To figure out the velocity at a given point in the string you need to find the tension there. The element at that position does not care how the tension is created.
Write an expression for ##T(x)##.
Shouldn't that denominator quadratic be raised to the power of 3/2?
Don't forget to apply an approximation for small r. And as @kuruman notes, it is the field normal to the axis that is interesting.
It's just Pythagoras.
To avoid confusion, I will take the point of interest as being at z' from the solenoid, instead of at x.
In (x,y,z) coordinates, where the negative z axis is the axis of the cylinder, you have a fixed point at (0,r,z'). Your solenoid element is at ##(R\cos(\phi)...
I thought this question was familiar, even in that the official answer is wrong. https://www.physicsforums.com/threads/how-is-work-calculated-on-a-conveyor-belt-with-friction.1061325/
In part a, nothing is rotating yet, so Euler's equation reduces to ##\vec\tau=I\dot{\vec\omega}##.
Part b is solved most simply using energy.
If you mean the generalisation of being at angle ##\theta##, that should work, but it still seems like overkill.
… and part b specifies "when the rod is vertical after rotating 90 degrees".
As I read the question, part a asks for the angular acceleration when released from horizontal and part b asks for the angular velocity at the vertical. Neither requires you to consider an arbitrary angle in between.
I didn’t read that in detail because it was evidently much more complicated than it needed to be.
You should be able to write down the MoIs about the pivot straight off: ##ML^2/3+m(L/3)^2+2m(2L/3)^2##.
Similarly the torque about the pivot: ##(ML/2+mL/3+2m(2L/3))g##.
I agree with your electrostatic force. You need to calculate q, though.
For the magnetic force, you could divide each strip into narrower strips and find the horizontal components of the pairwise attractions.