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I guess on a lot of the questions
its odd to me because in the second case you are expecting the work to be positive since at the bottom of the swing there is a maximum velocity and so the intial velocity should be smaller then the final leading to positive work integral.
the first is mgR(cos(θ) - cos(θi)) and the second is -mgR((cos(θ) - cos(θi)) the second gives a negative kinetic energy for the change from a higher θ to a lower θ(like from pi/2 to 0), is that correct?
And taking the opposite direction of displacement and force works, but trying to derive a situation where the point mass starts at zero velocity at a some θ and going to θ = 0 at max velocity makes no sense from this integral ∫force⋅displacement = Δk, where the directions are the same. Unless...
its when you take the integral ∫mgsin(θ)⋅ds and the direction of the ds and force is the same , then the integral sin is -cos for the integral, I don't see how to get this integral through your method, but isn't it valid for work-kinetic theorem ∫force⋅displacement = Δk
If i keep with your scenario, I have no problem with anything you said here.
In your same setup I have a problem with starting from the top with the θ initial greater than zero and going to θ=0, if you use the work kinetic theorem you get a negative Δk, that is the - mgR(cos(θ) -...
You need the change in sign to get the right answer, - mgR(cos(θ) - cos(θ(0)) will for instance give you a negative kinetic change if you take the initial θ(0) greater than θ. Which doesn't make sense for a pendulum starting from a higher height and ending at a lower height, it should have a...