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 \(\omega^{2} \sin \alpha>g / a\).
All the tools & learning materials you need for study success - in one app.
Get started for freeTwo frames \(R\) and \(\tilde{R}\) are moving relative to each other without rotation. A particle has kinetic energy \(T\) measured in \(R\) and \(\tilde{T}\) measured in \(\widetilde{R}\). Show that $$ T=\tilde{T}+\boldsymbol{u} \cdot \boldsymbol{p}+c $$ where \(\boldsymbol{p}=m \boldsymbol{v}\) is the momentum of the particle measure in \(R, \boldsymbol{u}\) is the velocity of \(\tilde{R}\) relative to \(R\), and \(c\) is a constant.
Suppose 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 \(\mathcal{T}\).
Show that if \(H\) is an orthogonal matrix, then \(H^{t}(H-I)=(I-H)^{t}\). Deduce that if \(H\) is also proper, then \(\operatorname{det}(I-H)=0\). Hence show that if \(\mathcal{T}\) and \(\tilde{T}\) are two (right-handed) orthonormal triads, then there exists a nonzero vector that has the same components in both triads.
\({ }^{\dagger}\) A rigid body has angular velocity \(\boldsymbol{\omega}\) and has one point \(O\) fixed relative to a frame \(\tilde{R}\). Show that if \(\boldsymbol{\omega} \wedge \tilde{D} \boldsymbol{\omega} \neq 0\), then \(O\) is the only point with zero acceleration relative to \(\tilde{R}\).
Count the number of degrees of freedom in each of the following systems. (a) A small bead sliding on a wire. (b) A lamina moving in its own plane. (c) A double pendulum confined to a vertical plane. This consists of a point mass \(A\) suspended from a fixed point by a thin rod; and a second point mass \(B\) suspended from \(A\) by a second thin rod. The rods are hinged at \(A\). (d) A double pendulum which is not confined to a vertical plane.
What do you think about this solution?
We value your feedback to improve our textbook solutions.