Problems

A bell of mass \(M\) is in the form of a hollow right circular cone of height \(h\) and semivertical angle \(\alpha\), and is made of thin uniform material. It is mounted on a light spindle passing through the vertex and perpendicular to the axis of the cone. Calculate its moment of inertia about the spindle.

A kite of mass \(m\) possesses an axis of symmetry on which lie the mass centre \(G\) and the point of attachment, \(P\), of the light string by which it is held. The string, \(PG\), may be assumed to lie in a fixed vertical plane, in which a horizontal wind blows with speed \(v\). The string makes an angle \(\theta\), and the kite an angle \(\phi\), with the horizontal in the senses shown. It is known that the force exerted by the wind on the kite has a magnitude \(F\) passing through a fixed point \(Q\) on \(PG\) (\(PQ = a\), \(QG = b\)), normal to the kite, where \(F = Cv\sin\phi\), \(C\) being a constant. Show that the kite adopts an equilibrium position described by \begin{equation*} \tan\phi = \frac{mg}{Cv}\left(1+\frac{b}{a}\right). \end{equation*} The string has fixed length \(l\) and is attached to the ground, and the wind speed at height \(h\) is given by \(v = \beta h\). Neglecting the variation of wind speed over the kite, show that it flies at a height governed by \begin{equation*} \tan\theta = \frac{\lambda ab}{(a+b)^2}\sin\theta-\frac{1}{\lambda\sin\theta}, \end{equation*} where \(\lambda = C\beta l/mg\). Show graphically that, for sufficiently large \(\lambda\), this equation has two roots in \(0 < \theta < \frac{\pi}{2}\).

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A circular hoop of radius \(a\) rolls without slipping, in a vertical plane, with angular velocity \(\omega\) along a rough horizontal table in a direction perpendicular to the edge. Prove that when it reaches the edge the centre of the hoop will fall through a vertical distance \(a(g-a\omega^2)/2g\) before the hoop leaves the edge, provided that \(a\omega^2 < g\). What happens if \(a\omega^2 \geq g\)?

A four-wheeled truck runs forward freely on level ground. The distance between the front and rear axles is \(D\), and the centre of gravity of the truck is at a distance \(\beta\) from the vertical plane through the front axle and at a height \(H\) above the ground. The moments of inertia of wheels and axles are negligible. Find the deceleration of the truck if the rear wheels become locked (the front wheels remaining free), and \(\mu\) is the coefficient of friction between the wheels and the ground. If the front rather than the rear wheels become locked show that the rear wheels remain on the ground provided that \(\mu < \beta/H\).

Six wires are connected to form the edges of a tetrahedron \(ABCD\). The resistances of opposite edges are equal. The resistance of \(AB\) is \(R_1\), that of \(AC\) is \(R_2\) and that of \(AD\) is \(R_3\). Show that if a current enters the network at \(A\) and leaves at \(D\) the total resistance of the circuit is \begin{equation*} \frac{(R_1R_2 + 2R_1R_3 + R_2R_3)R_3}{2(R_1 + R_3)(R_2 + R_3)}. \end{equation*}

Define the vector product of two vectors \(\mathbf{x}\) and \(\mathbf{y}\). Let \(\mathbf{u}\) be a vector of unit length in 3-dimensional space and let \(\mathbf{s}\) be a vector perpendicular to \(\mathbf{u}\); \(\mathbf{s}'\) is the vector obtained by rotating \(\mathbf{s}\) through an angle \(\theta\) about \(\mathbf{u}\). Show that, with a suitable sign convention for \(\theta\), \begin{equation*} \mathbf{s}' = \cos\theta\mathbf{s} + \sin\theta(\mathbf{u} \times \mathbf{s}). \end{equation*} Now let \(\mathbf{r}\) be any vector, and let \(\mathbf{r}'\) be the vector obtained by rotating \(\mathbf{r}\) through an angle \(\theta\) about \(\mathbf{u}\). Deduce a formula for \(\mathbf{r}'\) in terms of \(\mathbf{r}, \mathbf{u}\) and \(\theta\).