Thyristors and controlled rectifiers EE328 Power Electronics Assoc. Prof. Dr. Dr. Mutlu BOZTEPE BOZTEPE Ege University, Dept. of E&E
Outline of lecture S C I N O R T C E L E R E W O P 8 2 3 E E
Thyristors
Unijunction transistors
Principal of phase control
Single Phase controlled rectifier – Single Phase Half-wave Rectifiers – Single Phase Semiconverters – Single Phase Full converters – Single Phase Dual converters
Three Phase controlled rectifier – Three Phase Half-wave Rectifiers – Three Phase Semiconverters – Three Phase Full converters – Three Phase Dual converters
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
2
Thyristor
Most important type of power semiconductor device. They can operate as a bistable switch that can be turned on by a gate signal, but can not be turned off by the gate.
Proposed in 1950s at Bell Lab. The first thyristor was developed in 1957 by General Electric (GE) Have highest power handling capability up to ~4500 Volt, up to ~5000 Amperes Amperes Maximum switching frequency for typical thyristors is around 1kHz. But it can rise up to 20kHz for some special types.
It is inherently slow switching device compared compare d to BJTs BJTs or MOSFETs. MOSFETs. EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Structure
It is a four-layer semiconductor device of pnpn structure with three pn-junctions; e.g. J1, J2 and J3. Terminals; Anode (A), Cathode (K) and Gate (G) Forward blocking mode: When Anode voltage is made positive with respects to Cathode, the junctions J1 and J3 are forward biased, and J2 is reverse biased, and therefore a small leakage current can flow through the device. Reverse blocking mode: When Cathode has positive voltage than the Anode, J1 and J3 are reverse biased, and J2 is forward biased, and therefore a small leakage current can flow through the device. For both blocking modes the gate terminal is assumed as open circuit. EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Avalanche breakdown
Forward leakage current is very small. If the V AK is increased to a sufficiently Latching current large value, the leakage current increases and the junction J2 breaks down.
IT
Forward breakdown voltage
IL
This voltage is called as forward breakdown voltage (VBO). Since the other junctions J1 and J3 are already fwd biased, then the device will be in conducting state or on-state.
Forward leakage current
VBO
V AK
The anode current must be more than a value known as latching current to keep the thyristor is on-state. Otherwise the device will revert to the blocking condition as the V AK is reduced. Latching current is the minimum anode current to maintain the thyristor in the on-state immediately after it is turned on (no gate signal) EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Holding current
Once the thyristor conducts, it behaves as a conducting diode and there is no control over the device. Therefore the device current must be limited by external components, such as resistors.
IT Forward voltage drop
Latching current
IL
Forward breakdown voltage
IH Holding current
The forward voltage drop is due to the ohmic drop in the four layers and it is small, typically 1V.
VBO
V AK
If the fwd anode current is reduced below a level known as holding current IH, a depletion region is developed around junction J2 due to the reduced number of carriers, and the thyristor will be in blocking state. The holding current is very small in the order of milliamperes, and it is less than the latching current.
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Gate triggering
A thyristor can be turned on by increasing forward voltage beyond breakdown voltage V BO, but such a turn-on could be destructive. In practice, a positive gate-cathode voltage V GK, is applied to the thyristor. As the gate current is increased, the forward blocking voltage is decreased as shown in the figure Once the thyristor is turned on by gating signal and its forward current is greater than the holding current, the device continues to conduct. Thyristor is a latching device.
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Two-transistor model of thyristor
The latching action due to positive feedback can be demonstrated by using two-transistor model of thyristor.
I A I C 1 I C 2 1 I A I CBO1 2 I K I CBO2
ICBO1 and I CBO2 are leakage currents.
For a gating current I K I A I G and solving for I A
I A
2 I G I CBO1 I CBO 2 1 ( 1 2 )
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Two-transistor model of thyristor I A
2 I G I CBO1 I CBO 2
1 ( 1 2 ) The current 1 varies with the emitter current I A, and 2 varies with IK=I A+IG. When gate current I G is increased, I A increases too. An increase in IG also increases 1 and 2. The increase in 1 and 2 causes further increase Typical variation of current gain with emitter current in in I A, and go on… thyristor If (1 + 2) tends to be unity denominator approaches zero, resulting in large current of I A. Therefore can be turned on by a small gate current.
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Thyristor turn-on A thyristor can be turned on by the following ways; Thermals: If the temperature is high, there will be an increase in the number of electron-hole pairs. This increase would cause ( 1 + 2) to increase which may turn on the thyristor. This type of turn-on may cause thermal runaway and is normally avoided.
Light: If light is allowed to strike the junctions, the electron-hole pairs will increase; and the thyristor may be turned on. High voltage: If VAK is greater than the VBO, thyristor turns on. dv/dt: If the rate of rise of anode-cathode voltage is high, the charging current of the junction capacitance may trigger the thyristor and make it turned-on. The device must be protected against dv/dt. Gate current: If a thyristor forward biased, a positive gate-cathode voltage would turn on the thyristor. EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Thyristor types
Phase-control thyristors (SCRs)
Fast-switching thyristors (SCRs)
Gate-turn-of thyristors (GTOs)
Bidirectional triode thyristors (TRIACs)
Reverse-conducting thyristors (RCTs)
Static Induction thyristors (SITHs)
Light-activated silicon-controlled thyristor (LASCRs)
FET-controlled thyristor (FET-CTHs)
MOS-controlled thyristor (MCTs)
Triac
MCT
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SIT
GTO
LASCR
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Gate drive
The following points should be considered in designing the gate control circuit; – The gate signal should be removed after the thyristor is turned on. A continues gate signal increases the power loss in the gate junction. – While thyristor is reversed biased, there should be not gate signal; otherwise, the thyristor may fail due to increased leakage current. – The width of gate pulse t G must be longer than the time required for the anode current reach to the holding current.
Opto isolated gate drive EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
Pulse transformer isolated gate drive 12
Unijunction transistor
Since the device has one pn-junction and three leads, it is commonly called a unijunction transistor. With only one pn-junction, the device is really a form of diode. The emitter is heavily doped having many holes. The n region, however, is lightly doped. For this reason, the resistance between the base terminals is very high ( 5 to 10 kΩ) when emitter lead is open.
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Unijunction transistor
If voltage VBB is applied between B2 and B1 with emitter open, a voltage gradient is established along the n-type bar. Since the emitter is located nearer to B2, more than half of VBB appears between the emitter and B1. The voltage V1 between emitter and B1 establishes a reverse bias on the pn junction and the emitter current is cut off. Only leakage current flows. If a positive voltage is applied at the emitter the pn junction will remain reverse biased so long as the input voltage is less than V1 If the input voltage to the emitter exceeds V1, the pn junction becomes forward biased, and then the device is now in the ON state. If a negative pulse is applied to the emitter, the pn junction is reverse biased and the emitter current is cut off. The device is then in the OFF state.
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Equivalent circuit of UJT
The resistance of the silicon bar is called the interbase resistance RBB The inter-base resistance is represented by two resistors in series; RB1 and RB2.
RB2 is constant. RB1 is variable and depends on the bias voltage across the pn junction
The pn junction is represented in the emitter by a diode D. The ratio V1/VBB is called intrinsic stand-off ratio () which is between 0.51 to 0.82.
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Characteristics of UJT
Initially, in the cut-off region, as VE increases from zero, slight leakage current flows from terminal B2 to the emitter. This current is due to the minority carriers in the reverse biased diode. Above a certain value of VE, forward IE begins to flow, increasing until the peak voltage VP and current I P are reached at point P. After the peak point P, an attempt to increase V E is followed by a sudden increase in emitter current I E with a corresponding decrease in VE. This is a negative resistance portion. The negative portion of the curve lasts until the valley point Vv is reached. After the valley point, the device is driven to saturation.
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Design UJT circuit
The load line formed by R and Vs should intersect the device characteristics to the right of peak point but to the left of valley point, otherwise UJT will not turn on.
I p
V s V v I v
Therefore min&max values for R V s V v I v
V s V p
R
V s V p I p
where Vp can be calculated as
V p V 1 V D V BB V D
assume VS VBB
V p V S V D
V D: One diode fwd voltage drop, 0.5V
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Design UJT circuit
The pulse width of triggering pulse t g is
t g R B1C
Oscillation frequency is T
1 f
RC ln
1 1
A resistor RB2 is generally connected in series with B2 to compensate for the decrease in Vp due to temperature rise and to protect the UJT from thermal runaway.
R B 2
104 V S
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Exercise 1
Design the UJT triggering circuit. The parameters of UJT are V s=30V, =0.51, Ip=10 A, Vv=3.5V, and Iv=10mA. The frequency of oscillation is f=60Hz, and width of pulse is t g=50s.
Solution: V p 0.51 30 0.5 15.8V Let assume C=0.5 F 1 1 1 R 0.5 F ln T RC ln 1 60 1 0.51
V s V p V s V v R I v I p
R 46.7k
30 3.5
t g
10mA
R B1
R B 2
C
50 s 0.5 F
104 0.51 30
100
654
R
30 15.8 10 A
2.65k R 1.42 M Min&max limits for R
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19
Principle of phase control
Diode rectifiers produce a fixed output voltage. In order to control the output voltage of a rectifier, phase control thyristors must be used instead of diodes. The output voltages of these rectifiers are varied by varying the delay or firing angle of the thyristor. Phase controlled thyristors are turned on by the application of a short pulse to the gate and they are turned off by the process of natural or line commutation.
V dc
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V m 2
1 cos
20
Principle of phase control
There are two types of phase control converters: – Single phase converters. – Three-phase converters
Each type of converter can be divided into three categories: – S emic onverter : one quadrant converter, having one polarity of voltage and current
– F ull converter : two quadrant device whose output voltage polarity can be either positive or negative but whose output current has one polarity.
– Dual conver ter : four quadrant device whose output voltage and current can be of either positive of negative polarity.
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21
Single Phase half-wave SCR rectifier with R Load
For the positive half cycle of Vs, T1 is forward biased and when the thyristor is fired at wt= it conducts and input voltage appears across the load. When the input voltage goes negative at wt= thyristor is reverse biased and it is turned off. The firing angle (or delay angle) is defined as the time after the input voltage starts to go positive until the thyristor is fired at wt= . For this converter: 0 180° EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Single Phase half-wave SCR rectifier with R Load
d 3 3 e e / r u o f e d r / f f a t s / c e l e / s t p e d / t t . i w u . g n e . w w w / / : p t t h EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Single Phase half-wave SCR rectifier with R Load
Average output voltage V 1 V dc V m sin t d t m cos t 2 2
V m 2
1 cos
Rms output voltage V rms
1
V 2
2 m
sin
2
t d t
V m 2
1
V m2
1 cos 2 t d t 4
sin 2 2
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Exercise 2
For single phase half wave thyristor converter with R load, delay angle is =90°, determine, a) rectification efficiency, b) FF, c) RF, d) TUF, e) PIV Solution: V dc
V m 1 cos 90 0.1592V m 2
V m 2
1
90 180
sin2 90 2
0.3536V m
V 0.1592V m I dc dc R R P dc V dc I dc
V rms
I rms
0.1592V m 2 R
V rms R
0.3536V m R
P ac V rms I rms
a) Rectification efficiency
0.3536V m 2 R
0.1592V m P dc 20.27% 2 P ac 0.3536V m 2
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Exercise 2 (cont.) b) Form factor FF
0.3536V m V ac 2.221or 222.1% 0.1592V m V dc
c) Ripple factor RF FF 2 1
2.2212 1 1.983 or 198.3%
d) VA power at transformer secondary is I s I rms
0.3536V m
VA V s I s
V s
R
V m 2
e) PIV=Vm
0.707V m
0.3536V m 0.70 7V m R 2
V m
0.1592V 2 R 0.1014or (10.14%) TUF 0.707V 0.3536V R VA P dc
m
m
m
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Single phase semiconverters
Load current is assumed continues and ripple free. During the positive half cycle, T1 & D2 are fwd biased, and when the T1 is fired at wt= , load is connected to input supply. During wt +, the input voltage is negative and freewheeling diode Dm conducts. At wt= +, T2 is fired and Dm is reverse biased. Then the load is connected to the supply through T2 and D1. EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Single phase semiconverters
d 3 3 e e / r u o f e d r / f f a t s / c e l e / s t p e d / t t . i w u . g n e . w w w / / : p t t h EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Single phase semiconverters
Average output voltage 2V m 2 cos t V dc V m sin t d t 2 2
V m
1 cos
Rms output voltage V rms
2
V 2
2 m
sin
2
t d t
V m
1
2
V m2
1 cos 2 t d t 2
sin 2 2
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Exercise 3
Single phase semi converter is connected to a 120V 60Hz supply. Load current Ia can be assumed continues and its ripple content is negligible. Turns ratio is unity. Delay angle is =/2. a) express the input line current in a Fourier series; b) determine Vdc, Vrms, Harmonic factor, displacement factor, input power factor
Solution a) I dc
1
i (t ) d t 0
2
s
1
an I a cos n t d t I a cos n t d t 2
2 I a
n
I a sin n t d t I a sin n t d t 2
bn
sin n for n 1,3,5...
0
1
2 I a
n 0
for n 2,4,6...
1 cos n
for n 1,3,5...
for n 2,4,6...
a
i s (t ) I dc
n
cos n t bn sin n t
n 1, 2...
i s (t )
n 1,3,5...
2 I sn sin n t n
n tan
1
an bn
n 2
I sn an bn
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
2
2
2 2 I a n
cos
n 2 30
Exercise 3 (cont.) b)
V dc
V m
V rms
V m
I s1
1 cos 54.02V
1
2
sin 2
84.57V 2
2 2 I a cos 0.6366I a 4
2
I rms
2
1
PF
I a2 d t I a 1
2
0.7071I a
I HF s 1 0.4835 or 48.35% I s1
DF cos 0.7071 4 4
I s1 I s
cos
2
0.6366(lagging )
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31
Single phase semiconverter with RL load
The load current of a semiconverter is dependent on the load resistance inductance and the battery voltage E in series with the load. The converter operation can be divided into two modes: Mode 1 (0 wt ): Freewheeling diode is forward biased and load current is provided by the energy stored in the magnetic field.
Mode 2 ( wt
): Load current is provided by the supply.
The current avg and rms values can be calculated by solving first the differential equations above. (See the book for solution.) EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
32
Single phase full converter
Load current is assumed continues and ripple free. During the positive half cycle, T1 & T2 are fwd biased, and when the SCRs are fired at wt= , load is connected to input supply. T1&T2 will continue to conduct beyond wt= due to inductive load. At wt=+, T3&T4 are fired that makes T1&T2 are reverse biased. EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
33
Single phase full converter
For the period of wt the input voltage and current are positive and power flows from supply to load and the converter is said to be in rectification mode. For the period wt +, the input voltage is negative, input current is positive and power flows from the load to the supply. The converter is said to be operated in the inversion mode. EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
34
Single phase full converter
Average output voltage 2 V dc 2
2V m
V m sin t d t
2V m cos t 2
cos Note that: For purely resistive loads the output voltage will be similar to semiconverter
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Single phase full converters
Rms output voltage
V rms
2 2
V m2 sin 2 t d t
V m2 2
1 cos 2 t d t
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V m 2
V s
36
Exercise 4
Single phase full converter is connected to a 120V 60Hz supply. Load current Ia can be assumed continues and its ripple content is negligible. Turns ratio is unity. Delay angle is =/3. a) express the input line current in a Fourier series; b) determine Vdc, Vrms, Harmonic factor, displacement factor, input power factor
Solution a) I dc
1 2
i (t ) d t 0 s
2
1
an I a cos n t d t I a cos n t d t
4 I a
n
sin n for n 1,3,5...
0
for n 2,4,6...
bn
2
1
I a sin n t d t I a sin n t d t
4 I a
n 0
cos n for n 1,3,5...
for n 2,4,6...
a
i s (t ) I dc
n
cos n t bn sin n t
n 1, 2...
i s (t )
n 1,3,5...
2 I sn sin n t n
n tan 1
an bn
n
I sn an2 bn2
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2 2 I a n 37
Exercise 4 (cont.) b)
V dc
2V m
V rms
V m
I s1
cos 54.02V
2
V s 120V
2 2 I a 0.90032I a
2
I HF s 1 0.4834 or 48.34% I s1
I rms I a
0.5 3
1 DF cos
PF
I s1 I s
cos 0.45(lagging )
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38
Single phase fullconverter with RL load
The load current of a fullconverter is dependent on the load resistance inductance and the battery voltage E in series with the load. The converter operation can be divided into two identical modes.
Mode 1 (
Mode 2 ( +
For both mode the load current is provided by supply, then
wt
+ ): T1 & T2 conducts
wt 2 +
): T3 & T4 conducts
The current avg and rms values can be calculated by solving first the differential equations above. (See the book for solution.)
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
39
Single phase fullconverter
Harmonic content of output voltage vs. delay angle for single phase full converter. Load is continues The rms load current can be calculated approximately using voltage harmonics instead of analytical solution.
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40
Single phase dual converter
When two full converter are connected back to back, and the system will provide four-quadrant operation and is called as dual converter . If 1 and 2 delay angles of converter 1 and 2 respectively, the corresponding average output voltages are Vdc1 and Vdc2. The delay angles are controlled such that one converter operates as a rectifier and the other converter operates as an inverter, but both converter produce the same average voltage. Since the instantaneous voltage difference will result in circulating current between converters, two circulating current reactor Lr/2 are used . EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Single phase dual converter
V dc1
2V m
cos 1
V dc 2
2V m
cos 2
One converter is rectifying, the other is inverting V dc1
V dc 2
therefore
cos 2 cos 1 cos 1 2
1 EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Circulating current Assume circulating current İr is discontinues (İr(0)=0 ) t t 1 1 ir vr d t vo1 vo 2 d t Lr 2 Lr 2 1 1
V m Lr
2
t
1
sin t d t sin t d t 2 t
1
2V m cos t cos 1 Lr
The circulating current depends on 1 The maximum value can be
ir ,max
4V m Lr
If the peak load current is Ip, then the converters should carry a peak current of
I p ir , max I p
4V m Lr
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Circulating current
The dual converter can be operated with or without a circulating current. If only one converter operates at a time and carries load current, t he other converter is completely blocked by inhibiting gate pulses. However, operating with a circulating current has the following advantages; – Both converters are in continues conduction, independent of the load – Power flow in either direction at any time is possible. – Time response for changing from one quadrant to another is faster
Exercise 5: Dual converter supplied from 120V, 60Hz source, resistive load R=10 . Lr=40mH, 1=60°, 2=120°.
Peak circulating current ir
Peak load current i p
2V m Lr
1 cos 1
2
1 cos 60 11.25 A
2 120
3770.04
2 120 16.97 A 10
Peak current of converter1 is 16.97+11.25=28.22A EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
44
Three phase half-wave converter
Three phase converters provide higher average output voltage Output voltage ripple frequency is higher than single phase converters. Therefore filtering requirement is simpler. For this reason 3-phase converters are used extensively in highpower applications.
Delay angle is defined starting from natural commutation points where phase voltages are equal. EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
45
Three phase half-wave converter
Load current is assumed constant. When T1 is fired at wt= /6+, the load voltage is Vo=Van, until T2 is fired at wt=5/6+. When thyristor T2 is fired, thyristor T1 is reverse biased, because line-to-line voltage Vab is negative, and T1 is turned off. For resistive loads and when /6, the load current will be discontinues. The frequency of output ripple is 3f s This converter is not used frequently in practice due to high ripple content. EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
46
Three phase half-wave converter
For continues load current:
Output dc voltage 3 V dc 2
5 6
V
m
sin t d t
6
3 3V m cos 2
Rms output voltage V rms
3V m
3 2 1 6
5 6
V m2 sin 2 t d t
6
3 8
co s 2
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47
3-phase half wave converter with RL load
Van
V bn
Vcn
V0 0
=30
=300
0
0
30
0
60
0
90
0
120
0
150
0
180
0
210
Van
0
240
0
270
0
300
0
330
0
360
V bn
0
390
t
0
420
Vcn
V0
=60
0
=600 0
0
30
0
60
0
90
0
120
0
150
0
180
0
210
0
240
0
270
0
300
0
330
0
360
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0
390
0
t
420
48
3-phase half wave converter with RL load
=900
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49
Three phase half-wave converter
For resistive loads: For </6, the Vdc and Vrms are same with constant load current case.
Vbn
Vcn
Van
200
100
0
For /6: Output dc voltage
-100
3 V dc V m sin t d t 2 6
3V m 1 cos 2 6
Rms output voltage
V rms
3
-200
Vload 200
150
100
V m2 sin 2 t d t
50
2 6
0
3V m
sin 2 24 4 8 3 5
1
0.3
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
0.31 Time (s)
0.32
0.33
50
3-phase half wave converter with R load V bn
Van
Vcn
=0 Vs
=00
0
0
30
0
60
0
90
0
120
0
150
0
180
0
210
0
240
0
270
0
300
0
330
0
360
V bn
Van
0
390
0
420
t
Vcn
=150 =150
V0
0
0
30
0
60
0
90
0
120
0
150
0
180
0
210
0
240
0
270
0
300
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0
330
0
360
0
390
0
420
t
51
3-phase half wave converter with R load
V bn
Van
Vcn
=300 =300
V0
0 0
30
0
60
0
90
120
0
150
0
180
0
0
210
0
240
300
0
330
0
0
360
V bn
Van
0
270
0
390
0
420
t
Vcn
=600 =600
V0
0
0
30
0
60
0
90
120
0
150
0
180
0
0
210
0
240
0
270
300
0
330
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
0
0
360
0
390
0
420
t
52
Exercise 6
3-phase half wave converter is operated from Y-connected 208V 60Hz supply. Load resistance R=10 . Half of the maximum possible average voltage is requested at the output. Calculate a)delay angle, b) rms and average output current, c)average and rms thyristor currents, d) rectification efficiency, e)Transformer utilization factor, f) input power factor Solution:
The maximum output voltage is V dc , max
3 3V m 3 3 169.83 140.45V 2 2
Desired output voltage, then 0.5*140.45=70.23V a) For resistive load and </6,
3 3 169.83 cos 60 then it is not valid ! 2 6 Therefore, the equation for >/6 should be used 70.23
70.23
3 3 169.83 1 cos 67.7 2 6 EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Exercise 6 b) rms and average output current V 70.23 I dc dc 7.02 A 10
R
V rms I rms
5
3 16 9.83 V rms R
24
94.74 10
67.7
180 1 cos 2 67.7 94.74 V 4 8 18 0 3
9.47 A d) rectification efficiency
c) average and rms thyristor currents I A
I dc
I R
3
I rms 3
7.02 3
2.34 A
9.47 3
P dc P ac
70.23 7.02 94.74 9.47
54.95%
5.47 A
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Exercise 6 e)Transformer utilization factor The rms line current is the same as the thyristor rms current
I s I R 5.47 A
V s 120.1V
VA 3V s I s 3 120.1 5.47 1970.84W
TUF
P dc 70.23 7.02 0.25 or ( 25%) VA 1970.84
f)
2 2 9 . 47 10 896.81W P I R Output power is o rms
Then input power factor is
PF
896.81 1970.84
0.455 (lagging )
Note that due to the delay angle, , the fundamental component of input line current is also delayed with respect to the input phase voltage
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Three phase semiconverter
Three phase semiconverters are used in industrial applications up to 120kW level, where one quadrant operation is required. The power factor of this converter decreases as the delay angle increases, but it is better than 3-phase half wave converters. v an V m sin t l vac van vcn 3V m sin t a 6 r t 2 u s e s 5 e e vbn V m sin t n e i 3 3 V sin t n g l g vab van vbn m 6 a a e t e t l l 2 n n i o v i o V m sin t L v cn L v 3 vcb vcn vbn 3V m sin t 2 EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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3-phase Semiconverter for > 600
Frequency of output voltage is 3fs The delay angle can be varied from 0 to At wt=7/6, Dm conducts due to Vac starts to be negative If there were no Dm, the freewheeling action would be accomplished by T1 and D2.
=90°
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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3-phase Semiconverter for 600
Output dc voltage 7 6
3 V dc 3V m sin t d t 2 6
3 3V m 1 cos 2
Output rms voltage
V rms
3V m
3
7 6
3V m2 sin 2 t d t
2 6
3 1 sin 2 4 2
=90° EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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3-phase Semiconverter for 600
Each thyristor conducts for 120° and freewheeling diode Dm doesnt conduct. Average output voltage
3 vab d t V dc 2 6
2
3 3V m 1 cos 2
2vac d t
5 6
=30°
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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3-phase Semiconverter for 600
Rms output voltage
V rms
3V m
3
2
2 6
v d t v d t 2 2 ab
5 6 2 ac
3 2 3 cos2 4 3 =30° EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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3-phase Semiconverter for 600
Current waveforms for thyristors and diodes
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
=30°
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Exercise 7
3-phase semiconverter is operated from Y-connected 208V 60Hz supply. Load resistance R=10 . Half of the maximum possible average voltage is requested at the output. Calculate a)delay angle, b) rms and average output current, c)average and rms thyristor currents, d) rectification efficiency, e)Transformer utilization factor, f) input power factor Solution:
The maximum output voltage is V dc , max
3 3V m
3 3 169.83
280.9V
Desired output voltage, then 0.5*280.9=140.45V a) The output voltage for semiconverter is
V dc
3 3V m 1 cos 2
3 3 169.83 140.45 1 cos 90 2 EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Exercise 7 b) rms and average output current I dc
V dc
R
14 0.45 10
3 1 sin 2 18 0.13V 4 2 2 2
V rms 3 16 9.83
I rms
V rms
R
14.05 A
18 0.13 10
18.01 A
c) average and rms thyristor currents I A
I R
I dc 3
I rms 3
14.05
3
4.68 A
18.01 3
d) rectification efficiency
P dc P ac
140.45 14.05 18 0.13 18.01
60.8%
10.4 A
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Exercise 7 e)Transformer utilization factor Since a thyristor conducts 2 /3, the rms input line current is I s I rms
2 3
18.01
2 3
14.71 A
V s 12 0.1V
VA 3V s I s 3 120 .1 14.71 5300VA
TUF
P dc 140.45 14.05 0.372 or (37.2%) VA 5300
f)
2 2 18 . 01 10 3243.6W P I R Output power is o rms
Then input power factor is
PF
3243.6 5300
0.61 2 (lagging )
Note that the power factor is better than that of 3-phase half-wave converter
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Three phase full converters
Known as a 6-pulse converter, or 3 phase bridge converter Used in industrial applications up to 120kW output power. Two quadrant operation is possible.
Output ripple frequency is 6fs
Thyristor is fired at interval of /3
Filtering requirement is less than semi- and half converters
Firing sequence is 12,23,34,45,56,61,12… l a r t u s e e n - g a e t l n i o L v
v an V m sin si n t 2 3 2 vcn V m sin t 3
vbn V m sin t
e s n e i l g a e t l n i o L v
6 vbc vbn vcn 3V m sin t 2 5 vca vcn van 3V m sin t 6 vab van vbn 3V m sin
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Three phase full converters
The thyristors are triggered at an interval of / / 3. T1 is triggered at t = ( /6 + ), T6 is already conducting when T1 is turned ON. During the interval ( /6 + ) to (/2 + ), T1 and T6 conduct together & the output load voltage is equal to v ab = (v an – v bn )
T2 is triggered at t = (/2 + ), T6 turns off naturally as it is reverse biased as soon as T 2 is triggered. During the interval ( /2 + ) to (5/6 + ), T1 and T2 conduct together & the output load voltage v O = v ac = (v an – v cn ) EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Three phase full converters
Current waveforms for thyristors and diodes
Line period 2 EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Three phase full converters
Output rms voltage V rms
3V m
3
2
6 1 2
3V m2 sin 2 t
3 3 4
co s 2
Output dc voltage
d t 6
V dc
3
3 3V m
2
3V m sin t
6
d t
6
cos
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Harmonic content of output voltage
Three phase full converters for continues load current (highly inductive) without Dm
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Exercise 8
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Exercise 8 (cont.)
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Output voltage for various values
Maximum delay angle max = 180 °
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Three phase full converters for or Dm is used
/3 for R load
For /3, the instantaneous output voltage vo will have a negative part. Since the current through thyristors can not be negative, the load current will always be positive. Thus for resistive loads, or when freewheeling diode is used, the instantaneous voltage can not be negative, and the full converter behave as a semiconverter.
Output dc voltage
V dc
3
2
3V m sin t d t
V rms
6
3 3V m 1 cos 3
Output rms voltage
3V m
3
2
3V m2 sin 2 t d t
6
3 1 sin 2 2
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Three phase full converters for or Dm is used
/3 for R load
Maximum delay angle max = 120 °
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Exercise 9
3-phase fullconverter is operated from Y-connected 208V 60Hz supply. Load resistance R=10 . Half of the maximum possible average voltage is requested at the output. Calculate a)delay angle, b) rms and average output current, c)average and rms thyristor currents, d) rectification efficiency, e)Transformer utilization factor, f) input power factor Solution:
The maximum output voltage is V dc , max
3 3V m
3 3 169.83
280.9V
Desired output voltage, then 0.5*280.9=140.45V a) For resistive load and /6,
V dc
3 3V m
cos
140.45
3 3 169.83
cos 60
/6 OK!
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Exercise 9 b) rms and average output current I dc
V dc R
14 0.45 10
V rms 3 169.83 I rms
V rms R
14.05 A
1 2
15 9.29 10
3 3 4
cos 2 60 159.29V
15.93 A
c) average and rms thyristor currents I A
I dc 3
I R I rms
14.05 3
2 6
4.68 A
15.93
2 6
d) rectification efficiency
P dc P ac
140.45 14.05 159.29 15.93
77.8%
9.2 A
Thyristor conducts 1/3 of the line period EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Exercise 9 e)Transformer utilization factor Since a thyristor conducts during 4/6 of line period, then I s I rms
4 6
15.93
4 6
13 A
V s 12 0.1V
VA 3V s I s 3 120.1 13 4683.9 W
TUF
P dc 140.45 14.05 0.421or ( 42.1%) VA 4683.9
f)
2 2 10 2537.6W P I R 15 . 93 Output power is o rms
Then input power factor is
PF
2537.6 4683.9
0.542 (lagging )
Note that the power factor is less than 3-phase semiconverter, but better than that of 3-phase half-wave converter
EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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Three phase dual converters
For four quadrant operation in many industrial variable speed dc drives , 3 phase dual converters are used. Used for applications up to 2 mega watt output power level. Dual converter consists of two 3 phase full converters which are connected in parallel & in opposite directions across a common load. The delay angles are controlled such that one converter operates as a rectifier and the other converter operates as an inverter, but both converter produce the same average voltage. Lr stands for the circulating currents EE328 Power Electronics, Dr. Mutlu Boztepe, Ege University 2014
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