What is the Hamiltonian for a bead on a rotating rod with fixed z and R?

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For example, if we took z to be a generalized coordinate, then the constraint equation would be \dot{z}=0, which is time dependent. Therefore, the Hamiltonian is not equal to T+U.In summary, the problem is describing a situation where a bead is threaded onto a rod and forced to spin with constant angular velocity about a fixed vertical axis. The Hamiltonian for this system is found to not equal T+U due to a missing term in the kinetic energy equation and the time dependence of the constraint equation. This shows that not all forms of generalized coordinates work for non-inertial frames.
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gluon1988
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Homework Statement



A bead of mass, [tex]m[/tex] is threaded on a frictionless, straight rod, which lies in the horizontal plane and is forced to spin with constant angular velocity, [tex]\omega[/tex], about a fixed vertical axis through the midpoint of the rod. Find the Hamiltonian for the bead and show that it does not equal [tex]T+U[/tex]

Homework Equations



[tex]\mathcal{L}=T-U[/tex]

[tex]\frac{d}{dt}\frac{\partial\mathcal{L}}{\partial\dot{q}}=\frac{\partial\mathcal{L}}{\partial{q}}[/tex]

[tex]p=\frac{\partial\mathcal{L}}{\partial\dot{q}}[/tex]

[tex]\mathcal{H}=\sum p_{i}\dot{q}_{i}-\mathcal{L}[/tex]

The Attempt at a Solution



The bead is threaded onto the road, so the radius is fixed. So is the z-axis. The only degree of freedom for the bead is [tex]\phi[/tex], the angle it is located at in reference to a starting point.

[tex]\mathcal{L}=\frac{1}{2}m(\dot{\phi} R)^{2}-U(\phi)[/tex]

[tex]p=\frac{\partial\mathcal{L}}{\partial\dot{\phi}}=m{R^2}{\dot{\phi}}[/tex]

[tex]\mathcal{H}=m{R^2}{{\dot{\phi}}^2}-\frac{1}{2}m(\dot{\phi} R)^{2}-U(\phi)=\frac{1}{2}m(\dot{\phi} R)^{2}+U(\phi)\rightarrow\mathcal{H}=T+U[/tex]??

I'm assuming I am getting the kinetic energy wrong but I really don't see what it could be with z and R fixed. Please help
 
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  • #2
Huh, I don't see any physical reason why H≠T+U. The two conditions seem to be met: the system is conservative (potential energy is velocity independent), and the equations of transformation connecting the rectangular and generalized coordinates are independent of time.

While it doesn't change the two points I listed above, why are you saying that z does not change? Seems to me like z is able to change.
 
  • #3
Mindscrape said:
Huh, I don't see any physical reason why H≠T+U. The two conditions seem to be met: the system is conservative (potential energy is velocity independent), and the equations of transformation connecting the rectangular and generalized coordinates are independent of time.

While it doesn't change the two points I listed above, why are you saying that z does not change? Seems to me like z is able to change.

The problem just stated that H≠T+U. I think they were trying to show that not every form of general coordinates will work for non-inertial frames. Regardless, I was missing a term of [tex]{{\omega}^2}{sin}^{2}(\phi){\phi}^2[/tex] in the kinetic energy term, which does in fact lead to H≠T+U.

The problem was listed on the easier section of the text, so I assumed they weren't going to vary z, which they didn't thankfully.

Thanks for the reply
 
  • #4
Oh, I see now what the problem was describing. It's written in the usual cryptic, non-explicit description that classical mechanics problems tend to have.

The equations of transformation connecting the rectangular and generalized coordinates are not independent of time after all.
 
  • #5
!



Your attempt at the solution is correct. The Hamiltonian for this system is indeed equal to the sum of the kinetic and potential energies, i.e. \mathcal{H}=T+U. The mistake you made is in your calculation of the kinetic energy. The correct expression for the kinetic energy of a bead on a rotating rod is given by T=\frac{1}{2}m(\dot{\phi} R)^{2}, as you have correctly written in your Lagrangian. This can be derived by considering the rotational motion of the bead and using the parallel axis theorem to account for the fixed radius of the rod. Therefore, your final expression for the Hamiltonian is correct and does not need to be modified.
 

FAQ: What is the Hamiltonian for a bead on a rotating rod with fixed z and R?

What is an Easy Hamiltonian problem?

An Easy Hamiltonian problem is a type of mathematical problem that involves finding a cycle in a graph that visits every vertex exactly once and returns to the starting vertex. It is named after the mathematician William Rowan Hamilton who first studied this type of problem in the 19th century.

How is an Easy Hamiltonian problem different from a regular Hamiltonian problem?

An Easy Hamiltonian problem is a special case of a Hamiltonian problem in which the graph is a complete graph, meaning that every vertex is connected to every other vertex. In a regular Hamiltonian problem, the graph can be any type of graph and the goal is to find a cycle that visits every vertex exactly once.

What are some applications of Easy Hamiltonian problems?

Easy Hamiltonian problems have practical applications in various fields, such as computer science, physics, and chemistry. They can be used to model and solve real-world problems, such as finding the most efficient route for a traveling salesman or designing a circuit for an electronic device.

What are some techniques for solving Easy Hamiltonian problems?

There are several techniques for solving Easy Hamiltonian problems, including brute force algorithms, backtracking algorithms, and dynamic programming. These techniques involve systematically searching for a cycle in the graph that satisfies the conditions of the problem.

Are there any known solutions for all Easy Hamiltonian problems?

No, there is no known general solution for all Easy Hamiltonian problems. However, for certain special cases of Easy Hamiltonian problems, such as the Knight's tour problem, there are known solutions that can be applied. In general, finding a solution to an Easy Hamiltonian problem requires careful problem-solving and may involve using a combination of techniques.

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