled, a scalar.
10Stationary
- Not moving.
Section 8 of 9Key terms
| Term | Meaning |
|---|---|
| Gravitational potential energy | UG = −Gm1m2/r for two masses. |
| Bound system | System with negative total energy. |
| Escape speed | Minimum launch speed to reach infinity, √(2GM/R). |
| Infinity | Reference separation where UG = 0. |
| Total energy | K + U. |
Section 9 of 9Exam technique
1
Dropping the minus sign and treating UG as positive.
2
Using surface-to-surface distance for r.
3
Using mgΔy for large height changes.
4
Forgetting that the zero of UG is at infinity, not at the surface.
5
Thinking escape speed depends on the object's mass.
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