gλ=GMR2−ω2Rcos2λ\mathrm{g}_{\lambda}=\dfrac{\mathrm{GM}}{\mathrm{R}^{2}}-\omega^{2} \mathrm{R} \cos ^{2} \lambdagλ=R2GM−ω2Rcos2λ
gλ=GMR2−ω2Rcosλ\mathrm{g}_{\lambda}=\dfrac{\mathrm{GM}}{\mathrm{R}^{2}}-\omega^{2} \mathrm{R} \cos \lambdagλ=R2GM−ω2Rcosλ
gλ=GMR2−ωRcos2λ\rm{g_{\lambda}=\dfrac{G M}{R^{2}}-\omega R \cos ^{2} \lambda}gλ=R2GM−ωRcos2λ
gλ=GMR2−ωRcosλ\rm{g_{\lambda}=\dfrac{\mathrm{GM}}{\mathrm{R}^{2}}-\omega R \cos \lambda}gλ=R2GM−ωRcosλ