rlc circuits
DESCRIPTION
RLC Circuits. PH 203 Professor Lee Carkner Lecture 24. RCL and AC. w d = 2 p f X C = 1/( w d C) X L = w d L If you combine a resistor, capacitor and an inductor into one series circuit, they all will have the same current but all will have difference voltages at any one time - PowerPoint PPT PresentationTRANSCRIPT
RLC Circuits
PH 203
Professor Lee Carkner
Lecture 24
RCL and AC
d = 2fXC = 1/(dC)
XL = dL If you combine a resistor, capacitor and an
inductor into one series circuit, they all will have the same current but all will have difference voltages at any one time Voltages are all out of phase with each other
RLC Circuit
RLC Impedance
Called the impedance (Z)
Z = (R2 + (XL - XC)2)½
The voltages for the inductor and capacitor are 180 degrees opposed and so subtract
V = IZ Can think of Z as a generalized resistance for any AC circuit
Time Dependence
The instantaneous value (v, i) The maximum value (V, I) The root-mean-squared value (Vrms, Irms)
However, the average of a sinusoidal variation is 0
Finding rms
Since power depends on I2 (P =I2R) it does not care if the current is positive or negative
Irms = I/(2)½ = 0.707 I
Vrms = V/(2)½ = 0.707 V The rms value is about
71% of the maximum
Phase Angle and Power Factor
They are separated by a phase angle often written as:
cos = IR/IZ = R/Z
But I and V are out of phase and sometime they reinforce each other and sometimes they cancel out
Can write power as:
Pav = IrmsVrms cos
We just need to know V and I through it at a given time
High and Low f
For high f the inductor acts like a very large resistor and the capacitor acts like a resistance-less wire
At low f, the inductor acts like a resistance-less wire and the capacitor acts like a very large resistor No current through C, full current through L
Natural Frequency
Example: a swing
If you push the swing at all different random times it won’t
If you connect it to an AC generator with the same frequency it will have a large current
Resonance
This condition is known as resonance
Low Z, large I (I = V/Z)
Z = (R2 + (XL - XC)2)½
This will happen when d = 1/(LC)½
Frequencies near the natural one will produce large current
Resistance and Resonance Note that the current still depends on the resistance
at resonance, the capacitor and inductor cancel out
If we change R we do not change the natural frequency, but we do change the magnitude of the maximum current
Since the effect of L and C are smaller in any case
Next Time
Read 32.1-32.5 Problems: Ch 31, P: 45, 46, 61, Ch 32, P:
12, 14