Max Impulse on a pendulum

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SUMMARY

The discussion focuses on analyzing the motion of a particle of mass m suspended from a string of length ℓ, which is deflected at an angle θ in a three-dimensional space. Key equations governing the system include energy conservation, expressed as E_i = E_r, and the condition that the final velocity vector must lie in the XZ-plane to avoid collision with the roof. The discussion highlights that angular momentum is not conserved due to the torque created by the weight of the particle. The primary challenge identified is the need for additional equations to solve for the unknown variables v_i and v_r.

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TL;DR Summary: An impulse is given to the pendulum so that it moves in 3 dimensions. What equations apply throughout its motion?

A particle of mass ##m## is suspended from a string of length ##\ell##. The string is then deflected at an angle ## \theta ##, where the particle and string are in the XY-plane.
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What is the maximum impulse in the Z-axis direction so that the particle does not hit the roof?
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What I already know (CMIIW):

1. Throughout its motion, the energy of the particle is conserved:
$$E_{i} = E_{r}$$
$$PE_{i} + KE_{i} = PE_{r} + KE_{r}$$
$$-m.g. \ell . \cos \theta + \frac{1}{2} . m . v_{i}^2 = 0 + \frac{1}{2} . m . v_{r}^2$$
$$v_{i}^2 = 2g. \ell . \cos \theta + v_{r}^2$$

2. The condition for a particle not to hit the roof is that its final velocity vector (when on the roof) is in the XZ-plane ##\rightarrow \left( v_r \right) _y = 0##
1.jpg


3. Angular momentum is NOT CONSERVED, because the weight creates torque (as well as linear momentum).

There are 2 unknown variables : ##v_i## and ##v_r##, while the only equation I have is energy conservation. What am I missing?
 
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This is nothing but a spherical pendulum. Angular momentum in what you have lanelef the y-direction is conserved due to rotational symmetry about the y-axis.

Also, please do not use periods as multiplication in ##\LaTeX##. Leaving the multiplication operator is fine.
 

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