Solution Found!
Same as .11, but use the following system: A bead of mass
Chapter 13, Problem 13.12(choose chapter or problem)
Same as Problem 13.11, but use the following system: A bead of mass m is threaded on a frictionless, straight rod, which lies in a horizontal plane and is forced to spin with constant angular velocity \(\omega\) about a vertical axis through the midpoint of the rod. Find the Hamiltonian for the bead and show that it is not equal to T + U.
Questions & Answers
QUESTION:
Same as Problem 13.11, but use the following system: A bead of mass m is threaded on a frictionless, straight rod, which lies in a horizontal plane and is forced to spin with constant angular velocity \(\omega\) about a vertical axis through the midpoint of the rod. Find the Hamiltonian for the bead and show that it is not equal to T + U.
ANSWER:Step 1 of 3
A bead of mass m threaded on a frictionless straight rod, which lies in a horizontal plane, is forced to spin with a constant angular velocity \(\omega\) about a vertical axis, through the midpoint of the rod.
Therefore, the kinetic energy of the system is equal to the sum of the translational kinetic energy and rotational kinetic energy.
\(T=\frac{1}{2} m \dot{r^{2}}+\frac{1}{2} l \omega^{2}\)
Here \(\dot{r}\) is the velocity of rotation and r is the position of the bead along the rod.
Moment of inertia of the rod is equal to the product of mass, square of the separation between the axis of rotation and mass.
\(I=m r^{2}\)
Now, write the total kinetic energy as follows,
\(\begin{aligned}
T & =\frac{1}{2} m \dot{r^{2}}+\frac{1}{2} l \omega^{2} \\
& =\frac{1}{2} m \dot{r}^{2}+\frac{1}{2} m r^{2} \omega^{2} \\
& =\frac{1}{2} m\left(\dot{r^{2}}+r^{2} \omega^{2}\right)
\end{aligned}\)