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Home » GATE Study Material » Electronics and Telecommunications » Electronic Components » The Thyristor or Silicon Controlled Rectifier (SCR)

The Thyristor or Silicon Controlled Rectifier (SCR)

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The Thyristor or Silicon Controlled Rectifier (SCR)

Thyristor

- or as it is also known the silicon controlled rectifier (SCR)

Thyristors or silicon controlled rectifiers (SCR) are find many uses in electronics, and in particular for power control. Indeed thyristors have been called the workhorse of high power electronics. Here the silicon controlled rectifiers are able to switch large levels of power are used in a wide variety of different applications. Thyristors even finds uses in low power electronics where they are able to find applications in many circuits from light dimmers to power supply over voltage protection.

 

Discovery


The idea for the thyristor or silicon controlled rectifier (SCR) was first described by Shockley in 1950. It was referred to as a bipolar transistor with a p-n hook-collector. The mechanism for the operation of the thyristor was analysed further in 1952 by Ebers. Then in 1956 Moll investigated the switching mechanism of the thyristor. Development continued and more was learned about the device such that the first silicon controlled rectifiers became available in the early 1960s where it started to gain a significant level of popularity for power switching.

 

Structure


The thyristor consists of a four layer p-n-p-n structure with the outer layers are referred to as the anode (n-type) and cathode (n-type). The control terminal of the SCR is named the gate and it is connected to the p-type layer located next to the cathode.

Structure of a thyristor or silicon controlled rectifier (SCR)

Structure of a thyristor or silicon controlled rectifier (SCR)

The level of doping varies between the different layers of the thyristor. The cathode is the most heavily doped. The gate and anode are the next heavily doped. The lowest doping level is within the central n type layer. This is also thicker than the other layers and these two factors enable a large blocking voltage to be supported. Thinner layers would mean that the device would break down at lower voltages.

In view of the very high currents and power levels that some thyristors are used to switch, thermal considerations are of paramount importance. The anode of the SCR or silicon controlled rectifier is usually bonded to the package since the gate terminal is near the cathode and needs to be connected separately. This is accomplished in such a way that heat is removed from the silicon to the package. Apart from the internal considerations, the external heat-sinking considerations for the thyristor must be carefully implemented otherwise the device may overheat and fail.

Thyristors are usually manufactured from silicon. There are two main reasons for this. One is the voltage, current and thermal handling properties of silicon enable it to meet the requirements of the power industry, and secondly silicon technology is well developed and very cheap to use.

 

Operation


In operation the SCR may be considered as two back to back transistors. The transistor with its emitter connected to the cathode of the thyristor is a n-p-n device whereas the transistor with its emitter connected to the anode of the SCR is a p-n-p variety. The gate is connected to the base of the n-p-n transistor.

Equivalent circuit of a thyristor or silicon controlled rectifier (SCR)

Equivalent circuit of a thyristor or silicon controlled rectifier (SCR)

This arrangement forms a positive feedback loop within the thyristor. The output of one transistor fed to the input of the second. In turn the output of the second transistor is fed back to the input of the first. As a result it can be seen that the total current gain of the device exceeds one. This means that when a current starts to flow, it quickly builds up until both transistors are fully turned on or saturated.

When a voltage is applied across a thyristor no current flows because neither transistor is conducting. As a result there is no complete path across the device. If a small current is passed through the gate electrode, this will turn "on" the transistor TR2. When this occurs it will cause the collector of TR2 to fall towards the voltage on the emitter, i.e. the cathode of the whole device. When this occurs it will cause current to flow through the base of TR1 and turn this transistor "on". Again this will now try to pull the voltage on the collector of TR1 towards its emitter voltage. This will cause current to flow in the emitter of TR2, causing its "on" state to be maintained. In this way it only requires a small trigger pulse on the gate to turn the thyristor on. Once switched on, the thyristor can only be turned off by removing the supply voltage.



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