Playground
Right-triangle visualization of E^2 = (pc)^2 + (mc^2)^2. Adjust beta to see pc and E grow while mc^2 stays fixed.
Variables
| Symbol | Name | SI | Dimension | Range |
|---|---|---|---|---|
| Total Energyoutput Total relativistic energy of the particle | J | ML^2T^-2 | 0 – 1e-9 | |
| Momentum Relativistic momentum magnitude | kg·m/s | MLT^-1 | 0 – 1e-18 | |
| Rest Mass Invariant rest mass | kg | M | 0 – 1e-25 |
Deep dive
Derivation
From four-momentum P^μ = (E/c, p_x, p_y, p_z), the invariant P^μ P_μ = (E/c)^2 - p^2 must equal (mc)^2 in every frame. Multiplying by c^2 gives E^2 - (pc)^2 = (mc^2)^2.
Experimental verification
Verified daily in colliders: invariant mass reconstruction at the LHC (Higgs discovery) depends on this relation.
Common misconceptions
- Total energy is not simply (1/2)mv^2 + mc^2 — only a low-speed expansion
- Even a particle at rest has energy mc^2
- Massless particles have energy and momentum, but no rest frame
Real-world applications
- Invariant mass reconstruction at colliders
- Photon–matter pair production thresholds
- Compton scattering kinematics
- Nuclear mass defects
Worked examples
Electron at 1 MeV momentum
Given:
- p:
- 5.344e-22
- m:
- 9.1093837015e-31
Find: E
Solution
pc = 1 MeV, mc^2 = 0.511 MeV → E = sqrt(1 + 0.511^2) ≈ 1.123 MeV.
Photon at 500 nm
Given:
- p:
- 1.325e-27
- m:
- 0
Find: E
Solution
E = pc = 3.97e-19 J ≈ 2.48 eV.
Scenarios
What if…
- scenario:
- What if p = mc?
- answer:
- E = sqrt(2)·mc^2 ≈ 1.414 mc^2; the particle's kinetic energy equals 0.414 mc^2.
- scenario:
- What if m is complex (tachyons)?
- answer:
- E^2 - (pc)^2 < 0 — hypothetical tachyons with spacelike four-momenta; none observed.
- scenario:
- What if we use natural units c = 1?
- answer:
- E^2 = p^2 + m^2 — the cleanest form, used throughout high-energy physics.
Limiting cases
- condition:
- p → 0
- result:
- E → mc^2
- explanation:
- Pure rest energy — Einstein's famous equation.
- condition:
- m → 0
- result:
- E = pc
- explanation:
- Photons and other massless particles.
- condition:
- pc >> mc^2
- result:
- E ≈ pc
- explanation:
- Ultra-relativistic limit dominated by momentum.
Context
Albert Einstein / Paul Dirac · 1905
Einstein's 1905 relativity paper implied this relation; Dirac used it as the mass-shell constraint for relativistic quantum mechanics.
Hook
What is the total energy of a proton with 1 GeV/c of momentum?
Using E^2 = (pc)^2 + (mc^2)^2 with pc = 1 GeV and m_p c^2 ≈ 0.938 GeV, compute E ≈ 1.37 GeV.
Dimensions:
- lhs:
- E^2 → [M^2 L^4 T^-4]
- rhs:
- (pc)^2 + (mc^2)^2 → [M^2 L^4 T^-4]
- check:
- Both sides energy². ✓
Validity: Universally valid for any free particle in special relativity, including massless particles.