Zener Diode | Definition | Working Principle | Characteristics | Applications

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Similar to the ordinary diode, there are other types of diodes that are commonly and frequently used in electronic circuits for industrial and domestic applications. One of these is the Zener diode.


The Zener diode is a special type of diode that is designed to work in reverse bias and in the so-called Zener region of the diode characteristic curve. This region is after the reverse-biased voltage has exceeded the breakdown voltage (breakdown point).

Zener Diode Working Principle

If the reverse bias voltage is less than the breakdown voltage, or if the Zener diode is forward biased, it acts as an ordinary diode. That is, in forward bias it allows current, and in reverse bias it blocks current. After this voltage has surpassed the breakdown point (in reverse bias), the diode falls in the Zener region, where it conducts without getting damaged. Current in this region is called avalanche current. For a Zener diode, it is also called Zener current.

As soon as the voltage decreases, the diode retains its non-conducting condition and gets back to its normal properties. This specific property of being operational in the reverse bias and with avalanche current is given to the Zener diode by a rich doping of the semiconductor material.

Moreover, by controlling the amount of doping, the thickness of the depletion region in the PN junction and the breakdown voltage can be set to any value.

Zener current: Same as the avalanche current (the higher current after breakdown occurs in a semiconductor device) in a Zener diode.

Zener Diode Characteristics Curve

Figure 1 shows the characteristic curve of a Zener diode, which is more or less similar to that of an ordinary diode.

The range after the Zener knee (breakdown voltage) until the rated voltage of a Zener diode is reached is called the Zener region.

Zener diode characteristic curve.

Figure 1 Zener diode characteristic curve.

In this region, a small change in voltage leads to a large change in current. For instance, a change of 1 V in voltage can cause the current to increase by 10×.

Zener knee: a Sharp curve in the characteristic curve of a Zener diode where the breakdown voltage is reached and breakdown occurs.

Zener region: Region in the characteristic curve of a Zener diode where the breakdown has occurred because of the reverse voltage surpassing a certain value.

A Zener diode works when reverse biased. Otherwise, it behaves as an ordinary diode.

As can be understood from the characteristic curve, in this region, when the reverse voltage is smaller in absolute value than the Zener breakdown voltage, the current is very small and confined to the so-called leakage current, which is negligible and can be ignored.

But for higher reverse voltages, there is an abrupt and large increase in current. In other words, whereas the voltage remains almost constant, the current has a considerable variation. This is the significant property of a Zener diode, which can be employed.

A Zener diode has a different symbol to differentiate it from other diodes. This symbol is shown in Figure 2. The physical shape of a Zener diode can be the same as that of a regular diode.

Symbol for a Zener diode.

Figure 2 Symbol for a Zener diode.

Zener Diode Applications

The main application of a Zener diode is in voltage regulation.

Voltage regulation implies keeping a voltage at a desired value irrespective of current and other factors that tend to change it. It is very important for many devices to protect them from overvoltage (and excessive current, as a result).

The specific property of a Zener diode is that in its operating range the voltage drop across it is constant (it has an internal self-regulatory characteristic). This could be understood from the characteristic curve in Figure 1, which can be expressed differently: large current change in a Zener diode causes only a small variation in voltage. That is, the voltage drop across it is almost constant. In this respect, if a Zener diode is in parallel with another component, or device, the voltage across that device is kept constant, because of the Zener diode.

Voltage regulation: Controlling electric voltage in a circuit or a device to remain within the desired range (small variation) under different load conditions.

Figure 3 depicts a load in parallel with a Zener diode, both in series with the 200 Ω resistor R. Notice the polarity of the Zener diode.

The role of the resistor R is to provide the leverage for current adjustment. The Zener diode is a current governed device. If we remove R, the whole voltage is applied to the load.

Zener diodes come in different voltages, for example, 5.6, 7.5, 10, and 16 V, just to name a few. For each purpose, the right size diode (voltage and rated current) must be employed.

Zener diode in a circuit, regulating load voltage

Figure 3 Zener diode in a circuit, regulating load voltage.

Application Examples

The following examples show the application of a Zener diode and the concerns for the proper rating. Note the polarity of the circuits in the reverse biasing of the Zener diode. If a Zener diode is used in forward bias, it performs as a regular diode.

In all the examples, there is a resistor in series with the Zener diode and the load. The Zener diode is in parallel with the load. When necessary, we refer to this resistor as the series resistor.

Example 1

In Figure 4 the 100 Ω resistor is the load and the diode used is a 4.7 V Zener diode. In each of the three cases, find the current in the load (note polarity difference of the Zener diode in cases 2 and 3).


1. Following Ohm’s law, the current is


The voltage drop in the 50 Ω resistor is (50)(0.08) = 4 V.

2. The Zener diode is forward biased, and it behaves as a regular diode. The voltage drop across it is only 0.7 V.

Current in the load = 0.7 ÷ 100 = 0.007 A = 7 mA

Current in the 50 Ω resistor = (12 − 0.7) ÷ 50 = 0.226 A = 226 mA

Current in the diode = 226 − 7 = 219 mA

3. The Zener diode is reverse biased and performs as a voltage regulator

Current in the load = 4.7 ÷ 100 = 0.047 A = 47 mA

Total circuit current = Current in the 50 Ω resistor = (12 − 4.7) ÷ 50 = 0.146 A = 146 mA

Current in the diode = 146 − 47 = 99 mA

zener diode in forward and reverse bias mode

Figure 4 Example 1. (a) No Zener diode in the circuit. (b) The zener diode is forward biased. (c) The zener diode is reverse biased.

Example 2

If the value of the 50 Ω resistor in Example 1 is changed to 200 Ω, what is the change in the circuit current, in case 3 only?


The current in the 50 Ω resistor must always be greater than the load current because it is the sum of the current is the Zener diode and the load. If we calculate the currents in the load and in the 50 Ω resistor, we have

$\begin{align}  & Load\text{ }Current=\frac{4.7}{100}=0.047A \\ & Current\text{ }in\text{ }the\text{ }50\Omega \text{ }Resistor=\left( 12-4.7 \right)\div 200=0.036A \\\end{align}$

But, we observe that this current is smaller than the load current; thus, this is not a possible case. A value of 200 Ω resistor is not acceptable.

Example 2 shows that in selecting a series resistor for inclusion in the circuit when a voltage regulator is used, care must be taken not to have an improper size resistor.

 In such a case the circuit does not function as desired. The action of a Zener diode is that it absorbs the extra current of the circuit that would flow through the load. But, in the case of Example 3, there is no extra current.

For the circuit just discussed, the current is 12 ÷ 300 = 0.04 A and the Zener diode does not play any role.

When using a Zener diode, it is important to remember that:

1. The voltage across the load (in case the Zener diode is removed) must be more than the Zener diode value for voltage regulation to happen.

2. Current in the series resistor (the total circuit current) must be higher than the load current.

3. We cannot entirely eliminate the series resistor.

For regulating the voltage across a load we cannot entirely eliminate the series resistor.

Zener Diodes in Series and Parallel

In the same way that diodes could be put in series if a larger regulated voltage is required a number of (compatible) Zener diodes can be put together in series. For example, in Figure 5, three Zener diodes are put together to provide a larger regulated voltage for the load.

Also, it is possible to put Zener diodes in parallel to increase the current capacity. Figure 6 depicts an example.

Zener diodes in series.

Figure 5 Zener diodes in series.

Zener diodes in parallel.

Figure 6 Zener diodes in parallel.

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