carlgrace
- 555
- 10
IssacBinary said:IM NOT SAYING we can work out everything without maths. NO. OF COURSE you need maths.
So your telling me if you told someone
I = C d(Vc)/dt
they will be able to see what it means and just come up with the long paragraph explanation which you just told me? about the electrons moving, more there are the more push is needed etc..
I sure don't know anyone that does...
I can do the maths, I can get the end result and know what it means.
But I want a LONG PARAGRAPH that generally explains what is causing the OVERALL phase shift in the circuit: total impedance phase.
So...can you tell me?
Sure...
An inductor is a device that creates a magnetic field due to a changing current being forced in loops through it. This magnetic field induces a current on the same wire that creates it, but that induced current opposes the original current. So, like a cat chasing its own tail, the inductor opposes changes in its own current. It takes some time to set up this magnetic field. The faster the current changes, the more the induced magnetic field opposes the current change, so inductors are sort of devices that present a "resistance" frequency proportional to frequency (this is called impedance).
The voltage across this inductor is maximum when the time-rate-of-change of the current through it is maximum. This time-rate-of-change of current is maximum when the current passes through 0. Therefore, we get a 90 degree phase shift. This is qualitative, not "math". OF COURSE the voltage must act this way since we already saw that the inductor acts as kind of a frequency proportional resistor. So, its maximum opposing voltage must occur when the inducing current is changing most quickly. That is 1/4 of a period of the sinusoidal input current.
The capacitor is analogous in its behavior, but acts differently physically. The result is the same... the maximum current "through" a capacitor occurs at the point at which the time-rate-of-change of the voltage is a maximum. For a sinusoidal voltage, these occur shifted by 1/4 of a period.
You get various phase angles in real circuits because of the various contributions of pure resistances (which have no phase difference between maximum current and maximum voltage) and reactances. You can see this intuitively if you just think of Kirchoff's voltage and current laws. It is helpful to think of a single frequency. Algebraically, you just use vector algebra to sort out this situation.
The "overall phase shift" then breaks down like this. At a given frequency, the impedances of the inductors and capacitors can be thought of like resistances. Then, the input current or voltage will be split up between these devices in accordance with KCL and KVL. The amount of phase shift at this particular frequency depends on the relative impedances at that particular frequency. For example if the circuit is dominated by reactance at that particular frequency, you will get a lot of phase shift... if it is dominated by resistance at that frequency you will get a little bit of phase shift.
The relative amounts of resistance and reactance in the circuit will change as the frequency changes. The pure resistance will remain the same but the amount of "effective resistance" presented by the inductors and capacitors will change. This ratio of pure and "effective" resistance gives rise to the overall total impedance phase.
Hope this helps!
Carl