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ISU EE C.Y. Lee
Chapter 10RC Circuits
2ISU EE C.Y. Lee
ObjectivesDescribe the relationship between current and voltage in an RC circuitDetermine impedance and phase angle in a seriesRC circuitAnalyze a series RC circuitDetermine the impedance and phase angle in a parallel RC circuitAnalyze a parallel RC circuit Analyze series-parallel RC circuitsDetermine power in RC circuits
3ISU EE C.Y. Lee
Sinusoidal Response of RC Circuits
The capacitor voltage lags the source voltage Capacitance causes a phase shift between voltageand current that depends on the relative values of the resistance and the capacitive reactance
4ISU EE C.Y. Lee
Impedance and Phase Angle of Series RC Circuits
The phase angle is the phase difference between the total current and the source voltageThe impedance of a series RC circuit is determined by both the resistance (R) and the capacitive reactance (XC)
(Z = RjXC)(Z = jXC)(Z = R)
(ZC= 1/jC= jXC) (Z= R+ZC= RjXC)
5ISU EE C.Y. Lee
Impedance and Phase Angle of Series RC Circuits
In the series RC circuit, the total impedance is the phasor sum of R and jXCImpedance magnitude: Z = R2 + X2CPhase angle: = tan-1(XC/R)
6ISU EE C.Y. Lee
Impedance and Phase Angle of Series RC Circuits
Z = (47)2 + (100)2 = 110 = tan-1(100/47) = tan-1(2.13) = 64.8
Example: Determine the impedance and the phase angle
7ISU EE C.Y. Lee
Analysis of Series RC Circuits
The application of Ohms law to series RC circuits involves the use of the quantities Z, V, and I as:
IZV =
ZVI =
IVZ =
8ISU EE C.Y. Lee
Analysis of Series RC CircuitsExample: If the current is 0.2 mA, determine the source
voltage and the phase angle
XC = 1/2(1103)(0.0110-6) = 15.9 kZ = (10103)2 + (15.9103)2 = 18.8 kVS = IZ = (0.2mA)(18.8k) = 3.76 V = tan-1(15.9k/10k) = 57.8
9ISU EE C.Y. Lee
Relationships of I and V in a Series RC Circuit
In a series circuit, the current is the same through both the resistor and the capacitorThe resistor voltage is in phase with the current, and the capacitor voltage lags the current by 90
I
VR
VC
VS
10ISU EE C.Y. Lee
KVL in a Series RC Circuit
From KVL, the sum of the voltage drops must equal the applied voltage (VS)
Since VR and VC are 90out of phase with each other, they must be added as phasor quantities
VS = V2R + V2C = tan-1(VC/VR)
VR
VC
VS
I
VR= IR
VS= IZ = I(RjXC)VC= I(jXC)
11ISU EE C.Y. Lee
KVL in a Series RC CircuitExample: Determine the source voltage and the phase angle
VS = (10)2 + (15)2 = 18 V = tan-1(15/10) = tan-1(1.5) = 56.3
12ISU EE C.Y. Lee
Variation of Impedance and Phase Angle with Frequency
For a series RC circuit; as frequency increases: R remains constant XC decreases Z decreases decreases
f Z
R
13ISU EE C.Y. Lee
Variation of Impedance and Phase Angle with Frequency
Example: Determine the impedance and phase angle for each of the following values of frequency: (a) 10 kHz (b) 30 kHz
(a)XC = 1/2(10103)(0.0110-6) = 1.59 kZ = (1.0103)2 + (1.59103)2 = 1.88 k = tan-1(1.59k/1.0k) = 57.8
(b)XC = 1/2(30103)(0.0110-6) = 531 kZ = (1.0103)2 + (531)2 = 1.13 k = tan-1(531/1.0k) = 28.0
14ISU EE C.Y. Lee
Impedance and Phase Angle of Parallel RC Circuits
Total impedance in parallel RC circuit:Z = (RXC) / ( R2 +X2C)
Phase angle between the applied V and the total I: = tan-1(R/XC)
( )
jRXRXZ
jXRRjX
Z
jXRZ
C
C
C
C
C
+=
+
=
+=
1
111
+
==jRX
RXIIZVC
C
15ISU EE C.Y. Lee
Conductance, Susceptance and Admittance
Conductance is the reciprocal of resistance:G = 1/R
Capacitive susceptance is the reciprocal of capacitive reactance:
BC = 1/XCAdmittance is the reciprocal of impedance:
Y = 1/Z
16ISU EE C.Y. Lee
Ohms Law
Application of Ohms Law to parallel RC circuits using impedance can be rewritten for admittance (Y=1/Z):
YIV =
VYI =
VIY =
17ISU EE C.Y. Lee
Relationships of the I and V in a Parallel RC Circuit
The applied voltage, VS, appears across both the resistive and the capacitive branchesTotal current, Itot, divides at the junction into the two branch current, IR and IC
Vs, VR, VC
IR= V/R
Itot= V/Z = V((XC+jR)/RXC)IC= V/(jXC)
18ISU EE C.Y. Lee
KCL in a Parallel RC Circuit
From KCL, Total current (IS) is the phasor sum of the two branch currents
Since IR and IC are 90out of phase with each other, they must be added as phasor quantities
Itot = I2R + I2C = tan-1(IC/IR)
IR= V/R
Itot= V/Z = V((XC+jR)/RXC)IC= V/(jXC)
19ISU EE C.Y. Lee
KCL in a Parallel RC CircuitExample: Determine the value of each current, and describe
the phase relationship of each with the source voltage
IR = 12/220 = 54.5 mAIC = 12/150 = 80 mAItot = (54.5)2 + (80)2 = 96.8 mA = tan-1(80/54.5) = 55.7
Vs
20ISU EE C.Y. Lee
Series-Parallel RC CircuitsAn approach to analyzing circuits with combinations of both series and parallel R and C elements is to: Calculate the magnitudes of capacitive reactances (XC) Find the impedance (Z) of the series portion and the
impedance of the parallel portion and combine them to get the total impedance
21ISU EE C.Y. Lee
(Z)(Z')(Z"):
Z= Z' jZ"
( )mi jXRRZ ++=
111
( ) 22222
mie
meieie
XRRXRRRRRZ
++++
=
( ) 222
mie
me
XRRXRj++
22ISU EE C.Y. Lee
23ISU EE C.Y. Lee
c c
Z-plot
Z:
Zs:
fC ():Z"
( ) ( )22 ZZZ +=
24ISU EE C.Y. Lee
Z-plot
25ISU EE C.Y. Lee
RC Lag NetworkThe RC lag network is a phase shift circuit in which the output voltage lags the input voltage
=
RXC1tan90o
26ISU EE C.Y. Lee
RC Lead NetworkThe RC lead network is a phase shift circuit in which the output voltage leads the input voltage
=
RXC1tan
27ISU EE C.Y. Lee
Frequency Selectivity of RC CircuitsA low-pass circuit is realized by taking the output across the capacitor, just as in a lag network
28ISU EE C.Y. Lee
Frequency Selectivity of RC CircuitsThe frequency response of the low-pass RC circuit is shown below, where the measured values are plotted on a graph of Vout versus f.
10 V
29ISU EE C.Y. Lee
Frequency Selectivity of RC CircuitsA high-pass circuit is implemented by taking the output across the resistor, as in a lead network
30ISU EE C.Y. Lee
Frequency Selectivity of RC CircuitsThe frequency response of the high-pass RC circuit is shown below, where the measured values are plotted on a graph of Vout versus f.
10 V
31ISU EE C.Y. Lee
Frequency Selectivity of RC CircuitsThe frequency at which the capacitive reactance equals the resistance in a low-pass or high-pass RC circuit is called the cutoff frequency:
RCfC 2
1=
32ISU EE C.Y. Lee
Coupling an AC Signal into a DC Bias Network
33ISU EE C.Y. Lee
Summary
When a sinusoidal voltage is applied to an RC circuit, the current and all the voltage drops are also sine wavesTotal current in an RC circuit always leads the source voltageThe resistor voltage is always in phase with the currentIn an ideal capacitor, the voltage always lags the current by 90
34ISU EE C.Y. Lee
Summary
In an RC circuit, the impedance is determined by both the resistance and the capacitive reactance combinedThe circuit phase angle is the angle between the total current and the source voltageIn a lag network, the output voltage lags the input voltage in phaseIn a lead network, the output voltage leads the input voltageA filter passes certain frequencies and rejects others
Chapter 10ObjectivesSinusoidal Response of RC CircuitsImpedance and Phase Angle of Series RC CircuitsImpedance and Phase Angle of Series RC CircuitsAnalysis of Series RC CircuitsAnalysis of Series RC CircuitsRelationships of I and V in a Series RC CircuitKVL in a Series RC CircuitKVL in a Series RC CircuitVariation of Impedance and Phase Angle with FrequencyVariation of Impedance and Phase Angle with FrequencyImpedance and Phase Angle of Parallel RC CircuitsConductance, Susceptance and AdmittanceOhms LawRelationships of the I and V in a Parallel RC CircuitKCL in a Parallel RC CircuitKCL in a Parallel RC CircuitSeries-Parallel RC CircuitsRC Lag NetworkRC Lead NetworkFrequency Selectivity of RC CircuitsFrequency Selectivity of RC CircuitsFrequency Selectivity of RC CircuitsFrequency Selectivity of RC CircuitsFrequency Selectivity of RC CircuitsCoupling an AC Signal into a DC Bias NetworkSummarySummary