Chapter 1: Problem 16
In Example (1.21), investigate the stability of the two additional equilibrium points in the case \(\omega^{2} \sin \alpha>g / a\).
Chapter 1: Problem 16
In Example (1.21), investigate the stability of the two additional equilibrium points in the case \(\omega^{2} \sin \alpha>g / a\).
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Get started for freeSuppose that the matrix \(H\) in \((1.5)\) is given by $$ H=\frac{1}{\sqrt{6}}\left(\begin{array}{ccc} \sqrt{2} & \sqrt{2} & \sqrt{2} \\ -2 & 1 & 1 \\ 0 & -\sqrt{3} & \sqrt{3} \end{array}\right) $$ Check that \(H^{\mathrm{t}} H=H H^{\mathrm{t}}=I\). Write down the components of \(\boldsymbol{e}_{1}\), \(e_{2}\), and \(e_{3}\) in \(\tilde{T}\), and the components of \(\tilde{e}_{1}, \tilde{e}_{2}\), and \(\tilde{e}_{3}\) in \(\mathcal{T}\).
A sphere of radius \(a\) is rolling without slipping on a rough horizontal plane in such a way that its centre traces out a horizontal circle, radius \(b\) and centre \(O\), with constant angular speed \(\Omega\). Let \((i, j, k)\) be an orthonormal triad with \(k\) vertical and \(i\) in the direction from \(O\) to the centre of the sphere. Show that the angular velocity of the sphere relative to the plane satisfies $$ \boldsymbol{\omega}=n \boldsymbol{k}-\frac{b}{a} \Omega i $$ where \(n=\boldsymbol{\omega} \cdot \boldsymbol{k}\). Show that if \(n\) is constant, then the locus of the point of contact on the sphere is a circle. What is its radius?
A plastic ball is held at the bottom of a bucket of water and then released. As it is released, the bucket is dropped over the edge of a cliff. What happens?
Establish the properties of the line \(L\) defined by \((1.41)\) for the general motion of a rigid body. That is, show that if \(P\) is a point of \(L\), then \(\boldsymbol{v}_{P}\) is proportional to \(\omega\); and show conversely that if \(v_{P}\) is proportional to \(\omega\), then \(P\) lies on \(L\). (Assume that \(\omega \neq 0\).)
\({ }^{\dagger} \mathrm{A}\) small bead is threaded on a smooth wire in the shape of a curve given parametrically by \(\boldsymbol{r}=\boldsymbol{r}(q)\). The wire rotates with constant angular velocity about a vertical axis. Show that $$ \frac{\mathrm{d}}{\mathrm{d} t}\left[\frac{1}{2} \dot{q}^{2} \frac{\mathrm{d} \boldsymbol{r}}{\mathrm{d} q} \cdot \frac{\mathrm{d} \boldsymbol{r}}{\mathrm{d} q}\right]=\dot{q} \frac{\mathrm{d} \boldsymbol{r}}{\mathrm{d} q} \cdot \ddot{\boldsymbol{r}} $$ where the dot is the time derivative relative to a frame rotating with the wire, and \(\boldsymbol{r}\) is measured from an origin on the axis Deduce that $$ \frac{\mathrm{d} \boldsymbol{r}}{\mathrm{d} q} \cdot \frac{\mathrm{d} \boldsymbol{r}}{\mathrm{d} q} \dot{q}^{2}-(\boldsymbol{\omega} \wedge \boldsymbol{r}) \cdot(\boldsymbol{\omega} \wedge \boldsymbol{r})-2 \boldsymbol{g} \cdot \boldsymbol{r}=\text { constant. } $$ Does this result still hold when the axis of rotation is not vertical?
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