Thyristor-Gleichrichter
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Visão Geral
Source: Ali Bazzi, Department of Electrical Engineering, University of Connecticut, Storrs, CT.
Similar to diodes, thyristors, also called silicon controlled rectifiers (SCRs), pass current in one direction from the anode to cathode, and block current flow in the other direction. However, current passage can be controlled through a "gate" terminal, which requires a small current pulse to turn on the thyristor so it can start conducting.
Thyristors are four-layer devices, composed of alternating layers of n-type and p-type material, thereby forming PNPN structures with three junctions. The thyristor has three terminals; with the anode connected to the p-type material of the PNPN structure, the cathode connected to the n-type layer, and the gate connected to the p-type layer nearest the cathode.
The objective of this experiment is to study a controlled thyristor-based half-wave rectifier at different conditions, and understand how different timings of the gate pulse affect the DC output voltage.
Princípios
The thyristor only conducts under the same conditions as a diode, in addition to the condition of having a gate pulse to trigger the conduction process. For example, if an AC source is connected in series with a thyristor and a resistive load, the positive half-cycle of the source is not enough to forward bias the thyristor; the thyristor will remain reverse biased or off until a gate pulse is applied. It will then start conducting during that half-cycle. Thus, the thyristor has three terminals, the anode (A), cathode (K), and gate (G). Gate pulses are generated by "gate drive" circuits that drive current into the gate. The delay between the AC source zero crossing the gate pulse command is termed the "firing angle" which is an electrical angle.
Fig.1 shows a simple half-wave thyristor rectifier circuit with a pulse generating circuit (R1, R2, D1, D2, and C) that generates current pulses at the thyristor's gate. When the pulse is available and is "fired" at a firing angle which is a certain delay period from the zero crossing of the input voltage Vde, the thyristor acts like a diode in terms of passing current in one direction. Once the current goes to zero and the gate pulse is not available, the thyristor will remain off until the current is positive again and a gate pulse is fired.
In this experiment, we will study a controlled thyristor-based half-wave rectifier at different firing angles. The average output voltages for different angles are compared to study the effect of controlling the turn-on time on the average DC output voltage.
Figure 1: Half-wave rectifier with SCR and resistive load.
Procedimento
ATTENTION: During this experiment, do not touch any part of the circuit while energized. Do NOT ground the VARIAC.
For this experiment, the variable transformer (VARIAC) at a low frequency of 60 Hz and peak of 35 V is used as the main AC source.
1. Setup
- Before starting, connect the differential probe to one scope channel.
- Set the button on the differential probe to 1/20 (or 20X) attenuation.
- On the scope channel menu, set the probe to be at 10X unless 20X is available for the differential probe. If 10X is chosen, manually multiply any measurements or results by two to reach the 20X desired.
- To setup the VARIAC, make sure the VARIAC output (looks like a regular receptacle) is not connected to any cable.
- Keep the VARIAC OFF and make sure its knob is set to zero.
- Slowly adjust the VARIAC knob to around 15% output.
- Before connecting the differential probe to the circuit, tie the probe's terminals together and adjust its measured waveform on the screen to show zero offset voltage.
- Connect the output cable to the VARIAC, and the differential voltage probe across the VARIAC output banana plugs.
- Turn the VARIAC ON.
- Slightly adjust the VARIAC to achieve 35V peak.
- Take a copy of Vde to use for reference. Show two to five fundamental cycles.
- Turn the VARIAC OFF. Do not adjust its knob setting for the rest of the experiment.
2. Half-Wave Rectifier SCR Circuit with Resistive Load and Zero Firing Angle
- The main rectifier component is the SCR (S), which is a TYN058. The load resistor (R) is 51 Ω. The SCR control circuit is enclosed in the dotted box of Fig. 1.
- The control circuit uses diodes (1N4004), a 1 kΩ resistor (R1), a control resistor that is manually changed (R2), and a ceramic (no polarity) 1 µF capacitor (C).
- Make sure the SCR and diode polarities are correct. The dash on the diode is at the cathode while the SCR pin assignment is shown in Fig. 2.
- On the proto board, build the circuit shown in Fig. 1. Use a short circuit instead of R2.
- Connect the differential voltage probe across the load resistor to observe the output voltage, Vout.
- Turn the VARIAC ON.
- Adjust the time base on the scope to show Vout for the same number of fundamental cycles that were captured for Vde. Make a copy of the waveforms.
- Measure the average or mean Vout.
- Zoom in between the SCR turn-off point and the next SCR turn-on point. Measure the time difference using the scope cursors. Make a copy of the waveform.
- Keep the differential probe connection and other circuit connections the same for the next part.
- Turn OFF the VARIAC. Do NOT change the VARIAC voltage setting.
Figure 2: Pin assignment of the SCR.
3. Half-Wave Rectifier SCR Circuit with Resistive Load and Non-Zero Firing Angle
Two different resistors will be used as R2. The values should be between 100 and 1000 Ω. The resistance can read the resistance color code, or measured with a digital multimeter.
- Angle Setting #1 (small R2)
- Remove the short circuit, which was previously used instead of R2.
- Connect the small resistance value for R2.
- Turn the VARIAC ON.
- Adjust the time base on the scope to show Vout for the same number of fundamental cycles captured for Vde. Make a copy of the waveforms.
- Measure the average or mean Vout.
- Zoom in between the SCR turn-off point and the next SCR turn-on point. Measure the time difference using the scope cursors. Make a copy of the waveform.
- Keep the differential probe connection and other circuit connections the same for the next part.
- Turn OFF the VARIAC. Do NOT disassemble the circuit or change the VARIAC voltage setting.
- Angle Setting #2 (small R2)
- Replace R2 with the larger value resistor.
- Turn the VARIAC ON.
- Adjust the time base on the scope to show Vout for the same number of fundamental cycles captured for Vde. Make a copy of the waveforms.
- Measure the average or mean Vout.
- Zoom in between the SCR turn-off point and the next SCR turn-on point. Measure the time difference using the scope cursors. Make a copy of the waveform. The mean value should be what is expected from this equation:
<Vout>=V0[1+cos(α)]/(2π) (1)
which is slightly less than half the peak voltage of the input. - Turn OFF the VARIAC. Disassemble the circuit and return the VARIAC setting to zero.
Thyristors, also called silicon controlled rectifiers, or SCRs, are electronic devices used in light dimmers, motor speed controllers, and voltage regulators. Like a diode, a thyristor has an anode and a cathode, and conducts in only one direction. In fact, the schematic symbol for a thyristor resembles a diode, but with a third terminal representing the gate, which controls current flow. Unlike a diode, however, a small current pulse into the gate is required to switch the thyristor on so forward current can flow from anode to cathode. The thyristor switches off if this forward current drops below a latching threshold. In the off state, a thyristor blocks conduction in both directions. The ability to switch on and off allows the thyristor to rectify, that is to pass current of only one polarity and regulate the amount of AC power to allode. This video will demonstrate how to control a thyristor by triggering the gate at various points during an AC cycle.
Thyristors are composed of four alternating layers of P and N-type semiconductors, which form a PNPN structure. The anode lead is connected to the P-type material at one end. The cathode lead is connected to the N-type material at the other end. And the gate lead is connected to the P-type layer next to the cathode. In this simple circuit, with an AC power source in series with the thyristor and a load, the AC input by itself cannot drive the thyristor into forward conduction. Current can flow from anode to cathode only after a current pulse to the gate triggers the on state. This pulse must occur while the source voltage is positive. Otherwise, the thyristor remains off and blocks current. Thyristors are bi-stable, meaning they can rest in two different states. So the forward conducting mode persists as long as the source voltage is positive, and the current is above the latching threshold. If the current falls below this threshold, the thyristor enters the blocking mode and stays in that state until triggered again. The phase difference between the gate pulse and the zero crossing of a sinusoidal AC source is the firing angle. For example, a trigger pulse at the same time as the initial zero crossing has a firing angle of zero degrees, resulting in complete half-wave rectification, like a diode. In this case, the thyristor passes all the energy from the positive portion of the cycle to the load. If the pulse coincides with the peak of the AC voltage, the firing angle is 90 degrees, and the load receives energy from only half of the positive cycle. Finally, a pulse at the same time as the negative zero crossing results in a firing angle of 180 degrees, with no current conducted and no energy transferred at all. The objective of this experiment is to study a thyristor rectifier circuit triggered at different firing angles, and to compare the resulting average output voltages.
Because these experiments use 120 volt AC power, avoid contact with exposed wires, which may cause electrocution and injury or death. Do not touch any part of the circuit while it is energized, and do not ground the VARIAC. For more information about electrical safety, please watch the Jove Science Education video “Safety Precautions and Basic Equipment”. First, set up the oscilloscope by connecting the standard scope probe to one channel and the differential probe to a second channel. Configure the differential probe to one over 20 attenuation. Set the amplification on the oscilloscope menu for the differential probe channel. Use 20x if it is available for the differential probe. Otherwise, use 10x and double any oscilloscope measurements. Cancel any oscilloscope offset by clipping the differential probe terminals together and adjusting the traces vertical position to zero volts. During this experiment, the VARIAC provides AC voltage with a line frequency of 60 hertz. Before adjusting the VARIAC, make sure it is turned off and nothing is connected to the output. Then turn the control knob to 15 percent output. Connect the output cable to the VARIAC and connect the differential scope probe terminals to the banana plugs of the cable. Turn on the VARIAC, observe the waveform on the oscilloscope, and adjust the VARIAC so that the amplitude of it’s output V0 is 35 volts. Change the time base, that is the time interval per horizontal division of the oscilloscope to display two to five cycles of voltage. Capture and save a copy of this waveform and record this time base and designate it TB0 for later use. Finally, turn off the VARIAC, and do not change its setting.
This first experiment triggers a thyristor rectifier with a firing angle of zero degrees. Assemble the circuit as shown on a proto-board. Use the VARIAC for the input AC source V in. And a wire jumper in place of resistor R2. Connect the standard probe across input voltage V in, then connect the differential probe across load resistor R to observe output voltage V out. Turn on the VARIAC, and set the scope to time base TB0, which was recorded earlier. Because the firing angle is zero degrees, the thyristor acts like a diode, and the output voltage is a half-rectified sine wave. Use the scope’s built-in mathematical function to measure the mean output voltage. Adjust the time base to zoom in between the points when the thyristor turns off, then turns on again. Use the scope’s cursors to measure this time difference. Turn off the VARIAC, and do not change the voltage setting. Keep all VARIAC and scope connections the same for the next experiment.
To compare the results with two different non-zero firing angles, the next experiment will trigger the thyristor with a small, then a large resistance for R2. The resistances are, in this case, 300 ohms and 620 ohms. Use the smaller resistance to trigger the thyristor at a small firing angle. Remove the jumper that short-circuited R2. Then insert the 300 ohm resistor in its place. Turn on the VARIAC and set the scope to time base TB0. The firing angle is now greater than zero degrees, and, as a result, the thyristor is triggered later in the positive portion of the AC cycle. Measure the average output voltage as described earlier. Then zoom in and measure the time interval between when the thyristor turns off and back on. Turn off the VARIAC. Without changing the VARIAC setting or other connections, replace R2 with the larger resistor, and repeat the test. After the experiments are complete, turn off the VARIAC, set it to zero, and disassemble the circuit.
The output voltage of the thyristor rectifier circuit is zero until a gate pulse triggers the thyristor. After triggering, the output voltage is the remaining portion of a half-rectified wave. As the firing angle increases, the output voltage is more chopped compared to the input, and therefore the mean output voltage decreases. Consequently, the firing angle determines the amount of power a thyristor passes to the load.
Thyristors can control the amount of power transferred to a load, and were common in older adjustable DC power supplies. They are still used in many medium to high-voltage AC power control applications. First, common light dimmers used in homes and offices have a knob or slider than controls a potentiometer, which is a variable resistor. Changing the resistance changes the firing angle of a thyristor, and correspondingly increases or decreases the power that illuminates a light bulb. Anodic arc discharge is a practical and efficient means of synthesizing carbon nanotubes and graphene. Researches have used a magnetic field to enhance the controllability and flexibility of the process. The electrical discharge in this application is similar to that of arc welding. And both use high-voltage thyristors to control the power that creates the arc.
You have just watched Jove’s Introduction to Thyristor Rectifiers. You should now understand how thyristors work, and how they enable control of AC power to electrical devices. Thanks for watching.
Resultados
The AC input voltage waveform is chopped until the firing angle. Important relationships of the average output voltage and firing angles for different SCR rectifiers with input Vde= V0 cos(ωt) are:
• Single SCR and R load: <Vout>=V0[1+cos(α)]/(2π) (2)
• SCR bridge and R load: <Vout>= V0[1+cos(α)]/π (3)
• SCR bridge, current source load: <Vout>=2V0 cos(α)/π (4)
As the firing angle increases, the mean or DC voltage at the output decreases as the output voltage waveform across the resistive load is a chopped version of the input.
Applications and Summary
SCR's were common in older DC power supplies that required a variable DC output voltage from an AC input. By adjusting the resistor R2 in the above circuit, it is possible to adjust the average Vout and therefor an adjustable DC power supply results. SCRs are not common any more in DC power supplies as they switch at the input line frequency (typically 50 or 60 Hz), and new power supplies switch at 10 s or 100 s of kHz which makes filtering the output voltage to extract the DC component much easier with smaller capacitors. However, SCRs are still common in high voltage inverters where the switching frequency can be low at the line frequency since many high voltage and high current SCR's are available in the market.
Transcrição
Thyristors, also called silicon controlled rectifiers, or SCRs, are electronic devices used in light dimmers, motor speed controllers, and voltage regulators. Like a diode, a thyristor has an anode and a cathode, and conducts in only one direction. In fact, the schematic symbol for a thyristor resembles a diode, but with a third terminal representing the gate, which controls current flow. Unlike a diode, however, a small current pulse into the gate is required to switch the thyristor on so forward current can flow from anode to cathode. The thyristor switches off if this forward current drops below a latching threshold. In the off state, a thyristor blocks conduction in both directions. The ability to switch on and off allows the thyristor to rectify, that is to pass current of only one polarity and regulate the amount of AC power to allode. This video will demonstrate how to control a thyristor by triggering the gate at various points during an AC cycle.
Thyristors are composed of four alternating layers of P and N-type semiconductors, which form a PNPN structure. The anode lead is connected to the P-type material at one end. The cathode lead is connected to the N-type material at the other end. And the gate lead is connected to the P-type layer next to the cathode. In this simple circuit, with an AC power source in series with the thyristor and a load, the AC input by itself cannot drive the thyristor into forward conduction. Current can flow from anode to cathode only after a current pulse to the gate triggers the on state. This pulse must occur while the source voltage is positive. Otherwise, the thyristor remains off and blocks current. Thyristors are bi-stable, meaning they can rest in two different states. So the forward conducting mode persists as long as the source voltage is positive, and the current is above the latching threshold. If the current falls below this threshold, the thyristor enters the blocking mode and stays in that state until triggered again. The phase difference between the gate pulse and the zero crossing of a sinusoidal AC source is the firing angle. For example, a trigger pulse at the same time as the initial zero crossing has a firing angle of zero degrees, resulting in complete half-wave rectification, like a diode. In this case, the thyristor passes all the energy from the positive portion of the cycle to the load. If the pulse coincides with the peak of the AC voltage, the firing angle is 90 degrees, and the load receives energy from only half of the positive cycle. Finally, a pulse at the same time as the negative zero crossing results in a firing angle of 180 degrees, with no current conducted and no energy transferred at all. The objective of this experiment is to study a thyristor rectifier circuit triggered at different firing angles, and to compare the resulting average output voltages.
Because these experiments use 120 volt AC power, avoid contact with exposed wires, which may cause electrocution and injury or death. Do not touch any part of the circuit while it is energized, and do not ground the VARIAC. For more information about electrical safety, please watch the Jove Science Education video “Safety Precautions and Basic Equipment”. First, set up the oscilloscope by connecting the standard scope probe to one channel and the differential probe to a second channel. Configure the differential probe to one over 20 attenuation. Set the amplification on the oscilloscope menu for the differential probe channel. Use 20x if it is available for the differential probe. Otherwise, use 10x and double any oscilloscope measurements. Cancel any oscilloscope offset by clipping the differential probe terminals together and adjusting the traces vertical position to zero volts. During this experiment, the VARIAC provides AC voltage with a line frequency of 60 hertz. Before adjusting the VARIAC, make sure it is turned off and nothing is connected to the output. Then turn the control knob to 15 percent output. Connect the output cable to the VARIAC and connect the differential scope probe terminals to the banana plugs of the cable. Turn on the VARIAC, observe the waveform on the oscilloscope, and adjust the VARIAC so that the amplitude of it’s output V0 is 35 volts. Change the time base, that is the time interval per horizontal division of the oscilloscope to display two to five cycles of voltage. Capture and save a copy of this waveform and record this time base and designate it TB0 for later use. Finally, turn off the VARIAC, and do not change its setting.
This first experiment triggers a thyristor rectifier with a firing angle of zero degrees. Assemble the circuit as shown on a proto-board. Use the VARIAC for the input AC source V in. And a wire jumper in place of resistor R2. Connect the standard probe across input voltage V in, then connect the differential probe across load resistor R to observe output voltage V out. Turn on the VARIAC, and set the scope to time base TB0, which was recorded earlier. Because the firing angle is zero degrees, the thyristor acts like a diode, and the output voltage is a half-rectified sine wave. Use the scope’s built-in mathematical function to measure the mean output voltage. Adjust the time base to zoom in between the points when the thyristor turns off, then turns on again. Use the scope’s cursors to measure this time difference. Turn off the VARIAC, and do not change the voltage setting. Keep all VARIAC and scope connections the same for the next experiment.
To compare the results with two different non-zero firing angles, the next experiment will trigger the thyristor with a small, then a large resistance for R2. The resistances are, in this case, 300 ohms and 620 ohms. Use the smaller resistance to trigger the thyristor at a small firing angle. Remove the jumper that short-circuited R2. Then insert the 300 ohm resistor in its place. Turn on the VARIAC and set the scope to time base TB0. The firing angle is now greater than zero degrees, and, as a result, the thyristor is triggered later in the positive portion of the AC cycle. Measure the average output voltage as described earlier. Then zoom in and measure the time interval between when the thyristor turns off and back on. Turn off the VARIAC. Without changing the VARIAC setting or other connections, replace R2 with the larger resistor, and repeat the test. After the experiments are complete, turn off the VARIAC, set it to zero, and disassemble the circuit.
The output voltage of the thyristor rectifier circuit is zero until a gate pulse triggers the thyristor. After triggering, the output voltage is the remaining portion of a half-rectified wave. As the firing angle increases, the output voltage is more chopped compared to the input, and therefore the mean output voltage decreases. Consequently, the firing angle determines the amount of power a thyristor passes to the load.
Thyristors can control the amount of power transferred to a load, and were common in older adjustable DC power supplies. They are still used in many medium to high-voltage AC power control applications. First, common light dimmers used in homes and offices have a knob or slider than controls a potentiometer, which is a variable resistor. Changing the resistance changes the firing angle of a thyristor, and correspondingly increases or decreases the power that illuminates a light bulb. Anodic arc discharge is a practical and efficient means of synthesizing carbon nanotubes and graphene. Researches have used a magnetic field to enhance the controllability and flexibility of the process. The electrical discharge in this application is similar to that of arc welding. And both use high-voltage thyristors to control the power that creates the arc.
You have just watched Jove’s Introduction to Thyristor Rectifiers. You should now understand how thyristors work, and how they enable control of AC power to electrical devices. Thanks for watching.