Phase-Controlled Half-Wave Rectifier With Freewheeling Diode

In a half-controlled rectifier with an RL load and a freewheeling diode, the circuit configuration typically consists of a single-phase diode rectifier with an inductive load and an additional diode (freewheeling diode) connected in parallel with the load.

The freewheeling diode allows the inductive load to discharge its energy when the main thyristor(s) are turned off. This configuration is often used in applications where controlled rectification is needed, and the load has significant inductance.

Single Phase Half-controlled Rectifier RL Load With FD

Fig. 1. Single Phase Half-controlled Rectifier RL Load With FD

Circuit Components

Thyristor(s) (SCR): Thyristors are semiconductor devices that act as controlled rectifiers.

Diode (Freewheeling Diode): A diode connected in parallel with the load to provide a path for the inductive load current when the thyristor is off.

Inductive Load (RL): A load with inductance, such as a motor or a transformer.

Resistor (R): A resistor may be connected in series with the inductive load to limit the current.

Working of Half-controlled Rectifier RL Load With FD

a. Positive Half-Cycle:

During the positive half-cycle of the input AC voltage, the thyristor is triggered at α (firing angle) into conduction. The thyristor conducts, allowing the current to flow through the inductive load (RL) and the thyristor. The load current rises, and energy is stored in the inductor.

At the end of the positive half-cycle, the input voltage reverses polarity, causing the thyristor to naturally turn off (it is a half-controlled rectifier, so the thyristor only conducts during positive half-cycles).

When the thyristor turns off, the inductive load tries to maintain the current flow. However, since the thyristor is off, the freewheeling diode (FD) provides a path for the inductive current to circulate. The diode conducts, allowing the energy stored in the inductor to be released and the current to continue flowing through the load.

b. Negative Half-Cycle:

During the negative half-cycle of the input AC voltage, both the thyristor and the freewheeling diode FD are reverse-biased and, therefore, do not conduct. No current flows through the load during this half-cycle.

This configuration allows for controlled rectification during the positive half-cycles while providing a path for the inductive load current to circulate during the off periods (negative half-cycles) through the freewheeling diode. The resistor (R) can be added in series with the load to limit the current and control the circuit behavior further.

The circuit turn of time tc = π/ω

The SCR Conducts from α to 2π+ α to 3π and so on and FD is reverse biased during this condition.

The circuit’s voltage equation is stated as

Phase Controlled Half Wave Rectifier RL Load - 1

 θ = tan-1 (XL/R) and XL = ωl. Here, θ is the angle by which rms current Is lags Vs.

Half-Wave Rectifier With Freewheeling Diode in Power Electronics

Fig. 2. Half Controlled Rectifier Output RL Load With FD

Transient component it can be obtained by simplifying the following equation

Half-Wave Rectifier With Freewheeling Diode Formula - 1

During the negative cycle, the load current continuously conducts with the help freewheeling diode from π to 2π + α, 3π to 4π+ α and so on.

The load current equation during the Freewheeling diode period is given as

Half-Wave Rectifier With Freewheeling Diode Formula - 2

Analysis of Single-Phase Half-Controlled Rectifier With RL Load

The average load voltage Vo for the single-phase half-controlled rectifier is given by

Half-Wave Rectifier With Freewheeling Diode Formula - 3

The Load current IO is contributed by SCR from α to π, (2π + α) to 3π and so on, and by FD from 0 to α, it to (2π + α) and so forth. For ωt = α to π, (2π + α) to 3n, and so on, the waveshape of the thyristor current is the same as the waveshape of the io. Similar to this, for ωt = 0° to α, π to (2π + α), and so on, the waveform of the FD current, ifd, is the same as the waveform of the io.

While energy stored in the inductance L is returned to the source as power p2 for π to β (v0 is negative and i0 is positive), the load consumes power p1 from the source for α to π (both v0 and i0 are positive). Therefore, the difference between these two powers, p1 and p2, is the amount of net power used by the load.

For α to π, the load consumes energy, whereas for π to (2π + α), energy stored in L is transferred to the load resistance R via the FD. As a result, more electricity is used by the load. Therefore, it can be argued that using FD results in greater power being delivered to the load for the same firing angle.

With FD, the load current waveform is enhanced. Thus, utilizing a freewheeling diode has the following benefits:

  • An enhanced input PF
  • An improved load current waveform
  • Improved load performance.

The freewheeling diode prevents the load voltage v0 from going negative. FD kicks in whenever load voltage tends to drop. As a result, the load current is switched from the main thyristor to the FD, restoring the thyristor’s capacity for forward blocking.

As can be observed from the fig, the supply current is obtained from the source unidirectionally and as DC pulses. Thus, a single-phase half-wave converter adds a DC component to the supply line. This is bad since it causes the supply transformer to get saturated and other issues (harmonics, etc.).

Advantages of Half-Wave Rectifier With Freewheeling Diode

  • Half-controlled rectifiers are often more cost-effective than fully-controlled ones due to the reduced number of controlled components (typically only one thyristor).
  • They are simpler in design and control compared to fully controlled rectifiers, making them easier to implement and maintain.
  • The freewheeling diode provides a path for the inductive load current to circulate when the main thyristor is turned off. This helps reduce voltage spikes and improves the reliability of the circuit.
  • The presence of the inductive load (RL) can improve the power factor of the circuit. Inductive loads tend to offset the effects of capacitive loads, leading to a more balanced power factor.
  • The RL load helps in reducing the harmonic distortion in the output current waveform, leading to a smoother DC output.
  • The freewheeling diode provides a path for the inductive load current to circulate when the main thyristor is turned off. This helps reduce voltage spikes and improves the reliability of the circuit.

Disadvantages of Half-Wave Rectifier With Freewheeling Diode

  • The half-controlled rectifier can only control the positive half-cycle of the input AC waveform. This limitation might not be suitable for applications where precise control over the output is necessary.
  • Half-controlled rectifiers generally have lower efficiency compared to fully-controlled rectifiers, especially at lower loads. This is because only half of the input waveform is utilized, leading to higher conduction losses.
  • Half-controlled rectifiers are not suitable for applications where bidirectional power flow is required, as they can only be conducted in one direction.
  • The freewheeling diode aids in improving reliability, it adds complexity to the circuit, especially in terms of thermal management and protection mechanisms.

Matlab Code for Half-Wave Rectifier With Freewheeling Diode with RL Load

% Parameters

R = 10;                  % Load resistance (in ohms)

L = 0.1;                  % Load inductance (in Henrys)

Vrms = 230;          % RMS input voltage (in volts)

Frequency = 50;    % Frequency of the input AC voltage (in Hz)

Rf = 0.01;              % Freewheeling diode forward resistance (in ohms)

Vf = 0.7;                % Freewheeling diode forward voltage (in volts)

% Convert RMS voltage to peak voltage

Vpeak = Vrms * sqrt(2);

% Time vector

t = 0:1e-6:0.02;     % Time from 0 to 20 milliseconds with a step of 1 microsecond

% Input voltage (sinusoidal)

Vin = Vpeak * sin(2 * pi * Frequency * t);

% Half-controlled rectifier operation

alpha = 45;            

% Conduction angle (in degrees)

alpha_rad = deg2rad(alpha);

Vout = zeros(size(t));

% Rectifier operation based on conduction angle

for i = 1:length(t)

if Vin(i) * sin(alpha_rad) > 0

Vout(i) = Vin(i) * sin(alpha_rad);

else

Vout(i) = 0;

end

end

% Freewheeling diode operation

for i = 1:length(t)

if Vin(i) * sin(alpha_rad) <= 0

Vout(i) = Vf;

end

end

% Calculate current through RL load

I = Vout / (R + Rf) * exp(-Rf / L * t) .* (1 - exp(-L / (R + Rf) * t));

% Plot input voltage, output voltage, and load current

figure;

subplot(3,1,1);

plot(t, Vin, 'r');

title('Input Voltage');

xlabel('Time (s)');

ylabel('Voltage (V)');

subplot(3,1,2);

plot(t, Vout, 'b');

title('Output Voltage');

xlabel('Time (s)');

ylabel('Voltage (V)');

subplot(3,1,3);

plot(t, I, 'g');

title('Load Current');

xlabel('Time (s)');

ylabel('Current (A)');
Matlab Simulink Circuit of Half-controlled Rectifier RL Load With FD

Fig.3. Simulink Circuit of Half-controlled Rectifier RL Load With FD

Simulink Response of SCR Rectifier RL Load With FD

Fig.4 Simulink Response of Half-controlled Rectifier RL Load With FD

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