Upload
nicholas-parrish
View
215
Download
0
Embed Size (px)
Citation preview
DC to AC converter (Inverter)
Single phase
Q1
Q2
Vg2
Vg1Vs
C
C
RL
D
D
0.5Vs
0.5Vs
VL
IL
vg1
t
vg2
0 T/2 T
t0 T/2 T
Dead band = 1 μs
t0 T/2 T
Vs/2
-Vs/2
VL, IL
Q1 Q2 Q1
n=∞
vL=Σn=1,3,5,.. (2 Vs) / (nΠ) × sin(nωt)
Vn
n1 2 3 4 5 6 7 8
Harmonic contents in the output voltage
VLrms= Vs / 2
VL1= (2Vs) / (√2Π)
Q1
Q2
Vg2
Vg1Vs
C
C
RL
D1
D2
0.5Vs
0.5Vs
VL
ILLL
Heavily inductive load (RL → 0)
t0 T/2 T
Vs/2
-Vs/2
vL
Q1 Q2 Q1
t
iL
D1 Q1 D2 Q2
R-L load
iL= Σ (2Vs) / [ nΠ √ (R2+n2ω2L2) ] × sin (nωt - Θn)
Θn= tan-1(nωL / R)
Performance Parameters
HFn Harmonic Factor for the nth harmonic
HFn= (VLn) / VL1 for n > 1
THD Total Harmonic Distortion
∞
THD = 1 / VL1 ( Σ V2n ) 0.5
n=2, 3, 4,…
DF Distortion Factor
∞5
DF = 1 / VL1 [ Σ ( VLn / n2 )2 ] 0.5
n=2, 3, …
The Distortion Factor of the nth harmonic = VLn / ( VL1 n2) for n > 1
Lowest Order Harmonic LOH
is the harmonic component that is the closest to the fundamental and its amplitudeIs ≥ 3% of the fundamental
The harmonic voltage Vh
∞
Vh= ( Σ VLn2 ) 0.5 = ( VLrms
2 – VL12 )0.5
n= 3, 5, 7, ..
Vs= 48V R= 2.4 Ω
Calculate:a) The rms value of the load fundamental voltage.b) The output power.c) The average and peak current in the transistor.d) The THD, DF, the HF and DF of the LOH.
a) vL1 = (2Vs) / Π × sin ( ωt)
VL1rms = ( 2 × 48 ) / ( Π × √2 ) = 21.6 V
b) VLrms= 0.5 Vs = 24 V PL= (VLrms)2 / R = 242 / 2.4 = 240 W
c)
iQ1
t0 T/2 T
iQ2
t0 T/2 TPeak current in each transistor = 24/2.4 = 10A
Average current in each transistor = 5 A
d) Vh= ( 242 – 21.62 )0.5 = 10.46 V THD = 10.46 / 21.6 = 0.4843
VL3= 21.6/3 = 7.2 VVL5= 21.6/5 = 4.32 VVL7= 21.6/7 = 3.086 V
DF = 1/21.6 ×{ [ 7.2/32]2+ [4.32/52]2
+[3.086/72] 2}0.5 = 1/21.6 ×{ 0.64 + 0.02986 +0.004+ .. }0.5
= 0.038
Q1
Q2
Vg2
Vg1Vs
C
C
RL
D1
D2
0.5Vs
0.5Vs
VL
ILLL
The LOH = 3rd harmonic
HF3= 1/3 = 0.3333
DF3= 0.3333/32 = 0.03703 note that VL3= 0.3333 which is > 0.03 so LOH =3
The H-bridge single phase inverterVg1, Vg2
t
Vg3, Vg4
0 T/2 T
t0 T/2 T
Dead band = 1 μs
t0 T/2 T
Vs
-Vs
VL, IL
Q1, Q2 Q3, Q4
n=∞
vL=Σn=1,3,5,.. (4 Vs) / (nΠ) × sin(nωt)
Vn
n1 2 3 4 5 6 7 8
Harmonic contents in the output voltage
VLrms= Vs
VL1= (4Vs) / (√2Π)
Q3
Q2
Vg2
Vg3Vs
RL
D
DVL
IL
Q1
Q4
Vg1
Vg4
D
D
Q1, Q2
Vs= 48V R= 2.4 Ω
Calculate:a) The rms value of the load fundamental voltage.b) The output power.c) The average and peak current in the transistor.d) The THD, DF, the HF and DF of the LOH.
a) vL1 = (4Vs) / Π × sin ( ωt)
VL1rms = ( 4 × 48 ) / ( Π × √2 ) = 43.2 V
b) VLrms= Vs = 48 V PL= (VLrms)2 / R = 482 / 2.4 = 960 W
c)
iQ1, iQ2
t0 T/2 T
iQ3, iQ4
t0 T/2 TPeak current in each transistor = 48/2.4 = 20A
Average current in each transistor =10 A
d) Vh= (482 – 43.22 )0.5 = 20.92 V THD = 20.92 / 43.2 = 0.4843 (same)
VL3= 43.2/3 = 14.4 VVL5= 43.2/5 = 8.64 VVL7= 43.2/7 = 6.17 V
DF = 1/43.2 ×{ [ 14.4/32]2+ [8.64/52]2
+[6.17/72] 2}0.5
= 1/43.2 ×{ 1.6 + .3456 +0.1259+ .. }0.5
= 0.033 (same)
Q3
Q2
Vg2
Vg3Vs
RL
D
DVL
IL
Q1
Q4
Vg1
Vg4
D
D
LOH = 3rd harmonic
HF3 = 1/3
DF3= 1/(3×32) = 0.03703 (same) note that VL3= 14.4 which is > 0.03×VL1 so LOH =3
The quality of the output voltage is the same as for the 2-transistor circuit however,the H bridge inverter the output power is 4 times higher and the fundamental output Voltage is twice that of the 2-transistor circuit.
The H-bridge inverter shown in figure has anRLC load with R=10Ω, L=31.5mH, C=112μF.The inverter frequency is 60 Hz and the dc inputVoltage is Vs=220V.a) Express the instantaneous load current in Fourrier series.b) Calculate the rms load current at the fundamental frequency.c) Calculate the THD of the load current. d) Calculate the total power absorbed by the load as well as the fundamental power.e) Calculate the average dc current drawn from the supply.f) Calculate the rms and the peak current of each transistor.
Q3
Q2
Vg2
Vg3Vs
RD
DVL
IL
Q1
Q4
Vg1
Vg4
D
D
L C
Three-phase inverters120o conduction
180o conduction
120o conduction
Vs
Q1
Q4
Vg1
Vg4
D1
D4
a
Q3
Q6
Vg3
Vg6
D3
D6
b
Q5
Q2
Vg5
Vg2
D5
D2
c
R
R
R
a
b
c
@ any time only 2 transistors are conducting: 1 in an upper leg 1 in another lower leg
ωt60o
ωt60o
vG1
vG2
ωt60o
vG3
ωt60o
vG4
ωt60o
vG5
ωt60o
vG6
For 0 ≤ ωt < 60o
R
R
R
Vs
a
b
c
For 60o ≤ ωt < 120o
R
R
R
Vs
a
b
c
For 120o ≤ ωt < 180o
R
R
RVs
a
b
c
For 180o ≤ ωt < 240o
R
R
R
Vs
a
b
c
n’ n’ n’
n’
For 240o ≤ ωt < 300o
R
R
R
Vs
a
b
c
n’
For 300o ≤ ωt < 360o
R
R
RVs
a
b
c
n’
ωt60o
ωt60o
vab
vbc
ωt60o
vca
ωt60o
van’
ωt60o
vbn’
ωt60o
Vcn’
CV
CV CV
CV CV
CV CV
CV
Vs
0.5Vs
- 0.5Vs
-Vs
0.5Vs
-0.5Vs
ωt60o
ωt60o
vG1
vG2
ωt60o
vG3
ωt60o
vG4
ωt60o
vG5
ωt60o
vG6
180o conduction ( 3 transistors are conducting at any time)
For 0 ≤ ωt < 60o For 60o ≤ ωt < 120o For 120o ≤ ωt < 180o
For 180o ≤ ωt < 240o For 240o ≤ ωt < 300o
R
R
Vs
R a
b
c
n’
For 300o ≤ ωt < 360o
R
R
Vs
a
R b
cn’
R
Vs
a
R bR c
n’
R
Vs
aRb
R
c
n’
R
Vs
a
Rb
R
c
n’
Vs
R
R
Ra
bc
n’
R
ωt60o
ωt60o
vab
vbc
ωt60o
vca
ωt60o
van’
ωt60o
vbn’
ωt60o
Vcn’
CV
CV
Vs
-Vs
CV
CV
⅓Vs
⅔Vs
Voltage control techniques of single phase inverters
Single pulse width modulation
0Π 2Π
ωt
VL
Π/2
3Π/2
δ
δ
-Vs
Vs
vL= Σn=1,3,5,.. (4Vs / nΠ) sin(nδ/2) sin(nωt) ∞
VLrms= Vs √(δ/Π)
Multiple pulse width modulation
0 Π 2Π
ωt
VL
Π/2
3Π/2
-Vs
Vs
Π/3 2Π/3Π/6 5Π/6
δδ
δ
7Π/6 11Π/6
4Π/3 5Π/3
P= # of pulses per half cycleP=3
δ δδ
Decreases DF significantly
αm=2
vL= Σn=1, 3, ..Σm=1{4Vs /(nΠ) sin{ nδ/4 [ sin n(αm+3δ/4) – sin n(Π+αm+δ/4) ] }× sin(nωt)∞ 2p
VLrms= Vs √ (pδ/Π)
δ = M T/ (2p) Where M is the amplitude modulation index 0 ≤ M ≤ 1
Sinusoidal Pulse Width Modulation
Carrier waveform
Reference waveform
Ar
Ac
MA = Amplitude Modulation Index
Ar
MA = _______
Ac
MF = Frequency Modulation Index
carrier frequencyMF = --------------------------- (= 5) reference frequency
fC = carrier frequency
fR = reference frequency
0 ≤ MA ≤ 1
If MA > 1 over-modulation
ωt
ωt
-Vs
α1 α2
180o- α1
180o – α2
Vs
if MF is an odd number, quarter-wave symmetryis obtained and no even harmonics are presentin the output voltage.
For a 3-phase inverter, MF should be an oddtriplen number
SPWM reduces greatly the DF
MA0
U1
0 1
<1
over-modulation