Lab 3
Lab 3
DC-DC Converters:
1. Introduction and Background:
DC-DC converter converts voltage from dc to dc. DC converter is like a transformer that can both step up
and step down voltage but for dc only. DC converters use switching devices like IGBTs, MOSFETs, GTOs,
BJTs etc. There can be ripples in output voltage just like in the case of rectifiers, that’s why filters might
be used to filter out harmonics. Some of the performance parameters for dc converters are ripple factor,
THD, HD and conversion efficiency [1].
2.1. Methodology:
Circuit is simulated in Simulink (MATLAB) and results are also calculated using formulas from lecture
notes. At the end, calculated and simulated results are compared.
Equations used to calculate average output voltage, inductor ripple current and capacitor ripple voltage
for Boost converter for R and RL load are following
Vs
Vo ( avg )=
1−k
Vs
∆ I ( inductor )= kT
L
kIa
∆ Vc=
fC
2.2. Resistive Load:
Table 1: Resistive Load
2.3. RL Load:
Table 2: RL Load
2.7. Conclusion:
Boost converter steps up input DC voltage. Value of output DC voltage depends upon duty cycle. Duty
cycle can be varied by changing turn on time or switching frequency. As duty cycle is decreased, output
voltage also decreases. Output voltage also increases by decreasing switching frequency. Ripple in
output voltage and inductor current depend upon value of output capacitance and inductance value
respectively. If value of filter capacitance is decreased, ripple in output voltage is increased. Similarly, if
value of inductance is decreased, ripple current also increases.
3.1. Methodology:
Circuit is simulated in Simulink (MATLAB) and results are also calculated using formulas from lecture
notes. At the end, calculated and simulated results are compared.
Equations used to calculate average output voltage, inductor ripple current and capacitor ripple voltage
for Boost converter for R load are following
Vo ( avg )=k × Vs
Vs ( 1−k ) k
∆ I ( inductor )=
fL
k ( 1−k ) Vs
∆ Vc= 2
8 LC f
3.6. Conclusion:
Buck converter steps down input voltage. Value of output DC voltage depends upon duty cycle. By
increasing duty cycle (k), we get higher DC voltage and vice versa. By changing switching frequency,
ripples in output voltage and inductor current also change. As value of filter capacitance is increased,
ripple in output voltage and current are decreased. Same is the case for inductance value.
4.1. Methodology:
Circuit is simulated in Simulink (MATLAB) and results are also calculated using formulas from lecture
notes. At the end, calculated and simulated results are compared.
Equations used to calculate average output voltage, inductor ripple current and capacitor ripple voltage
for Boost converter for R load are following.
−k
Vo ( avg )= Vs
1−k
Vs ×k
∆ I ( inductor )=
fL
k × Ia
∆ Vc=
Cf
4.2. Resistive Load:
Table 10: Resistive Load
4.6. Conclusion:
Buck-Boost converter can both step up and step down DC voltage. When duty cycle is greater than 0.5,
voltage is stepped up and when duty cycle is below 0.5 voltage is stepped down. Changing frequency of
switching has a significant effect on ripple voltage and current. By increasing switching frequency, ripple
voltage and current is decreased. Similarly, increasing capacitance or inductance will also decrease
ripple voltage and current.
Lab 4
Inverters:
1. Introduction and Background:
Inverter is electronic circuit that converts DC voltage in AC voltage. Inverter can be either single phase or
three phase depending upon output voltage. Depending upon pulse and no of SCRs used inverter can be
single phase two or 04 pulses for single phase output case. Three phase inverter can have 120 or 180-
degree pulse width [2].
Methodology:
Circuits are simulated in Simulink MATLAB and theoretical calculations are drawn using formulas from
notes.
For single phase two pulse inverter theoretical calculations are made using following equations.
Vdc
Vo ( rms )=
2
Vo(t )
Io ( t )=
Z
Where,
Z=√ R 2+(wL)2
Further expression of output current requires Fourier solution.
For single phase two pulse inverter theoretical calculations are made using following equations.
Vo ( rms )=Vdc
∞
4 Vdc
Io ( t )= ∑ nπZ
sin ( nwt −θ )
n=1 ,3 , 5 ….
Z=√ R 2+(wL)2
THD from RMS from 1st harmonic 3rd harmonic 5th harmonic
Simulation Simulation from simulation from simulation from simulation
Current (A) 4.947 61.35 86.65 0.1456 0.02649
Voltage (V) 144 200 161.3 0.701 0.2083
Figure 5: Single Phase Two Pulse Inverter Output Voltage and Current
Figure 6: Single Phase Two Pulse Inverter’s Gate Pulses
THD from RMS from 1st harmonic 3rd harmonic 5th harmonic
Simulation Simulation from simulation from simulation from simulation
Current (A) 1.387 121.7 172.1 0.02243 0.07078
Voltage (V) 76.66 285.6 320.5 0.1086 0.5607
Figure 8: Single Phase Four Pulse Inverter Output Voltage and Current
Figure 9: Single Phase Four Pulse Inverter’s Gate Pulses
2.3. Single Phase 4 Pulse Inverter over Modulation:
Over modulation is technique of PWM in which output voltage of inverter is increased with it. Over
modulation in PWM occurs, when the width of pulse goes to 0 or/ and 100%
before the modulating signal has reached its maximum or minimum value.
Figure 10: Single Phase Four Pulse Inverter over Modulation
Table 18: RL Load
THD from RMS from 1st harmonic 3rd harmonic 5th harmonic
Simulation Simulation from simulation from simulation from simulation
Current (A) 0.915 151.8 214.6 0.1017 0.2559
Voltage (V) 52.08 318.6 399.6 0.4906 2.026
Figure 11: Single Phase Four Pulse Inverter over Modulation Output Voltage and Current
Figure 12: Single Phase Four Pulse Inverter’s Gate Pulses
2.4. Conclusion:
Single phase inverter provides single phase AC output. Magnitude of output voltage and harmonics in
output quantities depend on modulation techniques and no of switching devices. For two pulses scheme
i.e. using two SCRs output voltage’s magnitude is less compared to 04 pulse technique. Also THD is quite
high compared to other two circuits. Highest value of output and best quality of output is obtained
when over modulation technique is used.
3. Three Phase Inverters:
These inverters produce three phase output voltage. This circuit uses 06 switching devices to convert DC
voltage in AC voltage. Conduction mode of switches can use either 120 degrees or 180 degrees’
conduction mode. Apart from these SPWM technique can also be used for switching devices.
Methodology:
Circuits are simulated in Simulink MATLAB and theoretical calculations are drawn using formulas from
notes.
For three phase inverter with 120 and 180-degree conduction mode, theoretical calculations are made
using following equations (for Phase values).
Vo ( rms )=0.4082 Vs
Vo(rms)
Io ( rms )=
R
For 180-degree mode,
Vo ( rms )=0.4714 Vs
Vo(rms)
Io ( rms )=
R
For SPWM case with R load mode,
Vo ( rms )=0.625 Vs
Vo(rms)
Io ( rms )=
R
For SPWM case with RL load mode,
Vo ( rms )=0.625 Vs
Io ( rms ) is calculated by taking rms of ℱ expression
3.1. Three Phase Inverter with 120 and 180 Pulse Width:
In 120-degree mode, each switch conducts for 120 degrees. Conduction sequence of 06 switching
devices will be 16, 12, 23, 34, 45, and 56. For each 60-degree inverter any two of 06 switches will be on
as per sequence listed earlier. In 180-degree conduction mode, 03 switches will conduct simultaneously.
Two switches will be either from upper or lower les and other will be from remaining leg. Switching
sequence will be 612, 123, 234, 345, 456, and 561.
Figure 13: Three Phase Inverter with 120 and 180 Pulse Width
THD from RMS from 1st harmonic 3rd harmonic 5th harmonic
Simulation Simulation from simulation from simulation from simulation
Current (A) 31.09 16.33 22.05 0.006666 4.414
Voltage (V) 31.09 163.3 220.5 0.06666 44.14
Figure 14: Three Phase Inverter with 120 Pulse Width Output Voltage
Figure 15: Three Phase Inverter with 120 Pulse Width Gate Pulses
THD from RMS from 1st harmonic 3rd harmonic 5th harmonic
Simulation Simulation from simulation from simulation from simulation
Current (A) 31.07 18.86 25.47 0.01333 5.089
Voltage (V) 31.07 188.6 254.7 0.1333 50.89
Figure 16: Three Phase Inverter with 180 Pulse Width Output Voltage
Figure 17: Three Phase Inverter with 180 Pulse Width Gate Pulses
3.2. SPWM Three Phase Inverter with R load:
In Sinusoidal PWM, the width of each pulse is varied in proportion to the amplitude of the sine wave
evaluated at the center of the same pulse. The gating signals are generated by comparing a sinusoidal
reference wave with a triangular carrier wave. These modulated signals are then applied at gates of
three phase inverter’s switching devices.
THD from RMS from 1st harmonic 3rd harmonic 5th harmonic
Simulation Simulation from simulation from simulation from simulation
Current (A) 92.8 24.97 25.88 0.5014 0.2975
Voltage (V) 92.8 249.7 258.8 5.014 2.975
Figure 18: Three Phase Inverter with SPWM Output Voltage
THD from RMS from 1st harmonic 3rd harmonic 5th harmonic
Simulation Simulation from simulation from simulation from simulation
Current (A) 44.07 19.99 25.87 0.4992 0.2939
Voltage (V) 92.81 249.7 258.8 5.014 2.975
Figure 21: Three Phase Inverter with SPWM and RL load Output Voltage
3.4. Conclusion:
Three phase inverter produces higher output voltage. Three techniques are used to apply gate pulse at
switches. These are 120-degree pulse width, 180-degree pulse width and SPWM. 180-degree pulse
width produces higher output voltage than 120-degree pulses. Also for three phase inverter, 5 th
harmonic component is significant while 3rd harmonic component is negligible. With SPWM, overall RMS
output voltage is higher compared to previous modulation schemes but THD component is increased in
this scheme.
Lab 5
AC-AC Converters:
1. Introduction and Background:
AC-AC voltage controllers are circuits that convert AC input voltage into AC output voltage. They are
different from transformers in respect that, these circuits do not step up AC voltage and these can also
change frequency of AC input voltage along with phase on input voltage. There are different types of AC
controllers based upon method of control like indirect controllers, cycloconverters, matrix converters
etc. [3]
Methodology:
Circuits are simulated in MATLAB and also theoretical results are obtained with formulas.
Vo ( rms )=
Vm 1
√2 π √
π−α + (
sin 2 α
2 )
Vo ( rms )
Io ( rms )=
R
2
Po=Io ( rms ) R
Po
PF=
VsIs
For single phase controller (full wave) RL load
Vo ( rms )=
√
Vm 1
√2 π (
( β−α ) +
sin 2 α sin 2 β
2
−
2 )
Here, β is calculated by numerical methods
For 0≤α≤60
Vo ( rms )=√ 6 Vs
√(
1 π α sin 2 α
− +
π 6 4 8 )
For 60≤α≤90
Vo ( rms )=√ 6 Vs
√( 1 π 3 sin 2 α √ 3 cos 2 α
π 12
−
16
+
16 )
Vo ( rms )
Io ( rms )=
R
2
Po=3 Io ( rms ) R
Po
PF=
3 VsIs
For star connected configuration,
For 0≤α≤60
Vo ( rms )=Vs 1−
√ 3α 3
+
2π 4π
sin 2 α
For 60≤α≤90
Vo ( rms )=Vs
√ 1 3
+
2 4π
sin 2 α + sin ( 2α +60 )
Vo ( rms )
Io ( rms )=
R
2
Po=3 Io ( rms ) R
Po
PF=
3 VsIs
2.1. Single Phase:
Single phase voltage controllers use two SCRs that are connected anti parallel to each other but in series
with source voltage. During positive half cycle upper SCR conducts at a particular firing angle. Similarly,
during negative half cycle lower SCR conducts at 180+α.
Table 28: Single Phase AC-AC controller R load with firing angle of 60-degree
Two bridges of SCRs are connected parallel to voltage source. One is connected to positive and negative
terminals and other is connected oppositely.
Table 32: Single Phase AC-AC Cycloconverter with R load and 60 Degree Firing Angle
2.3. Conclusion:
RMS value of output voltage for controllers depend upon firing angle. As firing angle is increased value
of output voltage decreases. PF of circuit also decreases by increasing firing angle. With inductive load,
input current and useful active power is decreased compared to R load for same firing angle.
3. Three Phase AC-AC Voltage Controllers:
Three phase AC-AC voltage controller uses total 6 SCRs for conversion. A pair of SCRs connected anti-
parallel are used in each line. Gating sequence are so provided that at a time only two SCRs are turned
on at a time.
Table 36: Three Phase AC-AC Controller R Load and Firing Angle of 60
Figure 28: 3 Phase AC Voltage Controller with RL load 60 Degree Firing Angle
3.1. Conclusion:
Output voltage and PF are inversely related to firing angle. As firing is increased, output voltage and
power factor is decreased. Power factor of converter is further decreased for same firing angle as
compared with R load.