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EEL 3923C JD/ Module 2 Power Supply Design & Construction
Prof. T. Nishida���Fall 2010
2 EEL 3923C, Fall 2010, T. Nishida
II. General Power Supply • Converts ac powerline voltage into DC voltage of
required magnitude and stability for the electronic system
Diode Rectifier Filter Voltage
Regulator
120 V(rms) 60 Hz ac line input
Ref: Section 3.5, Sedra and Smith, Microelectronic Circuits, 5th Ed., Oxford, 2004.
3 EEL 3923C, Fall 2010, T. Nishida
General Power Supply Design • Useful reference on power supply design
Ref: http://www.st.com/stonline/books/pdf/docs/1707.pdf
4 EEL 3923C, Fall 2010, T. Nishida
II.1 Transformer • Ideal loss-less transformer
– No dissipation
– Voltage step-up/down determined ratio of coil turns on secondary/primary
– Current has inverse ratio
– Impedance transformation Ref: http://www.mpdigest.com/issue/Articles/2009/oct/Mini/Default.asp
5 EEL 3923C, Fall 2010, T. Nishida
Real Transformer • Real transformer
– Series resistance in windings, Rs, Rp – Stray leakage inductance, Xs, Xp – Core losses
• Eddy current, Rc • Magnetization, Xm
6 EEL 3923C, Fall 2010, T. Nishida
Module 2 Transformer Specs • EI30 series laminated transformer
Ref: http://ww2.pulseeng.com/products/datasheets/LT2010.pdf
7 EEL 3923C, Fall 2010, T. Nishida
LT SPICE Transformer Model
Ref: h'p://ltspice.linear.com/so5ware/scad3.pdf
8 EEL 3923C, Fall 2010, T. Nishida
Module 2 Transformer LTSPICE Model • 8:1 transformer with series resistance • Output voltage depends on load current
File: Module2_Transformer_+_RL.asc
9 EEL 3923C, Fall 2010, T. Nishida
Module 2 Transformer Implementation • Sealed case, switch, LED power indicator, and
fuse for safety (supplied in JD lab)
10 EEL 3923C, Fall 2010, T. Nishida
II.2 Diode Rectifier • Purpose: Convert ac transformer output
into waveform with non-zero DC component
• What is DC component?
11 EEL 3923C, Fall 2010, T. Nishida
P/N Junction Rectifier Diode • I-V characteristics
• Equivalent circuit
i
v
Reverse bias Forward bias
12 EEL 3923C, Fall 2010, T. Nishida
General Purpose Rectifier Diodes • Module 2 diode
Ref: http://www.fairchildsemi.com/ds/1N%2F1N4001.pdf
13 EEL 3923C, Fall 2010, T. Nishida
Module 2 Diode LTSPICE Model • Add 1N4004 diode model to LTSPICE diode model library
– Navigate to C:\Program Files\LTC\LTspiceIV\lib\cmp – Open standard.dio using notepad or by double-clicking and using LTSPICE – Insert the following into the file
.MODEL 1N4004 D(IS = 3.699E-09 RS = 1.756E-02 N = 1.774 XTI = 3.0 EG = 1.110 CJO = 1.732E-11 M = 0.3353 VJ = 0.3905 FC = 0.5 ISR = 6.665E-10 NR = 2.103 BV = 400 IBV = 1.0E-03 Iave=1000m Vpk=400 mfg=Fairchild type=silicon)
– Close and restart LTSPICE • Insert a generic diode into your schematic • Right-click the diode; you should see a dialog box
– Click ‘Pick New Diode’ – Select 1N4004 from the list of possible diodes – The diode should now look like:
Ref: http://www.fairchildsemi.com/models/PSPICE/Discrete/Diode.html
14 EEL 3923C, Fall 2010, T. Nishida
Half Wave Rectifier • Circuit (LTSPICE)
15 EEL 3923C, Fall 2010, T. Nishida
Half Wave Rectifier • Equivalent circuit using constant voltage model
• Effect of forward voltage drop
• Peak inverse voltage
16 EEL 3923C, Fall 2010, T. Nishida
Full Wave Rectifier • Disadvantages of half-bridge rectifier: maximum conduction angle
of 180º • Possible fixes:
• Use two half-bridge rectifiers (basic concept of center-tapped transformer approach)
• Bridge rectifier (similar to Wheatstone bridge circuit)
17 EEL 3923C, Fall 2010, T. Nishida
Full Wave Rectifier • Center-tapped transformer approach
Ref. Sedra & Smith, Fig. 3.26
vS(t), vO(t)
t
Note: Effect of VD drop.
PIV=2VS-VD
Where are the half-bridge rectifiers?
18 EEL 3923C, Fall 2010, T. Nishida
Full Wave Rectifier • Bridge rectifier approach
vS(t), vO(t)
t
Ref. Sedra & Smith, Fig. 3.27
PIV=VS-VD
What is the voltage drop?
(a) Positive half-cycle
Which diodes are forward-biased?
(b) Negative half-cycle
19 EEL 3923C, Fall 2010, T. Nishida
Module 2 Full Wave Rectifier • Note the importance of the ground reference
20 EEL 3923C, Fall 2010, T. Nishida
II.3 Filter • Purpose: Reduce voltage ripple
• Need shunt capacitor to pass DC and filter ac frequencies
21 EEL 3923C, Fall 2010, T. Nishida
Half Wave Rectifier With Filter Cap • Goal: First order
smoothing of output • Approach: Filter
capacitor • Assume capacitor
initially uncharged, vC(t=0)=0V
• Assume ideal diode for simplicity (i.e. neglect VD drop)
vS(t), vO(t)
t
T Vr
22 EEL 3923C, Fall 2010, T. Nishida
Half Wave Rectifier With Filter Cap • Approximate Analysis C charges up from t=0 to t=T/4 iD=iC+iL
where iL=vO/R and iC=Cdvs/dt
Diode turns off at peak. Why? vO(t=T/4) =VSpeak C discharges through R delivering load
current.
vO=VSpeake-t/RC Stops discharging when vO(t) less than vs
(t).
vO(t)
t vS (t)
23 EEL 3923C, Fall 2010, T. Nishida
Half Wave Rectifier With Filter Cap • Approximate Analysis
Define ripple voltage, Vr: VSpeak-Vr ≅VSpeake-T/R
LC
Assuming CR>>T,
Vr ≅ VSpeak(T/RLC) Vr ≅VO (T/C)(IL/VO) 0.05VO ≅ IL T/C
• Similar analysis for full wave rectifier with filter capacitor • What changes?
vS(t), vO(t)
t
T Vr
24 EEL 3923C, Fall 2010, T. Nishida
Capacitors Types Capacitor types Capacitance range Accuracy
Temperature stability
Leakage Comments
ElectrolyHc 0.1 µF -‐ ~1 F V poor V poor Poor Polarised capacitor -‐ widely used in power supplies for smoothing, and bypass where accuracy, etc is not required.
Ceramic 10 pF -‐ 1 µF Variable Variable Average Exact performance of capacitor depends to a large extent on the ceramic used.
Tantalum 0.1 µF -‐ 500 µF Poor Poor Poor Polarised capacitor -‐ very high capacitance density.
Silver mica 1 pF -‐ 3000 pF Good Good Good Rather expensive and large -‐ not widely used these days except when small value accurate capacitors are needed.
Polyester (Mylar)
0.001 µF -‐ 50 µF Good Poor Good Inexpensive, and popular for non-‐demanding applica@ons.
Polystyrene 10 pF -‐ 1 µF V good Good V good High quality, oBen used in filters and the like where accuracy is needed.
Polycarbonate 100 pF -‐ 20 µF V good V good Good Used in many high tolerance and hash environmental condi@ons. Supply now restricted.
Polypropylene 100pF -‐ 50 µF V good Good V good High performance and low dielectric absorp@on.
Teflon 100 pF -‐ 1 µF V good V v good V v good High performance -‐ lowest dielectric absorp@on.
Glass 10 pF -‐ 1000 pF Good Good V good Excellent for very harsh environments while offering good stability. Very expensive.
Porcelain 100 pF -‐ 0.1 µF Good Good Good Good long term stability
Vacuum and air 1 pF -‐ 10 000 pF OBen used as variable capacitors in transmiKers as a result of their very high voltage capability.
Ref: h'p://www.radio-‐electronics.com/info/data/capacitor/capacitor_types.php
25 EEL 3923C, Fall 2010, T. Nishida
Capacitor Applications ApplicaHon Suitable types Reasons
Power supply smoothing Aluminium electrolyHc High capacity, high ripple current
Audio frequency coupling
Aluminium electrolyHc
Tantalum
Polyester / polycarbonate
High capacitance
High capacitance, small size
Cheap, but values not as high as electrolyHcs
RF coupling
Ceramic COG
Ceramic X7R
Polystyrene
Small, cheap, low loss
Small cheap, but higher loss than COG
Very low loss, but larger than ceramic
RF decoupling
Ceramic COG
Ceramic X7R
Small, low loss. Values limited to around 1000 pF
Small, low loss, higher values available than for COG types
Tuned circuits Silver mica
Ceramic COG
Close tolerance, low loss
Close tolerance, low loss, although not as good as silver mica
Ref: h'p://www.radio-‐electronics.com/info/data/capacitor/capacitor_types.php
26 EEL 3923C, Fall 2010, T. Nishida
Module 2 LTSPICE Simulation Half Wave with Filter Cap
• Caution: Make sure + terminal of electrolytic capacitor is connected to positive secondary voltage lead
• Select standard value capacitance by right-clicking capacitor
27 EEL 3923C, Fall 2010, T. Nishida
Module 2 LTSPICE Simulation Half Wave with Filter Cap
• Note: Need to simulate long enough to reach steady-state – Start to save data after steady-state is reached
28 EEL 3923C, Fall 2010, T. Nishida
Module 2 LTSPICE Simulation Half Wave with Filter Cap
• Note: Positive current defined down in RL • Calculate percent ripple in output voltage
– Percent ripple = 100(Vr /VOmax )
29 EEL 3923C, Fall 2010, T. Nishida
Module 2 LTSPICE Simulation Full Wave with Filter Cap
• Caution: Make sure + terminal of electrolytic capacitor is connected to positive secondary voltage lead
30 EEL 3923C, Fall 2010, T. Nishida
II.4 Regulator • Purpose: Active circuit to achieve nearly
constant output voltage up to a max load current
• Approaches – Open-circuit
• Zener diode – Closed-circuit
• Op-amp, transistor • Specialized regulator ICs
31 EEL 3923C, Fall 2010, T. Nishida
Operation at Reverse Breakdown—���Zener Diodes
• Operation at reverse bias • Define VZ and IZ with opposite polarity
• Circuit symbol
• I-V characteristic
i
v -VZ -VZK
-IZK
-IZT
Figure 3.21, Sedra & Smith
32 EEL 3923C, Fall 2010, T. Nishida
Zener Diodes • Parameters: Identify on I-V characteristic
• Q point (i=IZT and v=VZ) • Zz= incremental resistance (slope = 1/Zz) • ΔV=Zz Δ I • IZK = minimum reverse current for operation in breakdown
region • Equivalent circuit (piece-wise linear)
• VZ = VZ0 + ZzIZ for IZ > IZK
+ VZ _
33 EEL 3923C, Fall 2010, T. Nishida
Zener Shunt Regulator • Zener diode placed in parallel with load (shunt)
Ref: http://www.st.com/stonline/books/pdf/docs/1707.pdf
34 EEL 3923C, Fall 2010, T. Nishida
Zener Shunt Regulator • Line regulation: Defined as change in output voltage, VO
for change in line voltage, V+, for no load • ΔVO=(rz/(rz+R)) ΔV+
• What is the effect of connecting a load? • Load regulation: Defined as ΔVo per 1mA when RL
chosen to draw IL=1mA • If ΔIL=+1mA, what is ΔIZ? • Effect of ΔIZ on ΔVO? Check zener I-V curve. • ΔVO = Zz ΔIZ
• What limits the lowest RL for the shunt regulator?
35 EEL 3923C, Fall 2010, T. Nishida
1N4728A – 1N4758A Zener Diodes
Ref: http://www.fairchildsemi.com/ds/1N%2F1N4745A.pdf
36 EEL 3923C, Fall 2010, T. Nishida
Module 2 Zener Diode LTSPICE Model • Add 1N4733A zener diode model to LTSPICE diode model library
– Navigate to C:\Program Files\LTC\LTspiceIV\lib\cmp – Open standard.dio using notepad or by double-clicking and using LTSPICE – Insert the following into the file
* 1N4733 * Motorola 5.1V 1W Si Zener pkg:DO-41 1,2 .MODEL 1N4733 D(IS=7.03E-16 RS=0.871 TT=5.01E-8 CJO=1.89E-10 VJ=0.75 M=0.33
BV=5.059 IBV=0.049 Vpk=5.1 mfg=Fairchild type=zener)
– Close and restart LTSPICE • Insert a generic diode into your schematic • Right-click the diode; you should see a dialog box
– Click ‘Pick New Diode’ – Select 1N4733 zener diode from the list of possible diodes – The zener diode should now look like:
Ref: http://www.duncanamps.com/spice/diodes/zener.mod
37 EEL 3923C, Fall 2010, T. Nishida
Module 2 Zener LTSPICE Model • Zener diode placed in parallel with load (shunt)
Ref: http://www.st.com/stonline/books/pdf/docs/1707.pdf
38 EEL 3923C, Fall 2010, T. Nishida
LM2940 Low Dropout Pos Regulator
Ref: http://www.national.com/ds/LM/LM2940.pdf
39 EEL 3923C, Fall 2010, T. Nishida
LM2940 Low Dropout Pos Regulator
Ref: http://www.national.com/ds/LM/LM2940.pdf
40 EEL 3923C, Fall 2010, T. Nishida
LT1086 Low Dropout Pos Regulator
Ref: h'p://cds.linear.com/docs/Datasheet/1086ffs.pdf
41 EEL 3923C, Fall 2010, T. Nishida
LT1086 Low Dropout Pos Regulator
Ref: h'p://cds.linear.com/docs/Datasheet/1086ffs.pdf
42 EEL 3923C, Fall 2010, T. Nishida
LM2940 Standard Pos Regulator
Ref: http://www.fairchildsemi.com/ds/LM/LM7805.pdf
43 EEL 3923C, Fall 2010, T. Nishida
LM3940 Regulator 5V to 3.3V Converter
Ref: http://www.national.com/ds/LM/LM3940.pdf