If the moment of inertia of a body of mass \(m\) about an axis which passes through the centre of mass is \(mk^2\), show that the moment of inertia about a parallel axis a distance \(l\) from the first is \(m(k^2+l^2)\). A thin uniform rod of mass \(m\) is attached to a smooth hinge at one end. The rod falls from rest in the horizontal position. If the maximum strain which the hinge can take in any direction is \(mg\), show that the hinge will snap when the rod makes an angle \(\sin^{-1} \left(\frac{2\sqrt{3}}{3}\right)\) with the vertical. Describe, without explicit calculation, the motion of the rod after the hinge has broken.
A two-stage rocket carries a payload of mass \(m\). Each stage has mass \(M\) including fuel of mass \(\lambda M\), where \(0 < \lambda < 1\). When the fuel is ignited, it burns at a constant rate \(k\), and exhaust gases are ejected at constant speed \(w\) relative to the rocket. Justify carefully the following equation of motion, which ignores gravity, during the burning of the first stage: \begin{equation*} (2M + m - kt)\frac{dv}{dt} = wk, \end{equation*} where \(v\) is the speed of the rocket. If the first stage drops off when it is burnt out, and the second stage then ignites, find the velocity of the rocket when both stages are fully burnt. Find also the corresponding velocity for a single stage rocket, with the same properties \(k, w\), which has mass \(2M\) (including fuel of mass \(2\lambda M\)) and carries a payload of mass \(m\).
A uniform solid cylinder is projected up a rough plane with speed \(v\) in such a way that it has initially no rotation. The plane is inclined at an angle \(\alpha\) to the horizontal, and the coefficient of friction is \(\frac{1}{3}\tan\alpha\). Show that the frictional force acts down the plane for all times \(t\) less than \(t_1 = 2V\textrm{cosec}\alpha/3g\). Show also that at this time \(t_1\) a pure rolling motion cannot commence, and that at all later times the frictional force acts up the plane.
A particle of unit mass moves under the action of a force which is given in polar coordinates \((r, \theta)\) by \begin{equation*} -\frac{4q\cos\theta}{r^3}\hat{\mathbf{r}} - \frac{2q\sin\theta}{r^3}\hat{\boldsymbol{\theta}}, \end{equation*} where \(\hat{\mathbf{r}}, \hat{\boldsymbol{\theta}}\) are unit vectors defined in the usual way. The \(r\)-axis is taken to be \(\theta = 0\), and \(q\) is a positive constant. The particle is projected from \(r = a, \theta = 0\), perpendicularly to the \(r\)-axis, with velocity \((8q/a^2)^{\frac{1}{2}}\). Show that in the subsequent motion, \begin{equation*} \left(\frac{dr}{d\theta}\right)^2 = \frac{(r^2-a^2)r^2}{a^2(1+\cos\theta)}. \end{equation*} By using the substitution \(r = a\sec\lambda\), or otherwise, find and sketch the path of the particle.
The Cartesian components of a force which acts on a given particle of unit mass are \((E\cos\alpha t + \dot{y}B, E\sin\alpha t - \dot{x}B)\), where \((x, y)\) is the position of the particle relative to the origin \(O\). \(E\) and \(B\) are positive constants and a dot denotes differentiation with respect to time. The particle is at rest at \(O\) at time \(t = 0\). By introducing the variable \(\omega = x + iy\), or otherwise, find the position of the particle at all future times for any positive value of \(\alpha\). By examination of the solution for small values of \(\alpha\), or otherwise, describe the motion of the particle if \(\alpha = 0\).
Explain briefly the use of the method of complex impedances for solving problems in a.c. electrical networks. What is the relation of the method to that of partial fractions, integral and complementary function in the solution of ordinary differential equations? Find the conditions under which the bridge circuit shown below is in balance (i.e. no current flows through the meter), if the generator has angular frequency \(\omega\).