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DC-DC Converters

DC DC Converter

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Page 1: DC DC Converter

DC-DC Converters

Page 2: DC DC Converter

DC-DC ConvertersDC-DC converters are power electronic circuits that convert a DC

voltage to a different DC voltage level, often providing a regulated output.

A BASIC SWITCHING CONVERTERAn efficient alternative to the linear regulatorUses Power electronics switches like BJT,MOSFET IGBT…Also known as DC Chopper

Page 3: DC DC Converter

DC-DC Converters

Figure: (a) A basic DC-DC switching converter; (b) Switching

equivalent; ( c) Output voltage.

Assuming the switch is ideal• The output is the same as the

input when the switch ON• And the output is zero when the

switch OFF Periodic opening and closing of the

switch gives the pulsed output waveform.

The average or DC component of the output voltage is

Page 4: DC DC Converter

DC-DC ConvertersThe DC component of the output voltage will be less than or equal to

the input voltage for this circuit.ideal switch Zero loss Zero voltage across when ON Zero current

through it when OFFBut real switch has some power loss Considerable because it

creates heat on the switch.

Page 5: DC DC Converter

THE BUCK (STEP-DOWN) CONVERTER

Application Example: Controlling the speed of DC MotorLow-pass filter will be placed at the output

• The diode provides a path for the inductor current when the switch is opened and is reverse-biased when the switch is closed.

Page 6: DC DC Converter

THE BUCK (STEP-DOWN) CONVERTER

VOLTAGE AND CURRENT RELATIONSHIPS: in Fig. above, is when the switch is closed and is zero when the

switch is open, provided that the inductor current remains positive, keeping the diode on.

If the switch is closed periodically at a duty ratio D, the average voltage at the filter input is

An inductor current that remains positive throughout the switching period is known as continuous current.

Conversely, discontinuous current is characterized by the inductor current’s returning to zero during each period.

Page 7: DC DC Converter

THE BUCK (STEP-DOWN) CONVERTER

Buck converters and DC-DC converters in general, have the following properties when operating in the steady state

1. The inductor current is periodic.

2. The average inductor voltage is zero

3. The average capacitor current is zero

4. The power supplied by the source is the same as the power delivered to the load. For non-ideal components, the source also supplies the losses.

Page 8: DC DC Converter

THE BUCK (STEP-DOWN) CONVERTER

Assumptions for Analysis of Buck converter:• The circuit is operating in the steady state.• The inductor current is continuous (always positive)• The capacitor is very large, and the output voltage is held constant at

voltage Vo. This restriction will be relaxed later to show the effects of finite capacitance.• The switching period is; the switch is closed for time and open for time.• The components are ideal.

The key to the analysis for determining the output is to examine the inductor current and inductor voltage first for the switch closed and then for the switch open.

Page 9: DC DC Converter

THE BUCK (STEP-DOWN) CONVERTER

ANALYSIS FOR THE SWITCH CLOSED:• The voltage across the inductor is

• Rearranging,

Page 10: DC DC Converter

THE BUCK (STEP-DOWN) CONVERTER

ANALYSIS FOR THE SWITCH OPEN:• When the switch is open, the diode becomes forward-biased to carry the

inductor current • The voltage across the inductor when the switch is open is

• Rearranging,

• The derivative of current in the inductor is a negative constant, and the current decreases linearly

• The change in inductor current when the switch is open is

Page 11: DC DC Converter

THE BUCK (STEP-DOWN) CONVERTER

At steady state

• Solving for

• Therefore, the buck converter produces an output voltage that is less than or equal to the input.• An alternative derivation of the output voltage is based on the inductor voltage.• Since the average inductor voltage is zero for periodic operation

• Solving for .

Page 12: DC DC Converter

THE BUCK (STEP-DOWN) CONVERTER

The average inductor current must be the same as the average current in the load resistor, since the average capacitor current must be zero for steady-state operation.

The maximum and minimum values of the inductor current are computed as

Page 13: DC DC Converter

THE BUCK (STEP-DOWN) CONVERTER

where is the switching frequency.• The above Eq. can be used to determine the combination of L and f

that will result in continuous current. Since is the boundary between continuous and discontinuous current,

Page 14: DC DC Converter

THE BUCK (STEP-DOWN) CONVERTER

where is the minimum inductance required for continuous current.• In practice inductance is chosen greater than • The peak-to-peak variation in the inductor current is often used as a

design criterion in buck converter.• to determine the value of inductance for a specified peak-to-peak

inductor current for continuous-current operation:

Page 15: DC DC Converter

THE BUCK (STEP-DOWN) CONVERTER

• Since the converter components are assumed to be ideal, the power supplied by the source must be the same as the power absorbed by the load resistor.

• Basically from this expression we can say that DC-DC converter is DC transformer.

Page 16: DC DC Converter

THE BUCK (STEP-DOWN) CONVERTER

• OUTPUT VOLTAGE RIPPLE• In the preceding analysis, the capacitor was assumed to be

very large to keep the output voltage constant. • The variation in output voltage is computed from the

voltage-current relationship of the capacitor. • The current in the capacitor is

• While the capacitor current is positive, the capacitor is charging. From the definition of capacitance,

Page 17: DC DC Converter

THE BUCK (STEP-DOWN) CONVERTER

• The change in charge is the area of the triangle above the time axis

• resulting in

Page 18: DC DC Converter

THE BUCK (STEP-DOWN) CONVERTER

• Using =

• It is also useful to express the ripple as a fraction of the output voltage

Page 19: DC DC Converter

THE BUCK (STEP-DOWN) CONVERTER

• Using for

• It is also useful to express the ripple as a fraction of the output voltage

Page 20: DC DC Converter

CAPACITOR RESISTANCE—THE EFFECT ON RIPPLE VOLTAGE

The ESR may have a significant effect on the output voltage rippleA real capacitor can be modelled as a capacitance with an equivalent series resistance (ESR) and an equivalent series inductance (ESL).

ESR, often producing a ripple voltage greater than that of the ideal capacitance.

The inductance in the capacitor is usually not a significant factor at typical switching frequencies.

The ripple due to ESR can be approximated by first determining the ripple current assuming the capacitor ideal

Page 21: DC DC Converter

CAPACITOR RESISTANCE—THE EFFECT ON RIPPLE VOLTAGE

• The ripple voltage due to the ESR can be much larger than the ripple due to the pure capacitance.• In that case, the output capacitor is chosen on the basis of the

equivalent series resistance rather than capacitance only.

Page 22: DC DC Converter

SYNCHRONOUS RECTIFICATION FOR THE BUCK CONVERTER

Figure: A synchronous buck converter. The MOSFET S2 carries the inductor current

when S1 is off to provide a lower voltage drop than a diode.

Page 23: DC DC Converter

THE BOOST CONVERTERAssumptions1. Steady-state conditions exist.2. The switching period is, and the

switch is closed for time and open for.3. The inductor current is continuous

(always positive).4. The capacitor is very large, and the

output voltage is held constant at voltage.

5. The components are ideal.

Page 24: DC DC Converter

THE BOOST CONVERTER• ANALYSIS FOR THE SWITCH CLOSED:

• Solving for for the switch closed,

Page 25: DC DC Converter

THE BOOST CONVERTER• ANALYSIS FOR THE SWITCH OPEN:

• Solving for

Page 26: DC DC Converter

THE BOOST CONVERTERFor steady-state operation, the net change in inductor current must be

zero.

Solving for

Expressing the average inductor voltage over one switching period,

Page 27: DC DC Converter

THE BOOST CONVERTERAverage inductor current can be obtained by assuming Output power is

= Equating input and output powers

Page 28: DC DC Converter

THE BOOST CONVERTERA condition necessary for continuous inductor current is for to be

positive. Therefore, the boundary between continuous and discontinuous inductor

current is determined from

From a design perspective, it is useful to express in terms of a desired,

Page 29: DC DC Converter

THE BOOST CONVERTERThe peak-to-peak output voltage ripple can be calculated from the

capacitor current waveform.The change in capacitor charge can be calculated from

An expression for ripple voltage is then

where is the switching frequency.

Page 30: DC DC Converter

THE BOOST CONVERTERAs Buck Converter the voltage ripple due to the ESR is

Effects of Inductor Resistance • Inductors should be designed to have small resistance to minimize power loss and maximize

efficiency. • Inductor resistance affects performance of the boost converter, especially at high duty ratios.• For the boost converter, recall that the output voltage for the ideal case is

• The power supplied by the source must be the same as the power absorbed by the load and the inductor resistance, neglecting other losses.

where is the series resistance of the inductor.

Page 31: DC DC Converter

THE BOOST CONVERTER• The average diode current is

• Then • which becomes

• Substituting for

• Solving for,

Page 32: DC DC Converter

THE BOOST CONVERTER

Figure: Boost converter for a nonideal inductor. (a) Output voltage;

(b) Boost converter efficiency.

Page 33: DC DC Converter

BUCK-BOOST CONVERTER• The output voltage of the buck-boost converter can be either

higher or lower than the input voltage.• Assumptions :

1. The circuit is operating in the steady state.2. The inductor current is continuous.3. The capacitor is large enough to assume a constant output

voltage.4. The switch is closed for time and open for.5. The components are ideal.

Page 34: DC DC Converter

BUCK-BOOST CONVERTER

Figure: Buck-boost converter. (a)

Circuit; (b) Equivalent circuit for

the switch closed; (c) Equivalent

circuit for the switch open.

Page 35: DC DC Converter

BUCK-BOOST CONVERTER

Page 36: DC DC Converter

BUCK-BOOST CONVERTER• ANALYSIS FOR THE SWITCH

CLOSED:

ANALYSIS FOR THE SWITCH OPEN:

Page 37: DC DC Converter

BUCK-BOOST CONVERTER• For steady-state operation, the net change in inductor current

must be zero over one period.

• Solving for

• The required duty ratio for specified input and output voltages can be expressed as

Page 38: DC DC Converter

BUCK-BOOST CONVERTER• The average inductor voltage is zero for periodic operation,

resulting in

• Solving for yields

• The output voltage has opposite polarity from the source voltage.• If, the output voltage is larger than the input; and if, the output

is smaller than the input.

Page 39: DC DC Converter

BUCK-BOOST CONVERTER• Power absorbed by the load must be the same as that supplied by

the source, where

• Average source current is related to average inductor current by

• resulting in

• Substituting for and solving for , we find

Page 40: DC DC Converter

BUCK-BOOST CONVERTER

where is the switching frequency.

Page 41: DC DC Converter

BUCK-BOOST CONVERTER• OUTPUT VOLTAGE RIPPLE• The output voltage ripple for the buck-boost converter is

computed from the capacitor current .

• Solving for

Page 42: DC DC Converter

BUCK-BOOST CONVERTER• As is the case with other converters, the equivalent series resistance of

the capacitor can contribute significantly to the output ripple voltage. The peak-to-peak variation in capacitor current is the same as the maximum inductor current.

Page 43: DC DC Converter

BUCK-BOOST CONVERTER•As is the case with other converters, the equivalent series resistance of the capacitor can contribute significantly to the output ripple voltage. The peak-to-peak variation in capacitor current is the same as the maximum inductor current.

Page 44: DC DC Converter

Other Converter Topologies

CÚk Converter

Sepic Converter

Page 45: DC DC Converter

Other Converter Topologies

Full-bridge DC-DCConverter

Page 46: DC DC Converter

Other Converter TopologiesIsolated Full-bridge DC-DC Converter

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Other Converter Topologies

Isolated Half-bridge DC-DC Converter

Page 48: DC DC Converter

End of today’s session