The Newtonian-limit derivation of matches (from the trace-reversed equation for dust)…

PHYSICS · Multi-part · Fermi University Physics · Relativity & Gravitation · Newtonian gravitation as a field theory · Einstein's field equations

The Geometry of Gravity, Ch The Einstein field equations and the Newtonian limit

Problem

The Newtonian-limit derivation of κ\kappa matches ∇2Φ=12κc2ρ\nabla^2\Phi = \tfrac12\kappa c^2\rho (from the trace-reversed 0000 equation for dust) to Poisson's equation ∇2Φ=4πGρm\nabla^2\Phi = 4\pi G\rho_{\rm m}, giving κ=8πG/c4\kappa=8\pi G/c^4. Suppose instead someone forgets the trace-reversal factor of 12\tfrac12 and matches ∇2Φ=κc2ρ\nabla^2\Phi = \kappa c^2\rho directly to 4πGρm4\pi G\rho_{\rm m}. ((a)) Find the resulting (wrong) constant κwrong\kappa_{\rm wrong} in SI units. ((b)) Re-derive Poisson's equation using κwrong\kappa_{\rm wrong} in place of the correct κ\kappa, and use it to predict the surface gravity of Mars, given MMars=6.42×1023 kgM_{\rm Mars}=6.42\times10^{23}\,\mathrm{kg} and RMars=3.390×106 mR_{\rm Mars}=3.390\times10^6\,\mathrm{m}. ((c)) Compare with the measured value gMars=3.71 m s−2g_{\rm Mars}=3.71\,\mathrm{m\,s^{-2}}.

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