On a fictional planet, the gravitational force on a satellite is
\(F(r)=\frac{k}{r^2}\), where \(r\) is measured in meters and
\(k=2.4\times10^{13}\,\text{N}\cdot\text{m}^2\).
The planet's radius is \(R=4000\,\text{km}\).
a) Find the work \(W=\int_R^{r_2}F(r)\,dr\) required to move the satellite to \(r_2=12{,}000\,\text{km}\). Give the result in megajoules.
b) Evaluate \(\int_R^\infty F(r)\,dr\) and interpret the result.
Hints
- Convert all distances to meters.
- Integrate the inverse-square function.
- Interpret an infinite upper limit as moving arbitrarily far away.
Solution
1. Convert distances:
\(R=4\times10^6\,\text{m}\) and \(r_2=12\times10^6\,\text{m}\).
2. Since an antiderivative is \(-\frac{k}{r}\),
\(W=k\left(\frac{1}{R}-\frac{1}{r_2}\right)
=4\times10^6\,\text{J}=4\,\text{MJ}\).
3. For an infinite final distance,
\(\int_R^\infty\frac{k}{r^2}\,dr
=\frac{k}{R}
=6\times10^6\,\text{J}
=6\,\text{MJ}\).
4. This is the idealized work required to move the satellite infinitely far from the planet.
Answer
a) \(W=4\,\text{MJ}\)
b) \(6\,\text{MJ}\); this is the idealized escape work to move the satellite infinitely far away.