Power Electronic project
reference notes/455647_1_EE460-Project-131.pdf
King Fahd University of Petroleum and Minerals
Department of Electrical Engineering
EE Power Electronics Project
Design of a DC Chopper
I. Design of an AC/DC converter with the following the specifications:
AC supply voltage VS = 230 V (rms), 60 Hz.
The DC output voltage V01(dc) = 48 V.
The ripple factor of the output voltage RFV 5%.
II. Design of step-down DC chopper with the following specifications:
Switching (or chopping) frequency, fs = 20 kHz.
Dc input supply voltage VS = 48 V dc, where as the source available is an ac with 230 V
(rms).
Load resistance R = 5 .
The DC output voltage V02(dc) = 12 V.
The peak-to-peak output ripple voltage, VC 2.5%.
The peak-to-peak inductor ripples current, IL 5%.
III. Calculation for both circuits:
(a) Determine the values of Le and Ce for the output LC-filter.
(b) Determine the (peak and rms) voltage ratings and the (average, rms, and the peak) current for
all components and devices.
(c) Verify your design calculation by using Pspice simulation.
Design AC/DC
Circuit
Design DC-DC
Chopper Circuit AC 5
Output Load
The project will be due on Sunday December 22, 2013.
reference notes/455647_2_DC-20Converters-Design (1).pdf
....-ju"ncv
O.
214 Chapter 5 Dc-Dc Converters
Example 5.10 A buck converter is shown in Figure 5.29. The input voltage is V, == 110 V, the average load age is Va == 60 V, and the average load current is la == 20 A. The chopping u
1 == 20 kHz. The peak-to-peak ripples are 2.5% for load voltage, 5% for load current, and for filter Le current. (a) Determine the values of L" L, and Ceo Use PSpice (b) to verify the suits by plotting the instantaneous capacitor voltage vc, and instantaneous load current iL;
(c) to calculate the Fourier coefficients and the input current is. The SPICE model pax'ameters the transistor are IS == 6.734f, BF = 416.4, BR == 0.7371, CJC == 3.638P, CJE:: TR == 239.5N, TF = 30L2P, and that ofthe diode are IS :: 2.2E-15, BV = 1800V, IT ==
Solution
V, = 110 V, va = 60 V, I. == 20 A. ay: == 0.025 x Va = 0.025 x 60 = 1.5 V
Va 60 R==-=-=311
10 20
From Eq. (5.48),
Va 60 k = - = - = 05455V, 110 .
From Eq. (5.49),
Is = kla = 0.5455 x 20 == 10.91 A
alL = 0.05 x I. :: 0.05 x 20 == 1 A
M = 0.1 x 10 == 0.1 x 20 == 2 A
8. From Eq. (5.51), we get the value of L.:
VaWs - Va) 60 X (110 - 60) Le = MIV, = 2 x 20 kHz x 110 = 681.82 ~H
From Eq. (5.53) we get the value of Ce:
2c == ,11 e ,lV, X 81 1.5 x 8 X 20 kHz == 8.33 ~F
L4
+
+ Vs 110 V
FIGURE 5.29 o~-----------+----------~--------~Buck converter.
5.12 Chopper Circuit Design 215
Vs
L 8
v, OV
O~----------------------------*-------~~------~ (a) Circuit
Vgj
2ov~______________1~________-L____--'
o 27.28 IlS SOIlS
(b) Control voltage
FIGURE 5.30
Buck chopper for PSpice simulation.
Assuming a linear rise of load current iL during the time from t = 0 to tl = kT, we can write approximately
Ah Ah L- = L-- = AVe
t} kT
which gives the approximate value of L:
kTAVc kAVe L=~= AIJ
(5.128)
0.5454 X 1.5 = 40.91 H 1 X 20kHz f.L
b. k = 0.5455, / = 20 kHz, T = 11/ = 50 f.LS, and ton = k X T = 27.28 f.LS. The buck chopper for PSpice simulation is shown in Figure 5.30a. The control voltage Vg is shown in Figure 5.30b. The list of the circuit file is as follows:
Example 5.10 Buck Converter
vs 1 0 IX: 110V
VY 1 2 IX: OV ; Voltage source to measure input current
Vg 7 3 PULSE (OV 20V 0 O.1NS 0.1NS 27.28US 50US)
RB 7 6 250 ; Transistor base resistance
LE 3 4 681. 8200
216 Chapter 5 Dc-Dc Converters
CE
L
R
VX
J:M
4
4
8
5
o
o 8
5
o 3
8.33UF
40.91UH
3
rx:: DMOD
IC=60V initial voltage
; Voltage source to measure load Cll:rr••" ..
Freewheeling diode
.MODEL DMOD D(IS=2.2E-15 BV=1800V TT=O) ; Diode model parameters
Q1 2 6 3 QMOD ; BJ'1' switch
.MODEL QMOD NPN (IS=6.734F BF=416.4 BR=.7371 CJC=3.638P
+ CJE=4.493P TR=239.5N TF=301.2P) BJ'1' model parameters
•'!'RAN 1US 1. 6M3 1. 5M3 1US UIC ; Transient analysis
. PROBE ; Graphics postprocessor
.options abstol = 1.00n reltol = 0.01 vntol 0.1 ITL5=50000 ; convergence
.FOUR 20KHZ I(VY) ; Fourier analysis
•END
The PSpice plots are shown in Figure 5.31, where I(VX) = load I (Le) = inductor L, current, and V (4) = capacitor voltage. Using the PSpice in Figure 5.31 gives v" = Vc = 59.462 V, <1v,. = 1.782 V, M = 2.029 A, I(av)
19.813 A, <1h = 0.3278 A, and fa = 19.8249 A. This verifies the design; however, gives a better result than expected.
Example 5.10 A Buck Converter Temperature: 27.0
80.0V +_------_+------+_------_+_------+_----_+
6O.0V i-------------------"'-----------+
40.0 V +_----_+-----+_-------_+_--------+_------_+ o V (4)
20.0 A +_----_+------+_----_+_------+_----_+
19.6 A +_----_+-----+_----_+_-----+_----_+ 01 (VX)
~.OA+_----_+-----+_----_+_-----+_----_+
20.0 A 1------------------------------1 O.OA +_----_+-------+_--------+---------+_----_+
1.50 ms 1.52 ms 1.54 ms 1.56 ms 1.58 ms 1.60 ms o I (te)
TIme
FIGURE 5.31
PSpice plots for Example 5.10.
5.13 State-Space Analysis of Regulators 217
c. The Fourier coefficients of the input current are
FOURIER COMPONENTS OF TRANSIENT RESPONSE I (VY)
DC COMPONENT = 1.079535E+Ol
HARMONIC FREQUENC'f FOURIER NORMALIZED PHASE NORMALIZED m (HZ) COMPONENT COMPONENT (DEG) PHASE (DEG)
1 2.000E+04 1.251E+Ol 1.OOOE+OO -1.195E+Ol O.OOOE+OO 2 4.000E+04 1.769E+OO 1. 415E-Ol 7.969E+01 9.163E+Ol
3 6.000E+04 3.848E+OO 3.076E-Ol -3.131E+01 -1. 937E+Ol
4 8.000E+04 1. 686E+OO 1.348E-Ol 5.500E+01 6.695E+Ol
5 1. OOOE+05 1.939E+OO 1. 551E-01 -S.187E+Ol -3.992E+01
6 1.200E+OS 1.S77E+OO 1.261E-01 3.347E+01 4.S42E+01
7 1.400E+OS 1.014E+OO 8.107E-02 -7.328E+Ol -6.133E+Ol
8 1.600E+OS 1. 43SE+OO 1.147E-Ol 1.271E+Ol 2.466E+01
9 1.800E+OS 4.38SE-Ol 3.506E-02 -9.751E+Ol -8.S56E+01
TOTAL HARMONIC DISTORTION = 4.401661E+Ol PERCENT
Key Points of Section 5.12
• The design of a dc-dc converter circuit requires (1) determining the converter topology, (2) finding the voltage and currents of the switching devices, (3) finding the values and ratings of passive elements such as capacitors and inductors, and (4) choosing the control strategy and the gating algorithm to obtain the desired output.
5.13 STATE-SPACE ANALYSIS OF REGULATORS
Any nth order linear or nonlinear differential equation in one time-dependent variable can be written [26] as n first-order differential equation in n time-dependent variables Xl through Xn• Let us consider, for example, the following third-order equation:
(5.129)
where y' is the first derivative of y, y' = (dldt) y. Let y be Xl' Then Eq. (5.129) can be represented by the three equations
Xl' = X2 (5.130)
X2" = X3 (5.131)
X3" = -aOxl - alxZ - a3x3 (5.132)
In each case, n initial conditions must be known before an exact solution can be found. For any nth-order system, a set of n-independent variables is necessary and sufficient to describe that system completely. These variables Xl> X2, ... , Xn• are called the state variables for the system. If the initial conditions of a linear system are known at time to, then we can find the states of the systems for all time t > to and for a given set of input sources.
reference notes/455647_3_dc-dc-20step-20down-20converter.pdf
DC-DC Step-Down Converter
Dr. Mahmoud Kassas
Electrical Engineering Dept.
King Fahd University of Petroleum & Minerals
Dhahran, Saudi Arabia
reference notes/455647_4_Filter-20Design-20Diode.pdf
1
3.10 Rectifier Circuit Design:
Objectives: • Learn about Design Specifications • Become familiar with C-Filter Design • Learn about LC-Filter Design
2
The design of a rectifier involves determining the rating of semiconductor diodes. Rating specification in terms of:
• Average current • RMS current • Peak current • PIV "peak inverse voltage"
Design Specifications
3
• The output of the rectifiers contains harmonics.
• Filters can be used to smooth out the dc output voltage.
R
Le
+
-
V0VL
+
-
L-Filter
R
+
-
V0VL
+
-
C-Filter
Ce R
Le
+
-
V0VL
+
-
LC-Filter
Ce
filters:-DC
filters:-AC
Li
+
-
VLVs
+
-
LC-Filter
Ci Rectifier
4
Full-bridge Rectifier 120 V (rms), 60 Hz R = 500 Ω
• Design C-filter so that RF = 5% (Ripple- factor).
• With the value of C calculate Vdc.
5
Charging of capacitor When the instantaneous voltage vs is higher than the capacitor voltage vc, diodes D1 and D2 or D3 and D4 conduct supply voltage thereby charging the capacitor. Discharging of capacitor When the instantaneous supply voltage vs falls below the instantaneous capacitor voltage vc diodes D1 and D2 or D3 and D4 are reverse biased and the capacitor discharges through the load resistor. The capacitor voltage varies between Vcmin and Vcmax and this is known as the output ripple voltage. The output voltage waveforms and equivalent circuit on charging and discharging are shown below.
6
Equivalent Circuit:
0)0(1 =+=′+∫ LcL
e
RItVdtI C
eRC t
m LmC e
R VIVtV
−
=⇒==′ )0( eRC t
mLL eVIRV −
=⋅=
The capacitor discharges exponentially through R.
7
eRC t
mmppr
LLppr
eVVV
ttVttVV 2
)(
21)( )()( −
−
−
−=
=−==
⇒−≅− ,1 xe x
)1( 2 )(
e mmppr RC
t VVV −−≅−
2)( t RC V
V e
m ppr ≅−
f T
2 1
2 =≅
e
m ppr fRC
V V
2)( ≅∴ −
− =−=−= −
e
e m
e
m mpprmdc fRC
fRCV fRC VVVVV
4 14
42 1
)(
The peak-to-peak ripple voltage can be found from
Since x << 1
If t2
8
22 )( ppr
ac
V V −≅
( )142 1
4 14
24 −
=
− ==∴
e
e
e m
e
m
dc
ac
fRC fRC
fRC V
fRC V
V V
RF
F RFRf
Ce µ2.126 2 11
4 1
=
+
⋅ =
49.158=dcV
Thus the rms output ripple voltage
V
9
( )
∫∫
∑ ===
++= ∞
=
ππ
π ωω
π ω
π
ωω
00
1
2.sin 2 2.)(
2 1
sincos
VVtdtVtdtVV
tnbtnaVV
m mLdc
n nndcL
[ ]
+ +−
+ −
+−− =
+ +−
+ −
+−− =
++−=
=
==
∫
∫
∫∫
n n
n nVa
n tn
n nVa
tdtntnVa
tdtntVa
tdtntVtdtnVa
m n
m n
m n
m n
mLn
1 )1cos(
1 1)1cos(
1 )1cos(
1 1)1cos(
)1sin()1sin(
.cos.sin2
.cos.sin2.cos1
0
0
0
0
2
0
ππ π
ωπ π
ωωω π
ωωω π
ωωω π
ωω π
π
π
π
ππ
Obtain Fourier series for RL-Load:
10
( )( )11 14 +−
−+ =
nn V
a m n π
( )( ) [ ] ( )( )
( ) ( ) ( )( )
( )( ) ( )( )11 4
11 4
11 )1cos()1cos(2)1cos()1cos(
11 )1(1)1cos(11)1cos(
+− −
= −+
=
+− ++−−+++−−−
=
+− −++−+++−−
=
nnnn
nn nnnnn
nn nnnn
ππππ
ππ
For n = 1, 3, 5,…………… an = 0 For n = 0, 2, 4,……………………..
Details:
11
)223(............6cos 35 44cos
15 42cos
3 42
cos. )1)(1(
142
0.sin.sin2.sin1
4,2
2
0 0
−−−−=
+− −
+=∴
===
∑
∫ ∫
∞
=
EqntVtVtVVV
tn nn
VVV
tdtntVtdtnVb
mmmm L
n mm
L
mLn
ω π
ω π
ω ππ
ω ππ
ωωω π
ωω π
π π
12
LC-Filter (output) • Load resistance R = 40 Ω & Load inductance
L = 10 mH f = 60 Hz RF = 10% Equivalent circuit for harmonic is:
13
To make it easier for the nth harmonic ripple current to pass through the filter capacitor, the load impedance must be much greater than that of the capacitor impedance. This condition is generally satisfied by: 10 times
eCn LnR
ω ω 1)( 22 >>+
eCn LnR
ω ω 10)( 22 =+
14
n ee
n
e e
e on V
CLn V
Cn Ln
CnV 1)(
1 1
1
2 − −
= −
− =
ω ω
ω
ω
2 1
2
6,4,2
= ∑∞
= onnac VV
Under this condition the effect of the load is negligible (Voltage divider)
The total amount of ripple voltage due to all harmonics is:
15
π23 4
2 mV
V = π
m dc
V V
2 =
2202 1)2( 1 V CL
VV ee
ac − −
== ω
( ) mHL
CLfV V
V V
V VRF
FC C
LnR
e
eedcdc
o
dc
ac
e
e
83.30
1.0 14
1 326
2 10)(
2 22
22
=∴
= −
===
=
=+
π
µ ω
ω
From Eqn (3-22) we find that the second harmonic is the dominant one & its rms
&
For n = 2,
- 3.10 Rectifier Circuit Design:
- Slide Number 2
- Slide Number 3
- Full-bridge Rectifier 120 V (rms), 60 Hz R = 500 Ω
- Slide Number 5
- Equivalent Circuit:
- Slide Number 7
- Slide Number 8
- Slide Number 9
- Slide Number 10
- Slide Number 11
- LC-Filter (output)
- To make it easier for the nth harmonic ripple current to pass through the filter capacitor, the load impedance must be much greater than that of the capacitor impedance.���This condition is generally satisfied by:� 10 times
- Slide Number 14
- Slide Number 15