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Energy in terms of momentum: E=mc21+(p/mc)2E = mc^2\sqrt{1 + (p/mc)^2}E=mc21+(p/mc)2​

Proved
EnergyMomentum.energy_eq_sqrt_momentum

by Lucas · Oct 9, 2026 · Mathlib 0df444a (Lean v4.33.1)

mathematical-physicsspecial-relativity

Let c>0c > 0c>0, m>0m > 0m>0 and v∈R3\mathbf v\in\mathbb R^3v∈R3 with ∣v∣<c|\mathbf v| < c∣v∣<c. The total energy E=γmc2E = \gamma mc^2E=γmc2 and the momentum magnitude p=∣γmv∣p = |\gamma m \mathbf v|p=∣γmv∣ satisfy

E=mc21+(pmc)2.E = mc^2\sqrt{1 + \left(\frac{p}{mc}\right)^2}.E=mc21+(mcp​)2​.

Squaring both sides and rearranging yields the energy–momentum relation (1).

Preamble
import Mathlib
import Definitions.Def_EnergyMomentum_basic
Formal statement
namespace EnergyMomentum

/-- Energy in terms of three-momentum: `E = m c² √(1 + (p / (m c))²)`. -/
theorem energy_eq_sqrt_momentum (m c : ℝ) (v : Vec3)
    (hc : 0 < c) (hm : 0 < m) (hv : ‖v‖ < c) :
    energy m c v = m * c ^ 2 * Real.sqrt (1 + (‖momentum m c v‖ / (m * c)) ^ 2) := by sorry

end EnergyMomentum
Source
Wikipedia, *Energy–momentum relation*, https://en.wikipedia.org/wiki/Energy%E2%80%93momentum_relation (PDF snapshot supplied by the proposer), §Origins and derivation of the equation → Heuristic approach for massive particles; also §Classical correspondence (first display).
Read-back

What the Lean code literally says, in plain math · Aristotle (Harmonic) — same agent as the drafter; non-blind

Disclosure — this is NOT a blind read-back. It was written by the same agent (Aristotle, by Harmonic) that drafted this Lean statement, with full knowledge of the source material and of the intended meaning. It is not independent testimony and must not be mistaken for an independent audit; reviewers should check it against the Lean code themselves (or replace it with a blind read-back).

For all real m,cm, cm,c and v∈R3\mathbf v\in\mathbb R^3v∈R3 with 0<c0 < c0<c, 0<m0 < m0<m, ∣v∣<c|\mathbf v| < c∣v∣<c:

energy(m,c,v)=mc21+(∣momentum(m,c,v)∣mc)2,\mathrm{energy}(m,c,\mathbf v) = m c^2 \sqrt{1 + \left(\frac{|\mathrm{momentum}(m,c,\mathbf v)|}{m c}\right)^2},energy(m,c,v)=mc21+(mc∣momentum(m,c,v)∣​)2​,

where energy(m,c,v)=γmc2\mathrm{energy}(m,c,\mathbf v) = \gamma m c^2energy(m,c,v)=γmc2, momentum(m,c,v)=γmv\mathrm{momentum}(m,c,\mathbf v) = \gamma m \mathbf vmomentum(m,c,v)=γmv, γ=1/1−(∣v∣/c)2\gamma = 1/\sqrt{1-(|\mathbf v|/c)^2}γ=1/1−(∣v∣/c)2​. No junk values occur under the hypotheses.

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