H=v0sinθ0 g\mathrm{H}=\frac{\mathrm{v}_{0} \sin \theta_{0}}{\mathrm{~g}}H= gv0sinθ0
H=v02sinθ02 g\mathrm{H}=\frac{\mathrm{v}_{0}^{2} \sin \theta_{0}}{2 \mathrm{~g}}H=2 gv02sinθ0
H=v02sin2θ02 g\mathrm{H}=\frac{\mathrm{v}_{0}^{2} \sin ^{2} \theta_{0}}{2 \mathrm{~g}}H=2 gv02sin2θ0
H=v02sin2θ0 g\mathrm{H}=\frac{\mathrm{v}_{0}^{2} \sin ^{2} \theta_{0}}{\mathrm{~g}}H= gv02sin2θ0