Chapter 4: Problem 3
The semi-major axis of Jupiter's orbit is \(5.20 \mathrm{AU}\). Find its orbital period in years, and its mean (time-averaged) orbital speed. (Mean orbital speed of Earth \(\left.=29.8 \mathrm{~km} \mathrm{~s}^{-1} .\right)\)
Chapter 4: Problem 3
The semi-major axis of Jupiter's orbit is \(5.20 \mathrm{AU}\). Find its orbital period in years, and its mean (time-averaged) orbital speed. (Mean orbital speed of Earth \(\left.=29.8 \mathrm{~km} \mathrm{~s}^{-1} .\right)\)
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Get started for free*It was shown in \(\S 3.4\) that Kepler's second law of planetary motion implies that the force is central. Show that his first law - that the orbit is an ellipse with the Sun at a focus - implies the inverse square law. (Hint: By differentiating the orbit equation \(l / r=1+e \cos \theta\), and using \((3.26)\), find \(\dot{r}\) and \(\ddot{r}\) in terms of \(r\) and \(\theta\). Hence calculate the radial acceleration.)
*The potential energy of a particle of mass \(m\) is \(V(r)=k / r+c / 3 r^{3}\), where \(k<0\) and \(c\) is a small constant. (The gravitational potential energy in the equatorial plane of the Earth has approximately this form, because of its flattened shape - see Chapter 6.) Find the angular velocity \(\omega\) in a circular orbit of radius \(a\), and the angular frequency \(\omega^{\prime}\) of small radial oscillations about this circular orbit. Hence show that a nearly circular orbit is approximately an ellipse whose axes precess at an angular velocity \(\Omega \approx\left(c /|k| a^{2}\right) \omega\).
A star of mass M and radius R is moving with velocity v through a cloud of particles of density ?. If all the particles that collide with the star are trapped by it, show that the mass of the star will increase at a rate $$ \frac{\mathrm{d} M}{\mathrm{~d} t}=\pi \rho v\left(R^{2}+\frac{2 G M R}{v^{2}}\right) $$ Given that \(M=10^{31} \mathrm{~kg}\) and \(R=10^{8} \mathrm{~km}\), find how the effective crosssectional area compares with the geometric cross-section \(\pi R^{2}\) for velocities of \(1000 \mathrm{~km} \mathrm{~s}^{-1}, 100 \mathrm{~km} \mathrm{~s}^{-1}\) and \(10 \mathrm{~km} \mathrm{~s}^{-1}\).
A beam of particles strikes a wall containing \(2 \times 10^{29}\) atoms per \(\mathrm{m}^{3}\). Each atom behaves like a sphere of radius \(3 \times 10^{-15} \mathrm{~m}\). Find the thickness of wall that exactly half the particles will penetrate without scattering. What thickness would be needed to stop all but one particle in \(10^{6} ?\)
Show that Kepler's third law, \(\tau \propto a^{3 / 2}\), implies that the force on a planet is proportional to its mass. [This law was originally expressed by Kepler as \(\tau \propto \bar{r}^{3 / 2}\), where \(\bar{r}\) is a 'mean value' of \(r\). For an ellipse, the mean over angle \(\theta\) is in fact \(b\); the mean over time is actually \(a\left(1+\frac{1}{2} e^{2}\right)\); it is the mean over are length - or the median - which is given by \(a !\) Of course, for most planets in our Solar System these values are almost equal.]
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