What is the Maximum Height of a Pendulum with Given Initial Conditions?

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The discussion revolves around solving a pendulum problem using Lagrangian mechanics, specifically determining the maximum height a pendulum bob can reach when given an initial horizontal velocity. The user correctly identifies the pendulum's degree of freedom as the angle theta and formulates the Lagrangian as L = T - U, where T is kinetic energy and U is potential energy. However, they encounter difficulties with the Euler-Lagrange equation, which leads to a non-solvable differential equation. A suggestion is made to refer to another problem that may provide insights into solving the current issue. The user expresses a need for further clarification and assistance in resolving these challenges.
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I'm trying to solve this problem via Lagrangian mechanics, but I'm having trouble correctly formulating the problem, I'm hoping one of you kindly people can show me where I'm going wrong.

A pendulum bob of mass m hangs in the equilibrium position from a light, inextensible string of length l. It is given a horizontal velocity of (3gl)1/2. Find the vertical displacement of the bob when the string becomes slack.

So the bob has one degree of freedom, theta, the angle at which it hangs, and to find the height when the string goes slack we want the maximum height the bob can reach, which can be found if the maximum value of theta is calculated.

So L = T - U = (1/2)m(lθ.)2 - mgl(1-cosθ)

Is that correct so far?

If it is, then the problem I run into is that the Euler-Lagrange equation for this motion doesn't seem to be a differential I can solve, since I have θ.. +(g/l)sinθ = 0, and that doesn't seem to be solvable with the current methods I know.

Thank you for your help.
 
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Thank you for that link, I haven't had a chance to go through it in detail (it's been a hectic week), but it does look promising, I just need to figure it all out!
 
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