What is the Lagrangian and equation of motion for a bead on a rotating coil?

In summary: In the non-rotating frame, the z equation of motion would be the same regardless of the coordinate system I used.
  • #1
nhalford
2
0

Homework Statement


A bead of mass [itex]m[/itex] is threaded around a smooth spiral wire and slides downwards without friction due to gravity. The [itex]z[/itex]-axis points upwards vertically. Suppose the spiral wire is rotated about the [itex]z[/itex]-axis with a fixed angular velocity [itex]\Omega[/itex]. Determine the Lagrangian and the equation of motion.

Homework Equations


[tex]L = T - V[/tex]
[tex]\frac{\partial L}{\partial x} = \frac{d}{dt}\left(\frac{\partial L}{\partial \dot{x}}\right)[/tex]

The Attempt at a Solution


This is related to a previous problem in which the wire is not rotating and its shape is given as [tex]z = k\psi, \hspace{3mm} x = a\cos\psi, \hspace{3mm} y = a\sin\psi[/tex] where [itex]a[/itex] and [itex]k[/itex] are both positive. For that problem, the resulting equation of motion is [itex]\ddot{\psi} = -\frac{gk}{a^2 + k^2}[/itex]

We still have [itex]z = k\psi[/itex], but now [itex]x = a\cos(\psi + \Omega t)[/itex] and [itex]y = a\sin(\psi + \Omega t)[/itex]. This gives [itex]\dot{z} = k\dot{\psi}[/itex], [itex]\dot{x} = -a(\dot{\psi} + \Omega)\sin(\psi + \Omega t)[/itex] and [itex]\dot{y} = a(\dot{\psi} + \Omega)\cos(\psi + \Omega t)[/itex]. Then the kinetic energy is
[tex]
T = \frac{1}{2}m\left(\dot{x}^2 + \dot{y}^2 + \dot{z}^2\right) = \frac{1}{2}m\left(a^2\left(\dot{\psi}^2 + 2\dot{\psi}\Omega + \Omega^2\right) + k^2\dot{\psi}^2\right)
[/tex]
and the potential energy is [itex]V = mgz = mgk\psi[/itex]. Then the Lagrangian becomes:
[tex]
L = T - V = \frac{1}{2}m\left(a^2\left(\dot{\psi}^2 + 2\dot{\psi}\Omega + \Omega^2\right) + k^2\dot{\psi}^2\right) - mgk\psi.
[/tex]
This gives
[tex]
\frac{\partial L}{\partial \psi} = -mgk, \hspace{3mm} \frac{\partial L}{\partial \dot{\psi}} = m\left(a^2\dot{\psi} + a^2\Omega + k^2\dot{\psi}\right), \hspace{3mm} \frac{d}{dt}\left(\frac{\partial L}{\partial \dot{\psi}}\right) = m\left(a^2 + k^2\right)\ddot{\psi}
[/tex]
so plugging into Lagrange's Equation gives [itex]-mgk = m\left(a^2 + k^2\right)\ddot{\psi}[/itex] or [itex]\ddot{\psi} = -\frac{gk}{a^2 + k^2}[/itex], which is the exact same equation of motion as in the case with the coil not rotating. Obviously this isn't correct. Where am I going wrong here? My instinct is that there might be a problem with my choice of coordinates; in particular, [itex]\psi[/itex] is rotating, but I'm not sure if there is a better choice of coordinates.
 
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  • #2
Hello nhalford. Welcome to PF!

Why do you say your result is incorrect?

Suppose you went to the rotating frame. Then in this frame the wire would not be rotating but you would have centrifugal and Coriolis fictitious forces. Consider the directions of these fictitious forces and decide whether or not they would have any effect on the z equation of motion (or equivalently the ##\psi## equation of motion, since z and ##\psi## are proportional).
 
  • #3
Ah, you're right, thanks. It just seemed counterintuitive to me.
 

FAQ: What is the Lagrangian and equation of motion for a bead on a rotating coil?

1. What is a "Bead on a rotating coil" experiment?

The "Bead on a rotating coil" experiment is a common demonstration used in physics to show the effects of electromagnetic induction. It involves a conducting bead placed on a rotating coil connected to a power source. The rotation of the coil induces a current in the bead, causing it to move or levitate.

2. How does the "Bead on a rotating coil" experiment work?

The experiment works by utilizing the principles of electromagnetic induction. When the coil is rotated, it creates a changing magnetic field. This changing magnetic field induces a current in the conducting bead, which creates its own magnetic field. The interaction between the two magnetic fields causes the bead to move or levitate.

3. What factors affect the movement of the bead in the "Bead on a rotating coil" experiment?

The movement of the bead in the experiment can be affected by various factors such as the speed of rotation, the strength of the magnetic field, the conductivity of the bead, and the distance between the bead and the coil. These factors can be adjusted to control the motion of the bead and demonstrate different aspects of electromagnetic induction.

4. What is the significance of the "Bead on a rotating coil" experiment?

The "Bead on a rotating coil" experiment is significant because it helps to illustrate the principles of electromagnetic induction and its applications in various technologies such as generators, motors, and transformers. It also demonstrates the relationship between electricity and magnetism, which is a fundamental concept in physics.

5. Can the "Bead on a rotating coil" experiment be used for practical applications?

While the experiment itself may not have practical applications, the principles and concepts demonstrated in the "Bead on a rotating coil" experiment have numerous practical uses. For example, electromagnetic induction is used in power generation, electric motors, and wireless charging technologies. This experiment helps to understand and visualize these applications in a simple and tangible way.

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