Lagrangian Mechanics: Solving for x, y, and z Dot

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Homework Help Overview

The discussion revolves around applying Lagrangian mechanics to two different systems: a bead moving along a parabolic wire and a particle on a sphere using spherical coordinates. Participants are attempting to formulate the Lagrangian and derive the equations of motion for these systems.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the formulation of the Lagrangian for a bead on a parabolic wire and express confusion regarding the kinetic energy terms and their dependence on generalized coordinates. They also explore the application of the Lagrangian method for a particle on a sphere, questioning how to derive the time derivatives of the coordinates.

Discussion Status

Some participants have provided expressions for the time derivatives of the coordinates, while others express uncertainty about the correctness of these derivatives and the complexity of the resulting equations. There is an ongoing exploration of trigonometric identities to simplify the expressions.

Contextual Notes

Participants are navigating the challenges of deriving equations of motion from the Lagrangian framework, with specific concerns about the complexity of the expressions and the application of the chain rule in their calculations.

Gogsey
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1). A bead is confined to moving on a wire in the shape of a porabola, given by y=bx^2. Write down the Lagrangian, with x as the generalized coordinate, and the equations of motion for this sytem.

We have L(x, bx^2)
For writing out the Lagrangian as a function of x, I get.:

L = m/2((xdot) + b(xdot0)^2 - mgbx^2

Then we get L = m/2((xdot^2) + 2b(xdot^2) +(b^2)(xdot^4)) - mgbx^2

But when I go to take tthe partial derivatives, everythin for the kinetic energy is in terms of xdot, and that leaves nothing for thetadot, so I'm a little confused.

2). Apply the Lagrangian method for a for a particle moving on a sphere using spherical coordinates.

so so x = rsin(theta)cos(phi), y = rsin(theta)sin(phi), z = rcos(theta)

so L = m/2(x^2 + y^2 + z^2) - U(r)

How do you get xdot, ydot, zdot? I know you just take the derivativebut with respect to what? Phi and Theta, since r is constant?
 
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the "dot" represents a time derivative; you take the derivative with respect to time and apply the chain rule
 
Yeah that's what I thought, so I get

xdot = rcos(phi)cos(theta)(thetadot) - rsin(theta)sin(phi)(phidot)

ydot = rsin(phi)cos(theta)(thetadot) + rsin(theta)cos(phi)(phidot)

zdot = -rsin(theta)(thetadot)

Then you have to square then and put them into the Lagrangian expressio, which turns out to be a hug mess? It really gets nasty. Any trig identitites I can before squaring each term?
 
Actually I think I found them.

Applying the dentities I got:

xdot = r(cos(theta + phi)(thetadot + phidot)

ydot = r(sin(theta + phi)(phidot + thetadot)

And z is the same as before.
 
Ok, so I'm not sure if those time derivatives are correct or not? Do take the derivative of the x, y and z equations with respsct to r, theta and Phi?

Trouble is, when ypu do this then you get a god awful mess, then you have to square them, and now I'm lost.

Please Help
 
Look at question no. 3 in the PDF.
 

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