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Physics · Ch 5 — Gravitation

Expression for Gravitational Potential Energy

5.7.1

Expression for Gravitational Potential Energy

To find an explicit formula for gravitational potential energy, consider the work done AGAINST the Earth's gravitational force F⃗g\vec{F}_g while displacing an object through a small displacement dr⃗d\vec{r}; this work appears as an increase dU=−F⃗g⋅dr⃗dU=-\vec{F}_g\cdot d\vec{r} in the potential energy of the Earth-object system (the negative sign appears because dU is the work done by US, the external agent, working AGAINST the gravitational force). For a displacement from an initial position rir_i to a final position rfr_f, the total change in potential energy is obtained by integrating: ΔU=∫rirfdU=−∫rirfF⃗g⋅dr⃗.\Delta U=\int_{r_i}^{r_f}dU=-\int_{r_i}^{r_f}\vec{F}_g\cdot d\vec{r}.

The Earth's gravitational force on an object of mass m at distance r is F⃗g=−GMmr2r^\vec{F}_g=-\dfrac{GMm}{r^2}\hat{r} (the negative sign here shows the force points OPPOSITE to r^\hat{r}, i.e. towards the Earth's centre, while r^\hat{r} itself points outward from the centre to the object). Since the displacement dr⃗d\vec{r} is along r^\hat{r} for this radial problem, F⃗g⋅dr⃗=−GMmr2dr\vec{F}_g\cdot d\vec{r}=-\dfrac{GMm}{r^2}dr, and substituting: ΔU=−∫rirf(−GMmr2)dr=GMm∫rirfdrr2=GMm[−1r]rirf=GMm(1ri−1rf).\Delta U=-\int_{r_i}^{r_f}\left(-\dfrac{GMm}{r^2}\right)dr=GMm\int_{r_i}^{r_f}\dfrac{dr}{r^2}=GMm\left[-\dfrac{1}{r}\right]_{r_i}^{r_f}=GMm\left(\dfrac{1}{r_i}-\dfrac{1}{r_f}\right). …

Misc Ex.8Example 5.8: Change in potential energy raising a body from height $R_E$ to $5R_E/2$ above the surface

Worked out. A body of mass m is raised from height RER_E above the Earth's surface (distance 2RE2R_E from the centre) to height 5RE/25R_E/2 above the surface (distance 7RE/27R_E/2 from the centre). Using ΔU=GMEm(1ri−1rf)=GMEm(12RE−27RE)\Delta U=GM_Em\left(\frac{1}{r_i}-\frac{1}{r_f}\right)=GM_Em\left(\frac{1}{2R_E}-\frac{2}{7R_E}\right), combining the fractions over a common denominator of 14RE14R_E gives ΔU=GMEm(7−414RE)=3GMEm14RE\Delta U=GM_Em\left(\frac{7-4}{14R_E}\right)=\frac{3GM_Em}{14R_E}, i.e. an increase in potential energy of 314GMEmRE\frac{3}{14}\frac{GM_Em}{R_E}. …