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Submitted by: Dhruv Singh(2K20/EE/93)
Gaurav(2K20/EE/102)
Deepak Kumar(2K20/EE/86)
Deepak Modi(2K20/EE/87)
Himanshu Katawalia(2K20/EE/126)
The input voltage source is connected to a controllable solid state device
which operates as a switch. The solid state device can be a Power
MOSFET or IGBT. Thyristors are not used generally for DC- DC
converters because to turn off a Thyristor in a DC-DC circuit requires
another commutation which involves using another Thyristor, whereas
Power MOSFET and IGBT can be turned off by simply having the
voltage between the GATE and SOURCE terminals of a Power
MOSFET, or, the GATE and COLLECTOR terminals of the IGBT go to
zero.
The second switch used is a diode. The switch and the diode are
connected to a low-pass LC filter which is appropriately designed to
reduce the current and voltage ripples. The load is a purely resistive load.
The input voltage is constant and the current through load is also
constant. The load can be seen as current source.
The controlled switch is turned on and off by using Pulse Width
Modulation(PWM). PWM can be time based or frequency based.
Frequency based modulation has disadvantages like a wide range of
frequencies to achieve the desired control of the switch which in turn will
give the desired output voltage. This leads to a complicated design for
the low-pass LC filter which would be required to handle a large range of
frequencies.
Time based Modulation is mostly used for DC-DC converters. It is
simple to construct and use. The frequency remains constant in this
type of PWM modulation.
The Buck converter has two modes of operation. The first mode is
when the switch is on and conducting.
Mode I : Switch is ON, Diode is OFF
The voltage across the capacitance in steady state is equal to the output voltage.
Let us say the switch is on for a time TON and is off for a time TOFF. We define the time
period, T, as
and the switching frequency,
Let us now define another term, the duty cycle,
Let us analyse the Buck converter in steady state operation for this mode
using KVL.
Since the switch is closed for a time TON = DT we can say that Δt = DT.
While performing the analysis of the Buck converter, we have to keep in
mind that
1.The inductor current is continuous and, this is made possible by
selecting an appropriate value of L.
2.The inductor current in steady state rises from a value with a positive
slope to a maximum value during the ON state and then drops back down
to the initial value with a negative slope. Therefore the net change of the
inductor current over anyone complete cycle is zero.
Mode II: Switch is OFF, Diode is ON
Here, the energy stored in the inductor is released and is ultimately
dissipated in the load resistance, and this helps to maintain the flow of
current through the load. But for analysis we keep the original conventions
to analyse the circuit using KVL.
Let us now analyse the Buck converter in steady state operation
for Mode II using KVL.
Since the switch is open for a time
we can say that Δt = (1- D)T.
It is already established that the net change of the inductor current over
anyone complete cycle is zero.
The input voltage source is connected to an inductor. The solid- state
device which operates as a switch is connected across the source. The
second switch used is a diode. The diode is connected to a capacitor,
and the load and the two are connected in parallel as shown in the
figure above.
The inductor connected to input source leads to a constant input
current, and thus the Boost converter is seen as the constant current
input source. And the load can be seen as a constant voltage source.
The controlled switch is turned on and off by using Pulse Width
Modulation(PWM). PWM can be time-based or frequency based.
Frequency-based modulation has disadvantages like a wide range of
frequencies to achieve the desired control of the switch which in turn
will give the desired output voltage.
Time-based Modulation is mostly used for DC-DC converters. It is
simple to construct and use. The frequency remains constant in this
type of PWM modulation. The Boost converter has two modes of
operation. The first mode is when the switch is on and conducting.
Mode I : Switch is ON, Diode is OFF
The Switch is ON and therefore represents a short circuit ideally offering
zero resistance to the flow of current so when the switch is ON all the
current will flow through the switch and back to the DC input source. Let
us say the switch is on for a time TON and is off for a time TOFF. We define
the time period, T, as
and the switching frequency,
Let us now define another term, the duty cycle,
Let us analyze the Boost converter in steady state operation for this mode
using KVL.
Since the switch is closed for a time TON = DT we can say that Δt =DT.
Mode II : Switch is OFF, Diode is ON
In this mode, the polarity of the inductor is reversed. The energy stored in
the inductor is released and is ultimately dissipated in the load resistance,
and this helps to maintain the flow of current in the same direction
through the load and also step-up the output voltage as the inductor is
now also acting as a source in conjunction with the input source.
But for analysis, we keep the original conventions to analyze the
circuit using KVL.
Let us now analyse the Boost converter in steady state operation for
Mode II using KVL.
Since the switch is open for a time
we can say that
It is already established that the net change of the inductor current over
any one complete cycle is zero.
CS.PROJECT.pptx
CS.PROJECT.pptx
CS.PROJECT.pptx
CS.PROJECT.pptx
CS.PROJECT.pptx
CS.PROJECT.pptx

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CS.PROJECT.pptx

  • 1. Submitted by: Dhruv Singh(2K20/EE/93) Gaurav(2K20/EE/102) Deepak Kumar(2K20/EE/86) Deepak Modi(2K20/EE/87) Himanshu Katawalia(2K20/EE/126)
  • 2.
  • 3.
  • 4. The input voltage source is connected to a controllable solid state device which operates as a switch. The solid state device can be a Power MOSFET or IGBT. Thyristors are not used generally for DC- DC converters because to turn off a Thyristor in a DC-DC circuit requires another commutation which involves using another Thyristor, whereas Power MOSFET and IGBT can be turned off by simply having the voltage between the GATE and SOURCE terminals of a Power MOSFET, or, the GATE and COLLECTOR terminals of the IGBT go to zero. The second switch used is a diode. The switch and the diode are connected to a low-pass LC filter which is appropriately designed to reduce the current and voltage ripples. The load is a purely resistive load.
  • 5. The input voltage is constant and the current through load is also constant. The load can be seen as current source. The controlled switch is turned on and off by using Pulse Width Modulation(PWM). PWM can be time based or frequency based. Frequency based modulation has disadvantages like a wide range of frequencies to achieve the desired control of the switch which in turn will give the desired output voltage. This leads to a complicated design for the low-pass LC filter which would be required to handle a large range of frequencies. Time based Modulation is mostly used for DC-DC converters. It is simple to construct and use. The frequency remains constant in this type of PWM modulation. The Buck converter has two modes of operation. The first mode is when the switch is on and conducting.
  • 6. Mode I : Switch is ON, Diode is OFF The voltage across the capacitance in steady state is equal to the output voltage. Let us say the switch is on for a time TON and is off for a time TOFF. We define the time period, T, as and the switching frequency,
  • 7. Let us now define another term, the duty cycle, Let us analyse the Buck converter in steady state operation for this mode using KVL. Since the switch is closed for a time TON = DT we can say that Δt = DT.
  • 8. While performing the analysis of the Buck converter, we have to keep in mind that 1.The inductor current is continuous and, this is made possible by selecting an appropriate value of L. 2.The inductor current in steady state rises from a value with a positive slope to a maximum value during the ON state and then drops back down to the initial value with a negative slope. Therefore the net change of the inductor current over anyone complete cycle is zero.
  • 9. Mode II: Switch is OFF, Diode is ON Here, the energy stored in the inductor is released and is ultimately dissipated in the load resistance, and this helps to maintain the flow of current through the load. But for analysis we keep the original conventions to analyse the circuit using KVL. Let us now analyse the Buck converter in steady state operation for Mode II using KVL.
  • 10. Since the switch is open for a time we can say that Δt = (1- D)T. It is already established that the net change of the inductor current over anyone complete cycle is zero.
  • 11.
  • 12. The input voltage source is connected to an inductor. The solid- state device which operates as a switch is connected across the source. The second switch used is a diode. The diode is connected to a capacitor, and the load and the two are connected in parallel as shown in the figure above. The inductor connected to input source leads to a constant input current, and thus the Boost converter is seen as the constant current input source. And the load can be seen as a constant voltage source. The controlled switch is turned on and off by using Pulse Width Modulation(PWM). PWM can be time-based or frequency based. Frequency-based modulation has disadvantages like a wide range of frequencies to achieve the desired control of the switch which in turn will give the desired output voltage.
  • 13. Time-based Modulation is mostly used for DC-DC converters. It is simple to construct and use. The frequency remains constant in this type of PWM modulation. The Boost converter has two modes of operation. The first mode is when the switch is on and conducting. Mode I : Switch is ON, Diode is OFF
  • 14. The Switch is ON and therefore represents a short circuit ideally offering zero resistance to the flow of current so when the switch is ON all the current will flow through the switch and back to the DC input source. Let us say the switch is on for a time TON and is off for a time TOFF. We define the time period, T, as and the switching frequency, Let us now define another term, the duty cycle,
  • 15. Let us analyze the Boost converter in steady state operation for this mode using KVL. Since the switch is closed for a time TON = DT we can say that Δt =DT.
  • 16. Mode II : Switch is OFF, Diode is ON In this mode, the polarity of the inductor is reversed. The energy stored in the inductor is released and is ultimately dissipated in the load resistance, and this helps to maintain the flow of current in the same direction through the load and also step-up the output voltage as the inductor is now also acting as a source in conjunction with the input source.
  • 17. But for analysis, we keep the original conventions to analyze the circuit using KVL. Let us now analyse the Boost converter in steady state operation for Mode II using KVL. Since the switch is open for a time we can say that
  • 18. It is already established that the net change of the inductor current over any one complete cycle is zero.