Mr.Bomzh said:
Well I had a look at the paper and I went through it but it had only formulas and some for me vague explanations because I'm not that good at maths , anyways the paper felt like when youre really hungry but your hands are shaking and everything falls out of the spoon so you can;'t get no satisfaction. :D Ok let's take the simplest case , a rotating disc , a magnet at one point from both sides of the disc and contact points , now the magnetic field line from the magnet are goign through the disc parallel to the center shaft or axis and perpendicular to the surface of the disc , current goes from the center to the outer part of the disc or vice versa depending on the poles or way of rotation , the lorentz force then is 90 degrees shifted from the current or aka perpendicular to both current and magnetic field. If so far is fine but I still can't quite figure out why does there is current induced in the disc , well the only way that I could find out is that maybe one does need to imagine the disc being cut and made from many many smaller separate wires all starting from the middle going towards the outerside, moving such wires through the field of the magnets would induce current in them , so the only thing that differs here is that instead of many wires we have a one solid disc but we could effectively treat the part which passes the magnets at each given time as as sinbgle wire or piece of conductor through which the current moves right? and more the current can only move between the contacts so if the ciontacts are made at the same position at which the magnet is located then everytime a part of that disc moves through those magnets and the field they make in that part a current is induced which runs towards those contacts is they form a circuit , is that abour right?
Dr. Munley's paper explains this. The current path for the electrons is from the center towards the rim (or vice-versa, but let's go with center to rim for now). But as the electrons transit from center to rim, the disk is rotating. When an electron which starts at the center reaches the contact on the rim, it sweeps out a pie shaped sector of area. The B value is constant, and B is flux density in tesla, or weber/m
2. The flux ø is area times B, or A*B. THe area of the pie shaped sector is θ*R
2/2, where θ is the angular displacement in radians.
So the area is changing as the disk turns in a manner directly related to θ to the 1st power. But θ is related to angular valocity ω as follows:
θ = ω*t
Here "t" is time. Thus the area of the filamentary current loop is just ω*R
2*t/2. Thus the magnetic flux ø is the area times B, or ø = ω*B*R
2*t/2. Notice that t is in the 1st power (time).
But we know that v(t), the emf, is -N*dø/dt. What is the derivative of a constant times time to the 1st power? I.e. d(ω*B*R
2*t/2)/dt is just ω*B*R
2/2. In the derivative, time does not appear, because the derivative of t to 1st power is a constant. Thus the induced emf is indeed zero frequency, or "dc".
I can elaborate if needed. But please re-read Dr. Munley, and hopefully it will make more sense now.
Claude