1/38 passive components and circuits - ccp lecture 5
TRANSCRIPT
![Page 1: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/1.jpg)
1/38
Passive components and circuits - CCPLecture 5
![Page 2: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/2.jpg)
2/38
Content
Capacity Properties DC behavior AC behavior Transient regime behavior
![Page 3: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/3.jpg)
3/38
Web addresses
http://en.wikipedia.org/wiki/RC_circuit http://www.solarbotics.net/bftgu/starting_elect_pass_cap.html http://www.st-andrews.ac.uk/~jcgl/Scots_Guide/info/comp/passive/
capacit/capacit.htm http://www.phy.ntnu.edu.tw/oldjava/rc/rc.htm http://www.ac.wwu.edu/~vawter/PhysicsNet/Topics/DC-Current/
RCSeries.html http://academic.evergreen.edu/projects/biophysics/technotes/electron/
rc.htm#time_const http://www.sciences.univ-nantes.fr/physique/perso/charrier/tp/rcrlrlc/
index.html http://zone.ni.com/devzone/cda/ph/p/id/217
![Page 4: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/4.jpg)
4/38
Electric capacitance - circuit element The electrical property of a
circuit element to store electric charge when a voltage is applied.
Measurement unit: Farad [F]
F, nF, pF
QC
V
C
V
+ -
n eg a tiv e
ch a rg e
p o sitiv e
ch a rg e
c
dt
dVCI
dtdVI
dtdVdtdQ
C CC
![Page 5: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/5.jpg)
5/38
Electric capacitance - circuit element Electronic component -
capacitor.
It is characterized by its capacity.
For a capacitor, the capacitance depends on the geometrical size and the dielectric properties
C a p a c itor p la te w ith
sur fa ce A
d
C a p a c itor p la te w ith
sur fa ce A
D ie le c tr ic c h a ra c te r ize d
b y re la t iv e p e rm it iv ity
T erm in a l
r
pF/m85419,80
0
d
AC r
![Page 6: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/6.jpg)
6/38
Stored energy The capacitor doesn’t dissipate power, but it is storing
energy when it is charging and is releasing the energy when it is discharging:
2
000 2
1CVdt
dt
dVVCVIdtPdtW
TTT
e
We is energy stored when the capacitance is charging to VC voltage or is discharged from VC to 0.
![Page 7: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/7.jpg)
7/38
Parallel connection The equivalent capacitance is equal
with the sum of capacitances
n
iiech
ii
echi
ii
CC
VVQQ
V
QC
V
QC
1
;
;
B
C1 C2 Cn Cech
A
B
A
![Page 8: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/8.jpg)
8/38
Series connection
The equivalent capacitance is given by the following formula:
n
i iech
ii
echi
ii
CC
QQVV
V
QC
V
QC
1
11
;
;
C1 C2 Cn
Cech
A
A
B
B
![Page 9: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/9.jpg)
9/38
DC regime behavior In DC, the capacitor corresponds to an open-circuit.
21 VVVAB 0CC
dt
dVC
dt
dvCi AB
C
A B
V1 V2
VAB
A B
V1 V2
VAB
DC
R1
iC
R2 R1 R2
iC =0
![Page 10: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/10.jpg)
10/38
AC regime behavior In AC regime, the capacitance is equivalent with ZC
impedance. The sinusoidal voltage applied is considered through the phasorial representation..
CZX
CjZ
i
vvCj
eeVCjdt
eeVdCi
eeVvdt
dvCi
CC
CC
CC
jtjjtj
C
jtjC
CC
1
1
;
Capacitance’s reactance
![Page 11: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/11.jpg)
11/38
AC regime behavior Impedance (reactance) is frequency dependent. In alternative current, the imittances of the circuits with
capacitors are dependent of the signals frequency. The property of a circuit to pass or reject some
frequencies is called filtering. Low-pass filter High-pass filter Band-pass filter Band reject filter
![Page 12: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/12.jpg)
12/38
RC low-pass filter;
1
1
( ) 1( )
( ) 1
oo i C C
C
Co i i
C
o
i
vv v R i i
Z
Z j Cv v v
R Z Rj C
v jH j
v j j RC
For R=1,6 K and C=100pF :
67 101
1
106,121
1)(
fjfj
jfH
vi is a sinusoidal voltage with frequency f = ω/2π (or ω=2π f)
C
R
vi
voZ
C
iC
![Page 13: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/13.jpg)
13/38
RC low-pass filter - frequency characteristics
![Page 14: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/14.jpg)
14/38
RC low-pass filter - frequency characteristics Answer to the following questions:
What kind of representation is used for modulus-frequency and phase-frequency characteristics?
What is the modulus-frequency characteristic slope for 100Hz – 100KHz domain? And in10MHz – 100MHz domain?
What is the phase difference between input and output voltages at the 1MHz?
Represent, at a 1MHz frequency, the input voltage phasor and the output voltage phasor. How does this representation look at 100MHz?
At what frequency is the phase difference between input and output φ=30?
How are the previous characteristics modified if R=16KΩ and C=100pF? How are the previous characteristics modified if R=1KΩ and C=1nF?
![Page 15: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/15.jpg)
15/38
RC high-pass filter
RCj
RCj
jv
jvjH
v
CjR
Rv
ZR
Rv
Z
vv
Z
viiRv
i
o
iiC
o
C
oi
C
CCCo
1)(
)()(
1
;
For R=1,6 K and C=100pF:
6
6
7
7
101
10
106,121
106,12)(
fj
fj
fj
fjjfH
vi is a sinusoidal voltage with frequency f = ω/2π (or ω=2π f)
vi
voR
C
ZC
iC
![Page 16: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/16.jpg)
16/38
High-pass RC filter - frequency characteristics
![Page 17: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/17.jpg)
17/38
High-pass RC filter - frequency characteristics Answer to the following questions:
What kind of representation is used for modulus-frequency and phase-frequency characteristics?
What is the modulus-frequency characteristic slope for 100Hz – 100KHz domain? And in 10MHz – 100MHz domain?
What is the phase difference between input and output voltages at the 1MHz?
Represent, at a 1MHz frequency, the input voltage phasor and the output voltage phasor. How does this representation look at 100MHz?
At what frequency is the phase difference between input and output φ= =30?
How are the previous characteristics modified if R=16KΩ and C=100pF?
How are the previous characteristics modified if R=1KΩ and C=2.2nF?
![Page 18: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/18.jpg)
18/38
The high frequencies behavior At high frequencies, the capacitive reactance is much lower
than resistances from the previous circuits. The capacitance is equivalent with a short-circuit.
C
R
vi
vo
vi
voR
C
R
vi
vo
vi
voR
=0
vi
=
V H F
V H F
![Page 19: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/19.jpg)
19/38
Separation and pass capacitances In some circuits, the capacitances are used to
separate the DC components (DC - open-circuit) between two circuits without affecting the signal variation (AC short-circuit)
In these situations, they are called separation capacitances (separation of DC components). In other situations, realizing the same functions, they are called passing capacitances (for high frequency signals).
![Page 20: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/20.jpg)
20/38
Capacitance behavior in transient regime In this case, the transient regime consist in the
modification of a DC circuit steady state in a new DC steady state.
During these modifications, the capacitance cannot be considered open-circuit or short-circuit.
The transient regime analysis presumes the determination of the way of charging and discharging of the capacitance.
In transient regime, the circuit operations are described by differential equations.
![Page 21: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/21.jpg)
21/38
The capacitance charging from a constant voltage source
Considering the K switch on position 1, the capacitance will be discharged.
At the time t=t0, the switch is moved on position 2.
After enough time, t, the capacitance will be charged at the E voltage.
The transient regime is taking place between these two DC steady states.
C
R
E vC
1
2K
iC
vR
![Page 22: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/22.jpg)
22/38
The capacitance charging from a constant voltage source
CC
CC
CCCC
CR
vdt
dvE
RCvdt
dvRCE
dt
dvCiviRE
vvE
;
;
:TKV
t
CCCC evvvtv
)]()0([)()(
)()(
)()0( 0
tvv
ttvv
C
CC
The solution of the differential equation
RC Circuit time constant
C
R
E vC
1
K
iC
2
vR
![Page 23: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/23.jpg)
23/38
Voltage variation across the capacitance, vC
t
CR
t
C
CC
eEtvEtv
eEtv
Evv
)()(
)1()(
)(;0)0(
![Page 24: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/24.jpg)
24/38
Current variation through the capacitance, iC
t
CC e
R
E
R
tvEti
)()(
![Page 25: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/25.jpg)
25/38
Significance of the time constant If the transient process has the same slope like in origins
(initial moment), the final values of voltages and currents will be obtain after a time equal with circuit time constant.
As can be seen in the previous figures, the charging process continues to infinite.
Practically, the transient regime is considered to be finished after 3 (95% from the final values) or 5 (99% from the final values).
![Page 26: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/26.jpg)
26/38
Example (E=1V, R=1KΩ, C=1nF)
![Page 27: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/27.jpg)
27/38
The capacitance discharging regime on a resistance
At the initial time, the switch is considered on position 2. The capacitance is charged to E voltage.
At a reference time moment t=t0, The K switch is moved on position 1.
After enough time, t, the capacitance is totally discharged.
The transient regime is taking place between these two DC steady states.
C
R
E vC
1
K
iC
2
vR
![Page 28: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/28.jpg)
28/38
The capacitance discharging regime on a resistance
CC
CC
CCCC
CR
vdt
dv
RCvdt
dvRC
dt
dvCiviR
vv
0
;0
;0
0:TKV
t
CCCC evvvtv
)]()0([)()(
0)()(
)()0( 0
tvv
Ettvv
C
CC
The solution of the differential equation
tR
C
CR
t
C
eR
E
R
tvti
tvtveEtv
)()(
)()(;)(
C
R
E vC
1
2K
iC
vR
![Page 29: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/29.jpg)
29/38
Example (E=1V, R=1KΩ, C=1nF)
![Page 30: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/30.jpg)
30/38
Charging the capacitance from a constant current source The K switch is considered in
position 1. The capacitance is considered initially charged to the voltage vC(0).
At reference time t=t0, the K is switched in position 2.
The constant current source will charge the capacitance with the current I.
C
R
I
vC
1
2K
iC
vR
R 1
![Page 31: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/31.jpg)
31/38
Charging the capacitance from a constant current source
)()()(1
)()(1
)()(
000
0
0
0
tvttC
ItvdtI
C
tvdttiC
tvdt
tdvCi
CC
t
t
C
t
t
CCC
C
vC
vC
t
0
(t)
(0)
slope = I/C
C
R
I
vC
1
2K
iC
vR
R 1
![Page 32: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/32.jpg)
32/38
Observations
The voltage across the capacitance will raise linearly.
The charging slope (or discharging) is independent by the value of resistance R (so, the resistor can misform the circuit).
Theoretically, the voltage across the capacitance can raise infinitely . In these situations, we must take some measures to limit the voltage on the capacitance.
![Page 33: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/33.jpg)
33/38
The RC circuits behavior when pulses are applied
Consider a pulses signal source applied to a series RC circuit.
In analyzing the circuit behavior, we consider both voltages: the voltage across the capacitor, vC(t), and the voltage across the, vR(t).
Applying this signal source, the phenomena of charging and discharging described to transient regime are repetitive.
C
R
vC
iC
vR
vI
![Page 34: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/34.jpg)
34/38
Case A – the time constant is much lower than pulses duration
![Page 35: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/35.jpg)
35/38
Case B – the time constant is much greater than pulses duration
![Page 36: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/36.jpg)
36/38
Integrating circuit
If the output voltage is the voltage across the capacitor, the effect under the input signal is attenuation of edges, similarly with the integration operation.
In this situation,(when vO(t)=vC(t)), the circuit is called integration circuit.
The integration effect is higher in case B , when the time constant is greater then the pulse duration.
The integration function in transient regime corresponds to low-pass filtering in AC regime.
![Page 37: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/37.jpg)
37/38
Derivative circuit If the output voltage is the voltage across the resistor,
the circuit effect under the input signal is an accentuation of edges, similarly with derivative mathematical operation.
In this situation,(when vO(t)= vR(t)), the circuit is called derivative circuit.
The derivative effect is higher in case A , when the time constant is lower then pulse duration.
The derivative function in transient regime corresponds to high-pass filtering in AC regime.
![Page 38: 1/38 Passive components and circuits - CCP Lecture 5](https://reader035.vdocuments.mx/reader035/viewer/2022062423/56649e755503460f94b76c20/html5/thumbnails/38.jpg)
38/38
Answer to the following questions
How are the waveforms modified if the input source for the RC series circuit is a pulses current source?
Can the current source pulses be asymmetrical? (from 0 on the current axis)?
How does the voltage across the capacitor (or resistor) vary if the pulses have the same duration with the circuit time constant? Make the analysis starting with the initial time moment, when the capacitor is completed discharged.
For the homework problem from the end of lecture 2, consider that the resistor R is replaced by a capacitance C=10nF. Draw the waveform of the voltage across the capacitance.