Boost Regulator Average Output Voltage Expression Derivation and Duty Cycle

In this topic, you study How to derive an expression of Average Output voltage and Duty Cycle for Boost Regulator.


The boost regulator produces a higher average output voltage than the dc source input voltage. Let us assume large filter capacitance C connected across the load so that output voltage remains almost constant. The Resistive load is considered.

Circuit diagram

The working of a boost regulator is explained using the circuit diagram as shown in Figure 1. The switch ${S_1}$ shown in the circuit diagram can be a conventional thyristor i.e., SCR, a GTO thyristor, a power transistor, or a MOSFET.

Boost Regulator Circuit Diagram

Waveforms

The typical waveforms in the converter are shown in Figure 2.

boost Regulator Waveforms

Mode of Operation Interval 1: –

The time interval is 0  ≤  t ≤  ${T_{ON}}$. The switch ${S_1}$ is turned on. The circuit diagram for Mode of Operation Interval 1 is shown in Figure 3 and the corresponding waveforms are shown in Figure 2.

Circuit diagram of boost Regulator when switch S1 ON

Mode of Operation Interval 2: –

The time interval is ${T_{ON}}$ ≤ t ≤ ${T_{OFF}}$. The circuit diagram for Mode of Operation Interval 2 is shown in Figure 4 and the corresponding waveforms are shown in Figure 2.

Circuit diagram of boost Regulator when switch S1 OFF

The current passes through the capacitor as shown in Figure 4 can be find using KCL,

\[{i_C} = {i_L}\hspace{0.1cm} – \hspace{0.1cm}{i_O}\]

From the inductor voltage waveform, as shown in Figure 2, the equation for inductor voltage write as

\[{v_L} \hspace{0.1cm}= \hspace{0.1cm}-\hspace{0.1cm} ({V_O} \hspace{0.1cm}-\hspace{0.1cm} {V_S})\]

According to Faraday’s Law, the inductor volt-second product over a period T of steady-state operation is zero.

\[{({v_L})_{avg}} = 0\]

So apply Faraday’s Law, using the inductor voltage waveform, as shown in Figure 2, the inductor volt-second product over a period T equation write as

\[{V_S}\hspace{0.1cm}{T_{ON}}\hspace{0.1cm} – \hspace{0.1cm}({V_O}\hspace{0.1cm} – \hspace{0.1cm}{V_S})\hspace{0.1cm}{T_{OFF}}\hspace{0.1cm} = \hspace{0.1cm}0\]

In simplified form as

\[{V_S}\hspace{0.1cm}T\hspace{0.1cm} \hspace{0.1cm}= \hspace{0.1cm}{V_O}\hspace{0.1cm}{T_{OFF}}\]

\[{V_O}\hspace{0.1cm} =\hspace{0.1cm} \alpha \hspace{0.1cm}{V_S}….(1)\]

The turn – off time ${T_{OFF}}$ equation in terms of time period T and duty cycle $\alpha$ as

\[{T_{OFF}}\hspace{0.1cm} = \hspace{0.1cm}(1 – \alpha )\hspace{0.1cm}T….(2)\]

Put Equation 1 in Equation 2 gives

\[{V_S}\hspace{0.1cm}\hspace{0.1cm}T \hspace{0.1cm}=\hspace{0.1cm} {V_O}\hspace{0.1cm}(1 – \alpha )\hspace{0.1cm}T\]

or

\[{V_S} = {V_O}\hspace{0.1cm}(1 – \alpha )\]

\[{V_O} = \frac{{{V_S}}}{{(1 – \alpha )}}…(3)\]

Equation 3 describes the relationship between input dc source voltage and average output voltage in a boost converter.

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