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Zener Diode

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What is Zener Diode?

A Zener diode is a semiconductor device that makes the current flow in the forward or in the backward direction. The diode usually consists of a p-n junction which is heavily doped. The diode is designed to conduct the flow of current in the reverse direction after reaching a specified voltage.


The Zener diode has a reverse-breakdown voltage at which the diode starts conductivity electric current, and remains continuous in the reverse-bias mode. The voltage drop across the diode always remains constant irrespective of the applied voltage, and this feature of the Zener diode makes it suitable for voltage regulation.


Zener Diode Explanation

Zener diode that is also known as breakdown diode is a heavily doped semiconductor device that has been specially designed to operate in the reverse direction. When the potential reaches the Zener voltage which is also known as Knee voltage and the voltage across the terminal of the Zener diode is reversed, at that point of time, the junction breaks down and the current starts flowing in the reverse direction. This effect is known as the Zener effect.


Zener Diode Circuit Diagram

The above figure is the circuit diagram of the Zener diode. The Zener diode has its application in reverse biassing. In reverse biassing, the P-type material of the diode is connected with the negative terminal of the supply, and the n-type material is connected with the positive terminal of the supply. The diode consists of a very thin depletion region as it is made up of heavily doped semiconductor material.


Zener Diode Working

In a Zener diode, high-level impurities are added to the semiconductor material to make it more conductive. Due to the presence of these impurities, the depletion region of the diode becomes very thin. The intensity of the electric field is increased across the depletion region, due to heavy doping even if a small voltage is applied.


When no biassing is applied across the Zener diode, the electrons accumulate in the valence band of the p-type semiconductor material and no current flow occurs through the diode. The band in which the valence electrons are present is called the valence band electron. When external energy is applied across the valence band, the electrons get easily moved from one band to another.


When the reverse bias is applied across the diode and when the Zener voltage is equal to that of the supplied voltage, the diode starts conducting in the direction of reverse bias. The Zener diode voltage is the particular voltage at which the depletion region vanishes completely.


The intensity of the electric field increases across the depletion region when the reverse bias is applied across the diode. Hence, the electrons are free to move from the valence band of the P-type semiconductor material to the conduction band of the N-type semiconductor material. This movement of electrons decreases the barrier between p-type and n-type materials. Once the depletion region vanishes completely, the diode starts conducting current in the reverse bias direction.


Zener Diode Working in Reverse Biased

When it is in forwarding, the biased Zener diode operates just like any other normal diode. But a small leakage current flows through the diode when it is connected in reverse biassed mode. As the reverse voltage starts increasing and finally reaches the predetermined breakage voltage which is represented as Vz the current starts flowing through the circuit. It is determined by a series of resistors after the current increases to its maximum limit after which it remains constant over a wide range of applied voltage as it gets stabilised.


Types of a Breakdown of Zener Diode

There are two types of breakdown that can be observed for a Zener diode:

  1. Avalanche Breakdown:

    1. At high reverse voltage, Avalanche breakdown occurs both in the normal diode as well as Zener diode. The free electrons gain efficient energy and accelerate to the high velocity when a high value of reverse voltage is applied to the PN junction. These high-velocity electrons then collide with the other atoms and knock off the electrons of those atoms. 

    2. Due to the constant collision of the electrons with new atoms, a large number of free electrons has generated that result in electric current that increases rapidly in the diode. 

    3. Though this phenomenon of a sudden spike of the electric current may permanently destroy the normal diode, the Zener diode is designed to operate under this kind of voltage breakdown and can withstand a spike of current suddenly. 

    4. With Zener voltage (Vz) greater than 6V, the avalanche breakdown happens in the Zener diode.

  2. Zener Breakdown:

    1. When the reverse bias voltage which is applied reaches closer to the Zener voltage, the depleting electric field in the region gets stronger enough to pull electrons from the valence band. 

    2. This valence electron then gains a high amount of energy from a strong electric field of the depletion region and breaks free from the parent atom. 

    3. Therefore, in the Zener breakdown region, a small increase in the voltage results in a sudden spike of the electric current.


VI Characteristics of Zener Diode

The VI characteristics of the Zener diode is described through the graph, mentioned in the figure below. This shows that the Zener diode behaves like an ordinary diode when it is connected in forward bias. But when the reverse voltage is applied across the Zener diode, such that the reverse voltage rises beyond the predetermined rating, breakdown occurs on the Zener diode.


The electric current starts to flow in the reverse direction at the breakdown voltage of the Zener diode. The graph represents that the Zener diode has resistance. Further, it is shown that the graph of Zener breakdown is not exactly vertical. The voltage across the Zener diode is represented by the equation given below:


V = VZ + IZRZ


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Applications of Zener Diode

The major use of Zener diode is in industrial and commercial applications. Below are some of the important applications of the Zener diode.


As Voltage Stabiliser – The Zener diode is used for voltage regulation. It converts the fluctuating voltage of the source to a constant voltage and supplies it to the load. The Zener diode is always connected in parallel with the load, and it maintains a constant voltage VZ, thus stabilising the voltage.


For Metre Protection – In multimeters, the Zener diode is used to control the movement of the metre against any accidental overloads. The multimeter is connected in parallel with the Zener diode. When the overload occurs across the diode, the major amount of current passes through the diode, and in this way, the diode protects the metre from damage.


For Wave Shaping – A sine wave is converted into a square wave by using the Zener diode. This is done by connecting two Zener Diodes in series with the resistance of the circuit. It should be noted that the diode must be connected back to back and in the opposite direction to each other.

FAQs on Zener Diode

1. What is a Zener diode and how is it different from a normal p-n junction diode?

A Zener diode is a special type of semiconductor diode designed to operate continuously in the reverse breakdown region. Unlike a normal p-n junction diode, which can be permanently damaged by a reverse breakdown current, a Zener diode is specifically fabricated to handle it. The key difference lies in the doping concentration; Zener diodes are much more heavily doped than normal diodes, which creates a very thin depletion region and enables the unique Zener effect.

2. What is the circuit symbol for a Zener diode and what does it signify?

The circuit symbol for a Zener diode is similar to that of a normal diode, but with small, bent lines on the end of the perpendicular bar, often resembling the letter 'Z'. The anode (A) is represented by the flat base of the triangle, and the cathode (K) is the 'Z' shaped bar. This unique symbol immediately indicates that the component is designed for reverse-bias operation, its primary functional mode in circuits.

3. What are the main applications of a Zener diode in electronic circuits?

Due to its ability to maintain a constant voltage under reverse breakdown, the Zener diode has several important applications. The most common uses include:

  • Voltage Regulation: To provide a stable DC voltage from a fluctuating source, which is its primary application.
  • Overvoltage Protection: To protect sensitive circuits from sudden voltage spikes by shunting excess current to the ground.
  • Wave Shaping: To clip or limit parts of an AC waveform, for instance, in converting a sine wave into a square wave.
  • Voltage Reference: To provide a stable and known reference voltage in electronic circuits like power supplies and measurement instruments.

4. How does a Zener diode work as a voltage regulator?

To function as a voltage regulator, a Zener diode is connected in reverse bias, parallel to the load that requires a constant voltage. A series resistor is placed before the diode to limit the input current. When the input voltage rises above the diode's breakdown voltage, the excess current flows through the Zener diode instead of the load. This ensures the voltage across the load remains constant and stable at the Zener voltage (Vz), effectively regulating the output.

5. What are the V-I characteristics of a Zener diode?

The V-I (Voltage-Current) characteristics of a Zener diode show its behaviour under different biasing conditions.

  • Forward Bias: In the forward-biased region, it behaves just like a normal p-n junction diode. Current starts to increase significantly after crossing the knee voltage (typically ~0.7V for silicon).
  • Reverse Bias: In the reverse-biased region, a very small leakage current flows until the voltage reaches the breakdown voltage (Vz). At this specific voltage, the current increases sharply while the voltage across the diode remains almost constant. This sharp bend in the graph is known as the "Zener knee," and the stable voltage in this region is its key operational feature.

6. Why is a Zener diode always operated in reverse bias for its main applications?

A Zener diode is used in reverse bias because its unique voltage-stabilising property only manifests in the reverse breakdown region. When forward-biased, it acts like any standard diode, where the voltage drop is small and not precisely regulated. However, in reverse bias, once its specific Zener voltage (Vz) is reached, it can conduct a wide range of currents while keeping the voltage across itself almost perfectly constant. This unique stability against current changes is what makes it an effective voltage regulator and reference device.

7. What is the fundamental difference between Zener breakdown and Avalanche breakdown?

Both are mechanisms for reverse breakdown in a p-n junction, but they are caused by different physical phenomena and occur under different conditions:

  • Zener Breakdown: This mechanism dominates in diodes that are heavily doped and have a narrow depletion region. It occurs at lower reverse voltages (typically below 6V). The intense electric field across the thin depletion region is strong enough to directly break covalent bonds and generate a large current.
  • Avalanche Breakdown: This mechanism dominates in diodes that are lightly doped with a wider depletion region, occurring at higher reverse voltages (typically above 6V). Minority charge carriers are accelerated by the high voltage, gaining enough kinetic energy to collide with and knock out more electrons, leading to a rapid multiplication or "avalanche" of charge carriers.

8. Why is heavy doping essential for the functioning of a Zener diode?

Heavy doping is the most critical aspect of a Zener diode's construction because it leads to a very narrow depletion region. According to physics principles, a narrow region results in an extremely strong internal electric field, even with a low reverse voltage. This intense electric field is the key to enabling the Zener effect, where the field becomes strong enough to pull electrons directly from their covalent bonds, allowing the diode to conduct a controlled current in reverse bias at a precise, predetermined voltage.