What is the relationship between torque and angular momentum in a rigid body?

AI Thread Summary
The discussion centers on the relationship between torque and angular momentum in rigid bodies, emphasizing the equations that define this relationship. It highlights that external torque is equal to the rate of change of angular momentum, both for stationary and accelerating points. The equations presented show how angular momentum can be expressed relative to different points, including the center of mass and any accelerating point. A specific query is raised regarding the equation for external torque at an accelerating point and its components. Clarification on the variables involved is requested to facilitate better understanding and responses.
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Considering a Rigid Body/Angular Momentum/Torque

We know that Torque(ext) = dL/dt

Now with respect to stationary point S:
L(s, cm) = Ʃ(ρi x mivi)
and that dL(cm)/dt = Ʃτ(ext, CM)

Now with respect to ANY point, P, that is accelerating:
L(s,p) = L(cm) + ρ(cm) x Mv(cm)
And hence,
Ʃτ(ext, p) = dL(rel_p)/dt + ρ(cm) x Ma(p)
Ʃτ(ext, p) = dL(rel_cm)/dt + ρ(cm) x Ma(cm)

Can someone explain to me why this happens?:
Why this happens? : Ʃτ(ext, p) = dL(rel_p)/dt + ρ(cm) x Ma(p)

Thanks
 
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