That makes a lot more sense! Just to make sure, can F = ma be applied to all phenomena involving force? I'm trying to break this down. I understand that if a = 0 then F = 0, but I want to make sure that based on T = Fd, I can write it as T = (ma)d? and hence show that Torque is basically 0? Or is the 'F' from T = Fd basically coming from F = BILSin(x)?
You can't
really write that. The issue is the \(m\). The \(m\) isn't the same for the angular version, the real thing is actually:
Where \(\tau\) is torque, \(\alpha\) is angular acceleration, and \(I\) is the
moment of inertia. This is just a quantity analogous to mass in linear problems - There are formulas that let you calculate \(I\) for certain objects, but they (and all this message) are not assessable
The angular acceleration and \(a\) are also different! Writing \(\tau=Mad\) is basically saying, if I have a mass accelerating at a certain rate, and tie it to something else at a set distance that then causes it to spin, then you get torque. But \(a\neq\alpha\), and \(m\neq I\), because one is linear and one is rotational
(
Again, not assessable! This is uni stuff )
You can apply the idea in principal even without the maths though. No angular acceleration means no angular force, which means no torque (same thing)
Oh, and the force in the torque formula does come from \(F=BIL\sin{\theta}\) in a motor, but since you've got multiple sides and varying angles as the motor spins, you can't say, \(\tau=BIL\sin{\theta}\times d\)