Chapter 3: Problem 23
*Find the corresponding formulae for \(\partial e_{i} / \partial q_{j}\) for spherical polar coordinates, and hence verify the results obtained in Problem \(21 .\)
Chapter 3: Problem 23
*Find the corresponding formulae for \(\partial e_{i} / \partial q_{j}\) for spherical polar coordinates, and hence verify the results obtained in Problem \(21 .\)
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Get started for free*By comparing the Euler-Lagrange equations with the corresponding components of the equation of motion \(m \ddot{r}=-\nabla V\), show that the component of the acceleration vector in the \(q_{i}\) direction is $$ e_{i} \cdot \ddot{\boldsymbol{r}}=\frac{1}{m h_{i}}\left[\frac{\mathrm{d}}{\mathrm{d} t}\left(\frac{\partial T}{\partial \dot{q}_{i}}\right)-\frac{\partial T}{\partial q_{i}}\right] $$ Use this result to identify the components of the acceleration in cylindrical and spherical polars.
*A light rigid cylinder of radius \(2 a\) is able to rotate freely about its axis, which is horizontal. A particle of mass \(m\) is fixed to the cylinder at a distance \(a\) from the axis and is initially at rest at its lowest point. A light string is wound on the cylinder, and a steady tension \(F\) applied to it. Find the angular acceleration and angular velocity of the cylinder after it has turned through an angle \(\theta\). Show that there is a limiting tension \(F_{0}\) such that if \(F
*Parabolic co-ordinates \((\xi, \eta)\) in a plane are defined by \(\xi=r+x, \eta=\) \(r-x\). Find \(x\) and \(y\) in terms of \(\xi\) and \(\eta\). Show that the kinetic energy of a particle of mass \(m\) is $$ T=\frac{m}{8}(\xi+\eta)\left(\frac{\dot{\xi}^{2}}{\xi}+\frac{\dot{\eta}^{2}}{\eta}\right) $$ Hence find the equations of motion.
*Find the geodesics on a sphere of unit radius. [Hint: Use \(\theta\) as independent variable, and look for the path \(\varphi=\varphi(\theta)\). To perform the integration, use the substitution \(x=\cot \theta .]\)
A wedge-shaped block of mass \(M\) rests on a smooth horizontal table. A small block of mass \(m\) is placed on its upper face, which is also smooth and inclined at an angle \(\alpha\) to the horizontal. The system is released from rest. Write down the horizontal component of momentum, and the kinetic energy of the system, in terms of the velocity \(v\) of the wedge and the velocity \(u\) of the small block relative to it. Using conservation of momentum and the equation for the rate of change of kinetic energy, find the accelerations of the blocks. Given that \(M=1 \mathrm{~kg}\) and \(m=\) \(250 \mathrm{~g}\), find the angle \(\alpha\) that will maximize the acceleration of the wedge.
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