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![Page 1: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/1.jpg)
Diode Circuits or Uncontrolled Rectifier
Rectification: The process
of converting the alternating voltages and currents to
direct currents
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The main disadvantages of half wave rectifier are:
• High ripple factor, • Low rectification efficiency, • Low transformer utilization
factor, and, • DC saturation of transformer
secondary winding.
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Performance Parameters
22dcrmsac VVV −=
acdc PP /=η rectification effeciency
dcrms VVFF /=
11 22
222
−=−=−
== FFVV
VVV
VVRF
dc
rms
dc
dcrms
dc
ac
form factor
ripple factor
![Page 4: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/4.jpg)
121
2
21
21
2−=
−=
S
S
S
SSi
II
IIITHD
121
2
21
21
2−=
−=
S
S
S
SSv
VV
VVVTHD
FaactorntDisplacemeFactorDistortionII
IVIV
IVPPF
S
S
SS
SS
SS
*
coscos1
111
=
=== φφ
![Page 5: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/5.jpg)
Single-phase half-wave diode rectifier with resistive load.
![Page 6: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/6.jpg)
∫ ==π
πωω
π 0
sin21 m
mdcVtdtVV
2sin
21
0
22 mmrms
VtdtVV == ∫π
ωωπ
RV
RVI mdc
dc π==
RV
RVI mrms
rms 2==
the load and diode currents RVII m
DS 2==
![Page 7: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/7.jpg)
Example 1: The rectifier shown in Fig.2.1 has a pure resistive load of R Determine (a) The efficiency, (b) Form factor (c) Ripple factor (d) Peak inverse voltage (PIV) of diode D1.
ππ
πωω
π
πmm
mdcVVtdtVV =−−== ∫ ))0cos(cos(
2)sin(
21
0 RV
RVI mdc
dc π==
2)sin(
21
0
2 mmrms
VtVV == ∫π
ωπ R
VI mrms 2
=
%53.40
2*
2
*
**
====
RVV
RVV
IVIV
PP
mm
mm
rmsrms
dcdc
ac
dc ππη
57.12
2 ====π
πm
m
dc
rmsV
V
VVFF
211.1157.11 22 =−=−== FFVVRF
dc
ac
(d) It is clear from Fig2.2 that the PIV is
.
mV
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Half Wave Diode Rectifier With R-L Load
Fig.2.3 Half Wave Diode Rectifier With R-L Load
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( ) ( )
+−=
−φ
ω
φφωω tansinsin)(t
m etZ
Vti
( ) ( ) 0sinsin)( tan =
+−=
−φ
β
φφββ eZ
Vi m
)cos1(*2
sin*2 0
βπ
ωωπ
β
−== ∫ mmdc
VtdtVV
)2sin(1(5.0*2
)sin(*21
0
2 ββπ
ωπ
β
−+== ∫VmdwttVV mrms
![Page 10: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/10.jpg)
Single-Phase Full-Wave Diode Rectifier Center-Tap Diode Rectifier
![Page 11: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/11.jpg)
πωω
π
πm
mdcVtdtVV 2sin1
0
== ∫ RVI m
dc π2
=
( )2
sin1
0
2 mmrms
VtdtVV == ∫π
ωωπ R
VI mrms 2
=
PIV of each diode = mV2
RVII m
DS 2==
Example 3. The rectifier in Fig.2.8 has a purely resistive load of R Determine (a) The efficiency, (b) Form factor (c) Ripple factor (d) TUF (e) Peak inverse voltage (PIV) of diode D1 and(f) Crest factor of transformer secondary current.
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%05.81
2*
2
2*2
**
====
RVV
RVV
IVIV
PP
mm
mm
rmsrms
dcdc
ac
dc ππη
11.1222
2 ====π
πm
m
dc
rmsV
V
VVFF
483.0111.11 22 =−=−== FFVVRF
dc
ac
The PIV is mV2
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Single-Phase Full Bridge Diode Rectifier With Resistive Load
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Example 4 single-phase diode bridge rectfier has a purely resistive load of R=15 ohms and, VS=300 sin 314 t and unity transformer ratio. Determine (a) The efficiency, (b) Form factor, (c) Ripple factor, (d) The peak inverse voltage, (PIV) of each diode, , and, (e) Input power factor.
VVtdtVV mmdc 956.1902sin1
0
=== ∫ πωω
π
πA
RVI m
dc 7324.122==
π
( ) VVtdtVV mmrms 132.212
2sin1
2/1
0
2 ==
= ∫
π
ωωπ
%06.81===rmsrms
dcdc
ac
dc
IVIV
PPη 11.1==
dc
rms
VVFF
482.011 22
222
=−=−=−
== FFVV
VVV
VVRF
dc
rms
dc
dcrms
dc
ac The PIV=300V
Input power factor = 1cosRe==
SS
SS
IVIV
PowerApperantPoweral φ
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Full Bridge Single-phase Diode Rectifier with DC Load Current
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[ ]
[ ] .............,5,3,14
cos0cos2
cos2
sin*20
0
==−=
−== ∫
nforn
In
nI
tnn
ItdtnIb
oo
oon
ππ
π
ωπ
ωωπ
ππ
)..........9sin917sin
715sin
513sin
31(sin*4)( +++++= tttttIti o ωωωωω
π
%46151
131
111
91
71
51
31))((
2222222
=
+
+
+
+
+
+
=∴ tITHD s
π24
1o
SII =
%34.4814
21
241))((
2
2
2
1=−
=−
=−
=∴
π
πo
o
S
Ss I
IIItITHD
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Example 5 solve Example 4 if the load is 30 A pure DC From example 4 Vdc= 190.986 V, Vrms=212.132 V AIdc 30= and rmsI = 30 A
%90===rmsrms
dcdc
ac
dcIVIV
PPη 11.1==
dc
rmsVVFF
482.011 22
222=−=−=
−== FF
VV
VVV
VVRF
dc
rms
dc
dcrms
dc
ac
The PIV=Vm=300V
AII oS 01.27
230*4
24
1 ===ππ
Input Power factor= =PowerApperant
PoweralRe
LagI
IIV
IV
S
S
SS
SS 9.01*30
01.27cos*cos* 11 ===φφ
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Effect Of LS On Current Commutation Of Single-Phase Diode Bridge Rectifier.
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−= −
m
osV
ILu ω21cos 1 oSoS
rd ILfILV 42
4−=
−=
πω
osm
rdceinducsourcewithoutdcactualdc IfLVVVV 42tan −=−=
π
−=
322 2 uII o
sπ
π 2sin*
28
1u
uII o
S π=
( )
−
=
32
sin2uu
upfππ
Example 6 Single phase diode bridge rectifier connected to 11 kV, 50 Hz, source inductance Ls=5mH supply to feed 200 A pure DC load, find: (i) Average DC output voltage, (ii) Power factor. And (iii) Determine the THD of the utility line current. VVm 155562*11000 ==
VV actualdc 9703200*005.0*50*415556*2=−=
π
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.285.015556
200*005.0*50**2*21cos21cos 11 radV
ILum
os =
−=
−= −− πω
( ) ( ) 917.0
3285.
2285.0
285.0sin*2
32
sin*22
cos*1 =
−
=
−
=
=
ππππ uu
uuIIpf
S
S
AuII oS 85.193
3285.0
2200*2
322 22
=
−=
−=
ππ
ππ
Auu
II oS 46.179
2285.0sin*
285.0*2200*8
2sin*
28
1 =
==
ππ
%84.40146.17985.1931
22
1=−
=−
=
S
Si I
ITHD
![Page 21: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/21.jpg)
Three-Phase Half Wave Rectifier
![Page 22: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/22.jpg)
![Page 23: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/23.jpg)
mm
mdc VVtdtVV 827.0233sin
23 6/5
6/
=== ∫ πωω
π
π
π RV
RVI mm
dc*827.0
**233
==π
( ) mmmrms VVtdtVV 8407.08
3*321sin
23 6/5
6/
2 =+== ∫ πωω
π
π
π
RVI m
rms8407.0
=RV
RVII mm
Sr 4854.03
08407===
ThePIV of the diodes is mLL VV 32 =
Example 7 The rectifier in Fig.2.21 is operated from 460 V 50 Hz supply at secondary side and the load Ω resistance is R=20. If the source inductance is negligible, determine (a) Rectification efficiency, (b) Form factor (c) Ripple factor (d) Peak inverse voltage (PIV) of each diode.
![Page 24: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/24.jpg)
VVVV mS 59.3752*58.265,58.2653
460====
mm
dc VVV 827.0233
==π R
VRVI mm
dc0827
233
==π
mrms VV 8407.0=R
VI mrms
8407.0=
%767.96===rmsrms
dcdc
ac
dcIVIV
PPη
%657.101==dc
rmsVVFF
%28.1811 22
222=−=−=
−== FF
VV
VVV
VVRF
dc
rms
dc
dcrms
dc
ac
The PIV= 3 Vm=650.54V
![Page 25: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/25.jpg)
Three-Phase Half Wave Rectifier With DC Load Current and zero source induct
New
axis
![Page 26: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/26.jpg)
![Page 27: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/27.jpg)
321 3/
3/0
oo
ItdIa ∫−
==π
π
ωπ
[ ]
harmonicstrepleanallfor
nfornI
nfornI
tnnIdwttnIa
o
o
oon
0
17,16,11,10,5,43*
,....14,13,8,7,2,13*
sincos*1 3/3/
3/
3/
=
=−=
==
== −−∫
π
π
ωπ
ωπ
ππ
π
π
−−++−−++= ...8sin
817sin
715sin
514sin
412sin
21sin3
3)( ttttttIItI OO
s ωωωωωωπ
%24.1090924.119
*21
23
3/1))((2
2
2
1==−=−
=−
=
π
πO
o
S
Ss I
IIItITHD
![Page 28: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/28.jpg)
Example 8 Solve example 7 if the load current is 100 A pure DC
VVVV mm
dc 613.310827.0233
===π
AIdc 100=
VVV mrms 759.3158407.0 == AIrms 100=
%37.98100*759.315100*613.310
====rmsrms
dcdc
ac
dcIVIV
PPη
%657.101==dc
rmsVVFF
%28.1811 22
222=−=−=
−== FF
VV
VVV
VVRF
dc
rms
dc
dcrms
dc
ac
The PIV= 3 Vm=650.54V
![Page 29: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/29.jpg)
Three-Phase Full Wave Rectifier With Resistive Load
1 3 5
4 6 2
b
c
IL
VLIs
Ip
a
![Page 30: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/30.jpg)
![Page 31: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/31.jpg)
![Page 32: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/32.jpg)
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![Page 34: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/34.jpg)
LLmLLm
mdc VVVVtdtVV 3505.1654.12333sin33 3/2
3/
===== ∫ ππωω
π
π
π
RV
RV
RV
RVI LLLLmm
dc3505.123654.133
====ππ
( ) LLmmmrms VVVtdtVV 3516.16554.14
3*923sin33 3/2
3/
2==+== ∫ π
ωωπ
π
π
RVI m
rms6554.1
=
RV
RVI mm
r 9667.03
6554.1==
RVI m
S 29667.0=
![Page 35: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/35.jpg)
Example 10 The rectifier shown in Fig.2.30 is operated from 460 V 50 Hz supply and the load resistance is R=20ohms. If the source inductance is negligible, determine (a) The efficiency, (b) Form factor (c) Ripple factor (d) Peak inverse voltage (PIV) of each diode .
VVVV mm
dc 226.621654.133===
πA
RV
RVI mm
dc 0613.31654.133===
π
VVVV mmrms 752.6216554.14
3*923
==+=π
AR
VI mrms 0876.316554.1
==
%83.99===rmsrms
dcdc
ac
dcIVIV
PPη
![Page 36: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/36.jpg)
%08.100==dc
rmsVVFF
%411 22
222=−=−=
−== FF
VV
VVV
VVRF
dc
rms
dc
dcrms
dc
ac
The PIV= 3 Vm=650.54V
![Page 37: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/37.jpg)
Three-Phase Full Wave Rectifier With DC Load Current
![Page 38: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/38.jpg)
[ ]
....,.........15,14,12,10,9,8,6,4,3,2,0
),.....3(132),3(
112),3(
72),3(
52,32
cos2sin*2
1311751
6/56/
6/5
6/
==
==−=−==
−== ∫
nforb
IbIbIbIbIb
tnn
ItdtnIb
n
ooooo
oon
πππππ
ωπ
ωωπ
ππ
π
π
++−−= ttttvtItI o
s ωωωωωπ
13sin13111sin
1117sin
715sin
51sin32)(
%31251
231
191
171
131
111
71
51))((
22222222
=
+
+
+
+
+
+
+
=tITHD s
oS II32
= oS IIπ
3*21 =
%01.311/3*23/21))(( 2
2
1=−=−
=
πS
Ss I
ItITHD
Power Factor =S
S
S
SII
II 11 )0cos(* =
![Page 39: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/39.jpg)
![Page 40: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/40.jpg)
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−= −
LL
oSV
ILu ω21cos 1o
ord fLILIV 6
26
==π
ω
oLLrdceinducsourcewithoutdcactualdc fLIVVVV 635.1tan −=−=
−=
632 2 uII o
Sπ
π
=
2sin62
1u
uII o
S π
( )
−
=
−
=
=
63
sin*32
cos
632
2sin62
2cos
21
uu
uuuI
uu
Iu
IIpf
o
o
S
S
ππππ
π
![Page 42: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/42.jpg)
Example 11 Three phase diode bridge rectifier connected to tree phase 33kV, 50 Hz supply has 8 mH source inductance to feed 300A pure DC load current Find; Commutation time and commutation angle. DC output voltage. Power factor. Total harmonic distortion of line current.
oradu 61.14.2549.0 ==
−= −
LL
oSV
ILu ω21cos 1
dLLrdceinducsourcewithoutdcactualdc fLIVVVV 635.1tan −=−=
VVdcactual 43830300*008.*50*633000*35.1 =−=( ) ( ) 9644.0
62549.0
3*2549.0
2549.0sin3
63
sin*3=
−
=
−
=ππππ uu
upf
![Page 43: ee_435_2](https://reader031.fdocuments.in/reader031/viewer/2022032512/55cf9a18550346d033a06ee1/html5/thumbnails/43.jpg)
AuII ds 929.239
62549.0
3*300*2
632 22
=
−=
−=
ππ
ππ
Auu
II oS 28.233
22549.0sin*
2*2549.0*300*3432*
2sin
234
1 =
=
=
ππ
9644.02
2549.0cos*929.23928.233
2cos*1 =
=
=
uIIpf
s
S
%05.24128.233
929.239122
1=−
=−
=
S
Si I
ITHD