Undergrad Euler-Lagrange Equation Q: Where Does 2mr˙r˙θ Come From?

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The discussion centers on the derivation of the term 2mr˙r˙θ in the context of the Euler-Lagrange equation for a variable-length pendulum. It is clarified that this term arises from applying the chain rule to differentiate r², resulting in 2r˙. The participants confirm that the time derivative of the Lagrangian, specifically ∂L/∂θ̇, leads to the expression mr²θ̇. Additionally, there is a consensus that dr/dt can be ignored in the Euler-Lagrange equation context. Mastery of these concepts is emphasized for future studies in physics.
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Hello Volican, :welcome:

It comes from the time derivative of ##\partial {\mathcal L}\over \partial \dot\theta## $${\partial {\mathcal L}\over \partial \dot\theta }= mr^2\dot \theta $$
 
Thanks for writting back, much appreciated. I can see where that comes from and also the -mgrsinθ but can't see how they got the 2mr˙r˙θ. Any ideas? I am thinking that I can just completley ignore the dr/dt as it is not in the euler lagrange equation? Is this wrong?
 
$$
{d\over dt} \left ( {\partial {\mathcal L}\over \partial \dot\theta } \right ) = {d\over dt} mr^2\dot \theta = m {d\over dt} \left ( r^2\right ) \dot \theta + mr^2 {d\over dt} \dot \theta = 2mr\dot r\dot\theta + mr^2\ddot\theta$$
 
Aewsome! to differentiate r^2 did you use the chain rule?
 
Yes, the chain rule is awesome :smile: $$
{d\over dt} r^2 = {d\over dt} \left ( r \right ) r + r {d\over dt} \left ( r \right ) = 2 r\dot r $$

Make sure you speak this jargon fluently when pursuing further studies !
 
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