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![Page 1: Advance Electronic Circuit](https://reader031.fdocuments.us/reader031/viewer/2022013102/54fb85324a7959575b8b52fc/html5/thumbnails/1.jpg)
A. Kruger Lecture 9-15-1Advanced Electronic Circuits 55:036 The University of Iowa, 2009
55:195 Advanced Electronic Circuits
Lecture 9-15
Switching Regulators
Material: Lecture Notes & Handouts
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A. Kruger Lecture 9-15-2Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Why Study Power Supplies?
Electronic Design 01/4/10 page 33.
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A. Kruger Lecture 9-15-3Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Why Study Power Supplies?
We will look at this
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A. Kruger Lecture 9-15-4Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Switching Power Supplies
Primary switching power supplies
Convert line (120/240 VAC) to DC
Switchers, SMPS, medical switchers, etc.
Efficient
Small
Uses smaller transformer, inexpensive compared
to a non-switching power supply with the same power-handling capability
Cell-phone chargers, laptop power supplies, medical equipment, etc.
Secondary switching power supplies
Convert DC to DC
Also called DC/DC converters
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A. Kruger Lecture 9-15-5Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Linear Power Supply
Bulky, expensive transformer
Linear regulator, often
dissipates significant power
and need expensive heat
sinks.
Ripple voltage isfC
IV L
pp2
Where f is the line frequency (50/60 Hz)
Thus for good pre regulation, need large
C (bulky, $$$)
LI
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A. Kruger Lecture 9-15-6Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Switch Mode Power Supply
The rest of the circuit
can tolerate significant
ripple, so C can be small
Chop DC at 50
kHz – 1 MHz
Recall the universal
transformer equationfNaB
fNaBE
peak
rms 44.42
2
High frequencies require smaller transformers
Ripple voltage isfC
IV L
pp2
High frequencies require small C
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A. Kruger Lecture 9-15-7Advanced Electronic Circuits 55:036 The University of Iowa, 2009
DC/DC Converter
Linear Regulator Switching Regulator
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A. Kruger Lecture 9-15-8Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Switching Regulator Topologies
Buck Boost
Buck-Boost
IO DVV IO VD
V1
1
IO VD
DV
1
Note that the average output
voltage is essentially independent
from the value of L and C
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A. Kruger Lecture 9-15-9Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Buck Converter
ONS
S
ON
OFFON
ON tfT
t
tt
tD
What factors affects efficiency?
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A. Kruger Lecture 9-15-10Advanced Electronic Circuits 55:036 The University of Iowa, 2009
With switched closed, voltage cross the inductor is VI - Vo – VSAT and the
current though the inductor increases linearly. After tON, the inductor
current has increased byON
sattIoL t
L
VVVi
Assume output and input voltages are constant. VSAT is the voltage across the (BJT/FET) switch when
closed, and VD is the voltage cross the diode when conducting.
When the switch opens, current cannot change instantaneously, voltage
across inductor reverses, and cathode swings to below ground. The
voltage across the inductor is Vo+VD and the current decreases linearly as
the magnetic field collapses. After tOFF, the current has decreased by
OFFDo
L tL
VVi
In the steady state, the increase during tON should balance the decrease during tOFF , so that
OFFONSAT t
L
VVt
L
VVV DoIo
Solving for Vo and recognizing that tON + tOFF = 1/f and that D = tON + tOFF is the duty cycle D, then
IDIo DVVDVVDV 1SATNote that this is independent of the load current, L, and C
Switch
Close
Switch
Open
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A. Kruger Lecture 9-15-11Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Buck DC/DC Converter
Called continuous conduction mode (CCM),
where the inductor current never goes to zero
In the CCM, output voltage is independent of
the load current
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A. Kruger Lecture 9-15-12Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Buck Regulator: Discontinuous Mode
This is called discontinuous conduction mode
(DCCM)
ONsattIo
L tL
VVVi OFF
DoL t
L
VVi
When load current drops, the output voltage
stays constant, and ΔiL stays the same.
When the load current falls below a critical
value Iomin the inductor goes to zero during a
cycle.
i
ooomin
V
VV
L
TI 1
2
In DCCM, more energy is stored than
extracted in each cycle and the output voltage
rises (and some of our assumptions thus far
are not valid…)
The controller will reduce D to keep Vo fixed
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A. Kruger Lecture 9-15-13Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Buck Switching Regulator
Only valid for CCMIO DVV
When the converter goes into
DCCM, output voltage rises and
controller reduced duty cycle to
keep voltages fixed
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A. Kruger Lecture 9-15-14Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Buck Ripple Voltage
Capacitor smoothes output voltage. The capacitor charge current is IL – Io. The
charge applied and removed during one cycle corresponds to the hatched area
(remember Q = I t) The change in capacitor voltage is thus
LL
o IC
TItt
CC
QV
82222
11 OFFON
Note: both ΔIL and ΔVo are peak-to-peak values.
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A. Kruger Lecture 9-15-15Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Buck Ripple Voltage
LL
o IC
TItt
CC
QV
82222
11 OFFON
However, the capacitor has an ESR, that also contributes to the ripple voltage.
The voltage across the ESR is
Note that the voltage is not in phase with the voltage across the capacitor:
CESR iESRv
ESR
oESRr VjvV
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A. Kruger Lecture 9-15-16Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Buck Capacitor Selection
LL
o IC
TItt
CC
QV
82222
11 OFFON
Both capacitance and ESR contribute to ripple voltage.
CESR iESRv
ESR
oESRr VjvV
Capacitor dissipates (ESR) I 2C(rms) and must be able to handle this
Capacitor must be able to handle ripple current ΔILGood capacitor must can cost $$$
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A. Kruger Lecture 9-15-17Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Buck Coil Selection
Continuous Mode Discontinuous Mode
2
2
1LL Liw
LS
IOO
if
VVVL
)/1(
LL Ii 2.0
Suggested Design Equation
Coil must handle IP without
saturating the core.
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A. Kruger Lecture 9-15-18Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Efficiency
If all the components are lossless:
ESR = 0
VD = 0
ESL = 0
Switch resistance = 0
Then the buck DC/DC converter can provide 100% conversion
disso
o
PP
Pooo IVP
controllercapcoilDSWdiss PPPPPP
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A. Kruger Lecture 9-15-19Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Efficiency
disso
o
PP
Pooo IVP
controllercapcoilDSWdiss PPPPPP
SWSWSWSWSATD tivIVP 2 2
)(rmsCcap IESRP
)(2
)( fPIRP corermsLcoilcoil
RRFRsavgFDD tIVfIVP )(
Conduction loss Switching loss
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A. Kruger Lecture 9-15-20Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Buck Coil Selection
Continuous Mode Discontinuous Mode
2
2
1LL Liw
LS
IOO
if
VVVL
)/1(
LL Ii 2.0
Suggested Design
Equation
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A. Kruger Lecture 9-15-21Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Coil Selection
Coil must carry some rms
current IL to feed the load
Discontinuous Mode
OL II
O
I
OL I
V
VI 1
O
I
OL I
V
VI
Buck
Buck-boost
Boost
Coil must handle IP without
saturating the core.
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A. Kruger Lecture 9-15-22Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Switching Regulator: Controller
Both Pulse Frequency Modulation and Pulse Width Modulation (PWM) can
be used for control.
Most commercial ICs use PWM control with fs between 10 kHz and 1 MHz
Two-types of control: voltage and current-mode control
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A. Kruger Lecture 9-15-23Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Voltage Mode PWM Control
Voltage Mode Control Waveforms
Comparator
Sawtooth generator running at fS
Question: what type of feedback? How does it
affect the output resistance?
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A. Kruger Lecture 9-15-24Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Voltage Mode PWM Control
Voltage Mode Control Waveforms
Comparator
Sawtooth generator running at fS
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A. Kruger Lecture 9-15-25Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Error Amplifier in CCM Voltage Control
Assume changes in
output voltage is much
slower than fs
Equivalent for buck
converter operating in
CCM with voltage control
Model as a linear system
Will analyze later
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A. Kruger Lecture 9-15-26Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Gated Oscillator Converter
Reference
Oscillator, fixed
duty cycle
Switch
Uncommitted
op-amp
Comparator
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A. Kruger Lecture 9-15-27Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Gated Oscillator Converter
Comparator with hysteresis ~ 10 mV
Non-linear element non-linear feedback
More stable feedback, more efficient converter
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A. Kruger Lecture 9-15-28Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Gated Oscillator Converter
Very low supply current – oscillator switched only when needed, when FB drops
below reference
Adaptive base drive to make sure switch is not overdriven improve efficiency
Hysteresis ensures loop stability without complex compensation networks
D Duty cycle optimized for circuits where Vin and Vout differ by factor D
Can be uses to terminate switch
cycle prematurely Comparator with hysteresis ~ 10 mV
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A. Kruger Lecture 9-15-29Advanced Electronic Circuits 55:036 The University of Iowa, 2009
LT1173 DC/DC Converter
Switch frequency ~ 24 kHz, duty cycle ~ 50%
1 A internal switch
Comparator with ~ 5 mV hysteresis
Uncommitted op-amp
100 μA in standby mode
Step-up or step down
Supply 2.0 – 30 V
50% Duty cycle
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A. Kruger Lecture 9-15-30Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Wiring as a buck
regulator
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A. Kruger Lecture 9-15-31Advanced Electronic Circuits 55:036 The University of Iowa, 2009
L
CD
VI
Vo
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A. Kruger Lecture 9-15-32Advanced Electronic Circuits 55:036 The University of Iowa, 2009
L
CD
R2
R1
VI
Vo
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A. Kruger Lecture 9-15-33Advanced Electronic Circuits 55:036 The University of Iowa, 2009
L
CD
R2
R1
Choose either R2 or R1, solve for other one. Choose a
value > 50K
VI
Vo
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A. Kruger Lecture 9-15-34Advanced Electronic Circuits 55:036 The University of Iowa, 2009
L
CD
R2
R1
Choose either R2 or R1, solve for other one. Choose a
value > 50K
VI
Vo
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A. Kruger Lecture 9-15-35Advanced Electronic Circuits 55:036 The University of Iowa, 2009
L
CD
C1
R2
R1
Choose either R2 or R1, solve for other one. Choose a
value > 50K
VI
Vo
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A. Kruger Lecture 9-15-36Advanced Electronic Circuits 55:036 The University of Iowa, 2009
L
CD
C1C2
R2
R1
L1
Choose either R2 or R1, solve for other one. Choose a
value > 50K
VI
Vo
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A. Kruger Lecture 9-15-37Advanced Electronic Circuits 55:036 The University of Iowa, 2009
L
CD
C1C2
R2
R1
L1
Choose either R2 or R1, solve for other one. Choose a
value > 50K
VI
Vo
C = Low ESR
D = Schottky
L = No saturation
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A. Kruger Lecture 9-15-38Advanced Electronic Circuits 55:036 The University of Iowa, 2009
L
C
D
C1C2
R2
R1
L1
Choose either R2 or R1, solve for other one. Choose a
value > 50K
VI
Vo
C = Low ESR
D = Schottky
L = No saturation
Wiring as a boost
regulator
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A. Kruger Lecture 9-15-39Advanced Electronic Circuits 55:036 The University of Iowa, 2009
L
C
D
C1C2
R2
R1
L1VI
Vo
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A. Kruger Lecture 9-15-40Advanced Electronic Circuits 55:036 The University of Iowa, 2009
L
C
D
R2
R1
VI
Vo
Increasing Output Drive
Buck Regulator
What if this switch
can not handle the
peak and rms
currents?
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A. Kruger Lecture 9-15-41Advanced Electronic Circuits 55:036 The University of Iowa, 2009
L
C
D
R2
R1
VI
Vo
Increasing Output Drive, Take 1
Add external power
transistor to make
this a Darlington
Transistor
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A. Kruger Lecture 9-15-42Advanced Electronic Circuits 55:036 The University of Iowa, 2009
L
C
D
R2
R1
VI
Vo
Increasing Output Drive, Take 1
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A. Kruger Lecture 9-15-43Advanced Electronic Circuits 55:036 The University of Iowa, 2009
L
C
D
R2
R1
VI
Vo
Increasing Output Drive, Take 2
Add external
“high-side “switch
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A. Kruger Lecture 9-15-44Advanced Electronic Circuits 55:036 The University of Iowa, 2009
L
C
D
R2
R1
VI
Vo
Increasing Output Drive, Take 2
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A. Kruger Lecture 9-15-45Advanced Electronic Circuits 55:036 The University of Iowa, 2009
L
C
D
R2
R1
VI
Vo
Increasing Output Drive, Take 2
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A. Kruger Lecture 9-15-46Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Increasing Output Drive, Take 2
A application notes for a particular chip often
contain a wealth of information
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A. Kruger Lecture 9-15-47Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Increasing Output Drive, Take 3
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A. Kruger Lecture 9-15-48Advanced Electronic Circuits 55:036 The University of Iowa, 2009
LT1173 DC/DC Converter
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A. Kruger Lecture 9-15-49Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Error Amplifier in CCM Voltage Control
Assume changes in
output voltage is much
slower than fs
Equivalent for buck
converter operating in
CCM with voltage control
Model as a linear system
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A. Kruger Lecture 9-15-50Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Error Amplifier in CCM Voltage Control
What is the gain of Mod ?
Io DVV
sm
I
c
o
V
V
v
V
sm
c
V
vD
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A. Kruger Lecture 9-15-51Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Error Amplifier in CCM Voltage Control
Qj
j
V
V
V
VH z
sm
I
C
OCO
0
2
01
1
LCESRRQ
CESRLCz
)(
1
)(
11
coil
0
Note that L and C in loop create a complex pole pair, and ESR creates as zero.
Assume that the switching frequency is high enough so that PWM can be regarded as a
continuous process over range of (load) frequencies.
Purpose of EA is to provide good regulation and good phase margin to ensure stability.
Equivalent for buck
converter operating in
CCM with voltage
control
One can show that the control-to-output transfer function is (this assumes RL >> ESR,
normally a very good assumption)
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A. Kruger Lecture 9-15-52Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Error Amplifier in CCM Voltage Control
Purpose of EA is
to provide good
regulation and
good phase
margin to ensure
stability.
435
21
11)(
11
jjj
jj
V
VH
O
CEA
22
5
14
4
33
3
32
2
24
1
11111
CRCRCRCRCR2312 RRCCWith then
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A. Kruger Lecture 9-15-53Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Switching Regulator
435
21
11)(
11
jjj
jj
V
VH
O
CEA
Qj
j
V
V
V
VH z
sm
I
C
OCO
0
2
01
1
COEAHHTOverall loop gain:Qj
j
jjj
jj z
/)/()/(1
/1
11)(
11
0
2
0435
21
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A. Kruger Lecture 9-15-54Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Error Amplifier in CCM Voltage Control
For fast response the crossover frequency fx should be as high as possible. A common
choice is fx ~ fs/5
COEAHHTOverall loop gain:Qj
j
jjj
jj z
/)/()/(1
/1
11)(
11
0
2
0435
21
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A. Kruger Lecture 9-15-55Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Current-Mode Control
Pulse-by pulse current-limiting
Fast transient response
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A. Kruger Lecture 9-15-56Advanced Electronic Circuits 55:036 The University of Iowa, 2009
LT1070 Switching Regulator
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A. Kruger Lecture 9-15-57Advanced Electronic Circuits 55:036 The University of Iowa, 2009
LT1070 Switching Regulator
REFO VR
RV
1
21
Soft start: build up duty cycle
Boost configuration
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A. Kruger Lecture 9-15-58Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Flyback Regulator
Triple-output flyback
regulator
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A. Kruger Lecture 9-15-59Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Switched Capacitor Converters
Also called charge-pump converters
Flying capacitor converters
Generally used for low-power (~ 100 mA or less)
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A. Kruger Lecture 9-15-60Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Switched Capacitor Converters
Non-overlapping switches
Basic Circuit “Flying Capacitor”
Switch frequency 10–100 kHz
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A. Kruger Lecture 9-15-61Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Switched Capacitor Converters
Voltage Inverter
Step 1: Charge C1 to Vin
Step 2: All switches open
With proper
capacitors and
switches, the
inversion
efficiency can be
close to 100%
Step 3: Transfer charge
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A. Kruger Lecture 9-15-62Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Voltage Doubler
Reverse biased =>
can remove from
circuit
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A. Kruger Lecture 9-15-63Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Voltage Doubler
Note, only one set of switches are used. One can put the
other set of switches to generate other voltages
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A. Kruger Lecture 9-15-64Advanced Electronic Circuits 55:036 The University of Iowa, 2009
TC962 Charge Pump
Uncommitted Zener diode
Switches
Oscillator
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A. Kruger Lecture 9-15-65Advanced Electronic Circuits 55:036 The University of Iowa, 2009
TC962 Charge Pump
Uncommitted Zener diode
Switches
Oscillator
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A. Kruger Lecture 9-15-66Advanced Electronic Circuits 55:036 The University of Iowa, 2009
TC962 Charge Pump Oscillator
Charges the capacitors until V+
exceed VREF +VH/2 and the
comparator trips.
The square wave here has a
frequency that depend on the
charge/discharge currents and
capacitor
Discharges the capacitors until
V+ is less than VREF – VH/2 and
the comparator trips.
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A. Kruger Lecture 9-15-67Advanced Electronic Circuits 55:036 The University of Iowa, 2009
TC962 Charge Pump Oscillator
Lowers the frequency
Increases the frequency
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A. Kruger Lecture 9-15-68Advanced Electronic Circuits 55:036 The University of Iowa, 2009
TC962 Charge Pump Oscillator
Can supply one’s own
clock here
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A. Kruger Lecture 9-15-69Advanced Electronic Circuits 55:036 The University of Iowa, 2009
TC962 Charge Pump
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A. Kruger Lecture 9-15-70Advanced Electronic Circuits 55:036 The University of Iowa, 2009
ICL7662
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A. Kruger Lecture 9-15-71Advanced Electronic Circuits 55:036 The University of Iowa, 2009
More Circuits
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A. Kruger Lecture 9-15-72Advanced Electronic Circuits 55:036 The University of Iowa, 2009
More Circuits
Increase output current capacity
Noisy output
NOR gate helps synchronize
switching and reduce output
ripple noise
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A. Kruger Lecture 9-15-73Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Switched Capacitor Building Block
)( 211 VVCfT
qs
Charge transferred each cycle
)1(
)(
1
21
Cf
VVI
s
1
eq
1
CfR
s
Rewriting
eq
21 )(
R
VVI
VCq 1
Charge transferred per unit time is I
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A. Kruger Lecture 9-15-74Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Implementation
The switches are commonly implemented with FETs. While SC ideas have been
around for a long time, moderns IC manufacturing allows for commercially-viable
implementations.
The switched are not ideal and has an “on” resistance of a few Ohms
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A. Kruger Lecture 9-15-75Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Performance
Note that the output is unregulated
Size & characteristics of capacitors?
Output voltage is a function of the load
Switched-capacitor inverter
Thevenin equivalent
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A. Kruger Lecture 9-15-76Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Performance
2
1
142131
1)(2)(2 ESRC
CfESRCRRESRCRRR
pump
SWSWSWSWO
21
1
41
2 ESRCESRCCf
RRpump
SWO
20~RSW
kHz10,F1021 oscfCCExample ESR~RO 550
Pump frequency, and switch resistances depend on temperature and the supply voltage.
?OR
(sum of all switch resistances)
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A. Kruger Lecture 9-15-77Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Performance
Segment A is the voltage drop across the ESR of C2 at the instant it goes from being charged by C1
(current flowing into C2) to being discharged through the load (current flowing out of C2). The
magnitude of this current change is 2IO, hence the total drop is 2IO ×ESRC2 .
2
2
22
1ESRC
CfIV
pump
ORIPPLE
To reduce ripple, increase pump frequency, increase C2 and reduce ESR of C2. ESR of C1 is less
important.
The assumption is that C1 and C2 can charge/discharge during a pump cycle. If they are too big, this
can contribute to the ripple as well.
Segment B is the voltage change across C2 during time t2, the half of the cycle when C2 supplies current
to the load. The drop at B is IOUT × t2/C2 . The peak-to-peak ripple voltage is the sum of these voltages
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A. Kruger Lecture 9-15-78Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Switched-Capacitor Building Block
Assume CA and CB are initially uncharged. When the switch is thrown to (a), CA charges and attains a
charge CAVi. When the switch is thrown to (b) the capacitors are in parallel with value CT = CA+CB, and
charge CAVi on them, so the output voltage after the first cycle is
When the switch is returned to (a), CA again attains a charge CAVi. When the switch is thrown to (b), the
capacitors are in parallel and has a charge and output voltage after the second cycle:
One can see that the output voltage is a geometric series
or
The charge on CB after the first cycle is
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A. Kruger Lecture 9-15-79Advanced Electronic Circuits 55:036 The University of Iowa, 2009
Switched-Capacitor Building Block
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A. Kruger Lecture 9-15-80Advanced Electronic Circuits 55:036 The University of Iowa, 2009