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Physics · Ch 5 — Gravitation

Connection of the Potential Energy Formula with mgh

5.7.2

Connection of the Potential Energy Formula with mgh

The formula U(r)=−GMmrU(r)=-\dfrac{GMm}{r} derived in the previous section is the EXACT expression for gravitational potential energy at any distance r from the Earth's centre. For an object resting on the Earth's surface, r=Rr=R, so U1=−GMmRU_1=-\dfrac{GMm}{R}; lifted to height h above the surface, r=R+hr=R+h, so U2=−GMmR+hU_2=-\dfrac{GMm}{R+h}. The increase in potential energy on lifting the object is therefore ΔU=U2−U1=−GMmR+h+GMmR=GMm(1R−1R+h)=GMmhR(R+h).\Delta U=U_2-U_1=-\dfrac{GMm}{R+h}+\dfrac{GMm}{R}=GMm\left(\dfrac{1}{R}-\dfrac{1}{R+h}\right)=\dfrac{GMmh}{R(R+h)}.

Using g=GMR2g=\dfrac{GM}{R^2}, i.e. GM=gR2GM=gR^2, this can be rewritten as ΔU=gR2mhR(R+h)=mgh1+h/R=mgh RR+h\Delta U=\dfrac{gR^2mh}{R(R+h)}=\dfrac{mgh}{1+h/R}=\dfrac{mgh\,R}{R+h}. Only in the SPECIAL CASE where the height h is negligibly small compared to the Earth's radius R (so that R+h≈RR+h\approx R) does this reduce to the familiar ΔU≈mgh.\Delta U\approx mgh. …