Relativistic Momentum and Energy
Key idea: Use relativistic momentum p=γmv and the energy–momentum relation to solve problems for massive particles and photons, with worked examples.
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The core idea
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Learning objectives
- use the one-dimensional relativistic velocity addition formula to calculate velocities in different inertial frames or to solve problems
- Apply the relativistic energy–momentum relation E² = (pc)² + (mc²)² to solve problems, including selecting its limiting form.
- Show that E² = (pc)² + (mc²)² reduces to E = pc for massless particles and to E = mc² + ½mv² at low speeds.
At relativistic speeds, momentum and energy take forms that keep the laws of physics consistent across inertial frames. The key H3 tool is the energy–momentum relation: E² = (pc)² + (mc²)²
This is the maintained dynamics capstone before interpretation checks like the twin paradox and full-sequence confirmation.
1. Definitions (Must Know)
- Lorentz factor: γ = 1/(square root of (1-v²/c²))
- Rest mass, m (kg): invariant mass of the particle (do not use “relativistic mass”).
- Relativistic momentum (1D magnitude): p = γ mv
- Total energy: E = γ mc²
- Rest energy: E₀ = mc²
- Kinetic energy: K = E-E₀ = (γ-1)mc²
- Energy–momentum relation (H3): E² = (pc)² + (mc²)²
- Symbols used in this lesson: m (kg), v (m s⁻¹), c (≈ 3.00 × 10⁸ m s⁻¹), γ (dimensionless), p (kg m s⁻¹), E,E₀,K (J).
2. Key Ideas (What Earns Marks)
- In an isolated system, total energy and total momentum are conserved.
- The energy–momentum relation lets you solve problems without needing v explicitly.
- Required limits (H3 LO):
- massless particle (m = 0): E = pc (e.g. photon),
- low speed (v≪ c): E ≈ mc² + 1/2 mv².
Quick reference:
| Quantity | Relativistic form | Notes |
|---|---|---|
| Momentum | p = γ mv | Use m as rest mass |
| Total energy | E = γ mc² | Includes rest energy |
| Kinetic energy | K = (γ-1)mc² | Reduces to 1/2 mv² at low speed |
| Photon energy | E = pc | For m = 0 |
3. Detailed Explanations
A. Using the energy–momentum relation
If a question gives any two of (E,p,m), you can find the third from: E² = (pc)² + (mc²)²
This is especially useful for:
- high-speed particles where Newtonian K = 1/2 mv² is not valid, and
- photons (where m = 0).
B. The two required limits
Massless (m = 0): E² = (pc)² ⇒ E = pc
Low-speed (v≪ c): using the binomial approximation γ ≈ 1 + (1/2)(v²/c²), E = γ mc² ≈ mc² + 1/2 mv²
4. Common Mistakes
- Saying “protons are massless” (false). A photon is an example of a massless particle; a proton has non-zero rest mass.
- Using K = 1/2 mv² at relativistic speeds without checking v≪ c.
- Dropping the mc² term and treating total energy as just kinetic energy.
- Forgetting that conservation laws apply to an isolated system (external work/impulse breaks simple conservation statements).
5. Exam Tips
- If you see “photon” or “massless”, immediately use E = pc.
- If you see “show it reduces to…”, write the limit explicitly (m = 0 or v≪ c).
- Keep track of whether you’re asked for total energy E or kinetic energy K.
6. Worked Examples
Modelled example 1
Photon momentum from energy
Problem
Study the worked solution
Select the limit
Method
Set rest mass to zero.Reason
A photon is massless.Working
E² = (pc)² ⇒ E = pcRearrange
Method
Divide energy by c.Reason
Momentum has units J divided by m s⁻¹.Working
p = E/cCalculate
Method
Substitute c = 3.00 × 10⁸ m s⁻¹.Reason
Keep the supplied significant figures.Working
p = 1.1 × 10⁻²⁷ kg m s⁻¹
Guided practice 2
Total energy from momentum and rest mass
Problem
Try this before viewing the solution
Hints
Hint 1: calculate comparable energy terms
Hint 2: combine squares, not values
View solution step by step
Momentum term
Method
Convert p to the energy scale pc.Reason
Both terms inside the relation must have energy units.Working
pc = 1.20 × 10⁻¹⁰ JRest term
Method
Calculate rest energy.Reason
c² = 9.00 × 10¹⁶ m² s⁻².Working
mc² = 9.0 × 10⁻¹¹ JCombine
Method
Add squares and take the positive root.Reason
Total energy is positive.Working
E = square root of ((1.20 × 10⁻¹⁰)² + (9.0 × 10⁻¹¹)²) = 1.50 × 10⁻¹⁰ J
Common misconception 3
Low-speed check
Learner claim
Try this before viewing the solution
View solution step by step
Expand gamma
Method
For v≪ c, retain the leading correction.Reason
Higher powers of v/c are negligible.Working
γ ≈ 1 + (1/2)v²/c²Subtract rest contribution
Method
γ-1 removes the leading one.Reason
Kinetic energy excludes rest energy.Working
γ-1 ≈ (1/2)v²/c²Cancel factors
Method
The c² factors cancel.Reason
The classical kinetic-energy scale remains.Working
K ≈ ((1/2)v²/c²)mc² = (1/2)mv²
Examiner practice 4
Kinetic energy at 0.80c
Examination question
Try this before viewing the solution
View solution step by step
Calculate gamma
1 markMethod
At 0.80c, γ = 1.67.Reason
1/square root of (1-0.80²) = 1/0.60.Working
γ = 1.67Select energy
1 markMethod
Use K = (γ-1)mc².Reason
The question asks for kinetic, not total, energy.Working
K = (0.67)mc²Substitute
1 markMethod
Insert rest mass and c².Reason
c² = 9.00 × 10¹⁶ in SI.Working
K = (0.67)(2.0 × 10⁻²⁷)(9.00 × 10¹⁶)Calculate
1 markMethod
Give the result in joules.Reason
Two significant figures suit the data.Working
K = 1.2 × 10⁻¹⁰ J
Self-mark with the mark scheme
Compare your response with each mark point. Select a point only when your response contains that evidence.
Self-mark gamma, energy selection, substitution and result.
Challenge 5
When kinetic energy equals rest energy
Independent transfer
Try this before viewing the solution
Hints
Hint 1: cancel the common rest-energy scale
View solution step by step
Find gamma
Method
Cancel mc² from the non-zero-mass equation.Reason
The energy equality fixes a dimensionless factor.Working
γ-1 = 1 ⇒ γ = 2Invert gamma
Method
Square the reciprocal relation.Reason
This isolates the squared speed ratio.Working
1-v²/c² = 1/4Calculate speed
Method
Take the positive speed magnitude.Reason
The result must be below c.Working
v/c = square root of (3/4) = 0.866
7. Mind Stretchers
Mind stretcher 1: Why use E² = (pc)² + (mc²)² at all?Extension
Why is the energy–momentum relation often easier than working with v directly?
Answer
Because v can be hard to find from partial information, and many problems give p, E, or m directly. The relation links them algebraically and works cleanly for both massive and massless particles.
Mind stretcher 2: Why momentum must change from p = mvExtension
Why isn’t it enough to keep Newtonian momentum p = mv and just “add” relativistic energy corrections?
Answer
Because momentum conservation must hold consistently across inertial frames at high speeds, and the Newtonian p = mv does not transform correctly under Lorentz transformations. The relativistic momentum p = γ mv is needed so that conservation laws and collision outcomes remain consistent between frames.
8. Optional/Enrichment: Useful Unit Conversions
- Electronvolt: 1 eV = 1.602 × 10⁻¹⁹ J (energy gained by charge e across 1 V).
- Atomic mass unit: 1 u = 1.66 × 10⁻²⁷ kg.
Next in the maintained sequence: The Twin Paradox.
Continue with the next resource in this course.
Course and syllabus information
- Course
- GCE A-Level H3 Physics
- Edition
- GCE A-Level H3 Physics 2027