For v=0.6c, find the Lorentz factor.
Answer and explanation
1.25
γ=1/sqrt(1−0.6²)=1/0.8.
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1.25
γ=1/sqrt(1−0.6²)=1/0.8.
5 s
Δt=γΔτ=5 s.
The clock present at both events
Proper time belongs to the path joining the events.
16
s²=25−9=16, a timelike separation.
Zero
Null separations have zero invariant interval.
Lorentz transformations mix time with spatial separation. For separated events, simultaneity can differ between inertial frames.
Credit spatial separation and frame transformation.
Special relativity describes inertial-frame transformations with invariant vacuum light speed. It replaces Galilean transformations when relativistic effects matter.
UniversitySpecial relativity describes inertial-frame transformations with invariant vacuum light speed. It replaces Galilean transformations when relativistic effects matter.
UniversityGeneral relativity relates spacetime geometry to stress-energy. The metric determines spacetime intervals and causal structure.
Advanced universityGeneral relativity relates spacetime geometry to stress-energy. The metric determines spacetime intervals and causal structure.
Advanced universityThe speed is subluminal; Newtonian approximations become inaccurate as β increases.
UniversityThe speed is subluminal; Newtonian approximations become inaccurate as β increases.
UniversityThe clock moves at a constant speed between the two events; proper time is measured by that clock.
UniversityThe clock moves at a constant speed between the two events; proper time is measured by that clock.
UniversityUse the (+,−) sign convention. A negative result is spacelike, not an arithmetic error.
Advanced universityUse the (+,−) sign convention. A negative result is spacelike, not an arithmetic error.
Advanced universityConnect rotation, oscillations, central forces and continuous wave models.
Work with Gauss laws, electrical field models, thermodynamic laws and electromagnetic waves.
Compare relativistic measurement with quantum states, the Schrödinger equation and uncertainty.
Use Lagrangian and Hamiltonian methods, then interpret canonical ensembles.
Explore perturbation theory, scattering, variational quantum estimates and a conceptual bridge to general relativity.