Find the Lagrangian of an unwinding pendulum

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SUMMARY

The discussion focuses on deriving the Lagrangian for an unwinding pendulum by expressing kinetic and potential energies in terms of the angle θ and its time derivative. The initial confusion regarding the use of polar coordinates is clarified, emphasizing that Cartesian coordinates provide a simpler approach. The position of the bead is defined as x and y functions of θ, leading to a straightforward expression for the kinetic energy term. The final kinetic energy expression is confirmed as (l + aθ)²·θ̇².

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mishima
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Homework Statement
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Relevant Equations
L=T-V, ke=1/2mv^2
242045


I think my confusion on this is where the best origin for polar coordinates is. I've tried the center of the circle, and note the triangle made from the r coordinate reaching out to ##m, a,## and ##l+a\theta##. Then

$$r=\sqrt{a^2+(l+a\theta)^2}$$
$$\dot r = \frac {a(l+a\theta)} {\sqrt{a^2+(l+a\theta)^2}}$$

but my book has a much simpler expression for T where ##\dot r = 0##...I am missing some crucial insight.
 
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mishima said:
I think my confusion on this is where the best origin for polar coordinates is.
You should not be using polar coordinates. All you need to know is the kinetic and potential energies of the system expressed in terms of ##\theta## and its time derivative. You can do this by writing down the position of the bead as a function of ##\theta## in Cartesian coordinates and differentiating it to find the velocity.
 
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242165

From that I was able to get

$$x=(l+a\theta) sin\theta + a cos\theta$$
$$y=-(l+a\theta) cos\theta + a sin\theta$$

and so the ##(\dot x^2 + \dot y^2)## term in the kinetic energy was just ##(l+a\theta)^2\dot \theta^2##!

Thanks so much.
 

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