A Zener diode is a special type of semiconductor device widely used in modern electronic circuits for voltage regulation and protection. From smartphone chargers to power supply units and automotive electronics, Zener diodes ensure a stable and constant output voltage even when input voltage fluctuates. Designed to operate safely in the reverse breakdown region, this p–n junction diode maintains voltage stability without damage. Understanding the working of a Zener diode, its V–I characteristics, Zener breakdown, and avalanche breakdown is essential for students of Class 11 and 12 Physics. In this article, we will explore the definition, symbol, working principle, characteristics, applications, and solved examples of the Zener diode in a clear and simple manner.
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It is invented by C. Zener. A Zener diode is a p-n junction semiconductor device designed to operate in the reverse breakdown region. It is a highly doped p-n junction which is not damaged by high reverse current. It can operate continuously, without being damaged in the region of reverse background voltage. It forms a very thin depletion region and an extremely high electric field across the junction even for a small reverse bias voltage (~5 V).
In the forward bias, the Zener diode acts as an ordinary diode.
The symbol of the Zener diode is shown in the below figure.

Zener Breakdown
When a reverse bias is increased the electric field at the junction also increases. At some stage, the electric field becomes so high that it breaks the covalent bonds creating electron-hole pairs. Thus a large number of carriers are generated. This causes a large current to flow. This mechanism is known as Zener breakdown.
Avalanche breakdown
At high reverse voltage, due to the high electric field, the minority charge carriers, while crossing the junction acquire very high velocities. These by collision break down the covalent bonds, generating more carriers. A chain reaction is established, giving rise to a high current.
This mechanism is known as Avalanche breakdown.
The VI characteristics of a Zener diode are shown in the figure below.

When forward-biased voltage is applied to the Zener diode, it works like a normal diode.
When reverse-biased voltage is applied to a Zener diode, it allows only a small amount of leakage current until the voltage is less than the Zener voltage (Vz). As the reverse bias voltage (V) reaches the breakdown voltage of the Zener diode (Vz), there is a large change in current. Also, note that for a negligible change in the reverse bias voltage, a large change in current is produced.
A Zener diode is a specially designed p–n junction diode that operates in the reverse bias region to provide a constant voltage.
A Zener diode is connected in reverse bias (positive terminal to n-side and negative to p-side).
When the reverse voltage is small, only a tiny leakage current flows.
As the reverse voltage increases and reaches a specific value called the Zener breakdown voltage (Vz), the diode starts conducting heavily.
After breakdown, the voltage across the diode remains almost constant even if the current changes.
This property makes the Zener diode useful as a voltage regulator.
Example 1: Identify the semiconductor devices whose characteristics are given below, in the order (a), (b), (c), (d) :


1) Simple diode, Zener diode, Solar cell, Light-dependent resistance
2) Zener diode, Simple diode, Light-dependent resistance, Solar cell
3) Solar cell, Light-dependent resistance, Zener diode, Simple diode
4) Zener diode, Solar cell, Simple diode, Light-dependent resistance
Solution:
Zener diode
It can operate continuously without being damaged in the region of reverse-bias
wherein
1) It acts as a voltage regulator
2) In forward biasing it acts as an ordinary diode.
Solar cells
It is based on the photovoltaic effect. It converts solar energy into electrical energy.
wherein
One of the semiconductor regions is made so thin that the light incident on it reaches the PN junction and gets absorbed.
(a) represents a simple diode.
(b) represents zener diode
(c) solar cell
(d) light-dependent resistance.
Hence, the answer is option (1).
Example 2: In the given circuit, the current (in mA) through the zener diode is :
1) 3.3
2) 6.7
3) 2.5
4) 5.5
Solution:
Given:
Potential difference across $R_2=10 \mathrm{~V}$
Potential difference across $R_1=5 \mathrm{~V}$
$
\begin{aligned}
& R_1=500 \Omega \\
& R_2=1500 \Omega
\end{aligned}
$
First, calculate the current through $R_1$ :
$
\begin{gathered}
I_{R 1}=\frac{V}{R}=\frac{5}{500} \\
I_{R 1}=0.01 A=\frac{1}{100} A
\end{gathered}
$
Next, calculate the current through $R_2$ :
$
\begin{aligned}
I_{R 2} & =\frac{10}{1500} \\
I_{R 2} & =\frac{1}{150} A
\end{aligned}
$
Now, the current through the Zener diode is the difference between the two currents:
$
\begin{aligned}
I_Z & =I_{R 1}-I_{R 2} \\
I_Z & =\frac{1}{100}-\frac{1}{150}
\end{aligned}
$
Taking LCM (300):
$
\begin{gathered}
I_Z=\frac{3-2}{300} \\
I_Z=\frac{1}{300} A \\
I_Z=0.0033 A=3.3 \mathrm{~mA}
\end{gathered}
$
Example 3: The value of the resistor, RS′ needed in the dc voltage regulator circuit shown here, equals :

1. $\frac{V_i-V_L}{n I_L}$
2. $\frac{V_i+V_L}{n I_L}$
3. $\frac{V_i-V_L}{(n+1) I_L}$
4. $\frac{V_i+V_L}{(n+1) I_L}$
Solution
Let
$V_i=$ Input voltage
$V_L=$ Load voltage
$I_L=$ Load current
$n=$ Number of loads
Each load draws current $I_L$. Therefore, total current flowing through the series resistor $R_S$ is:
$
I_{\text {total }}=(n+1) I_L
$
Voltage drop across the series resistor:
$
V_{R S}=V_i-V_L
$
Using Ohm's Law:
$
\begin{gathered}
R_S=\frac{V_{R S}}{I_{\text {total }}} \\
R_S=\frac{V_i-V_L}{(n+1) I_L}
\end{gathered}
$
Hence, the answer is option (3).
Example 4: In the given circuit the current (in mA) through the Zener Diode is close to:
1) 5
2) 6
3) 4
4) 0
Solution:
Zener diode operates continuously without being damaged in the region of reverse-biased
wherein
1) It acts as the voltage regulator.
2) In forward biasing it acts as an ordinary diode.
Since the voltage across the zener must be less than 10 V, therefore it will not work in the breakdown region its resistance is infinite and the current through it is zero.
Hence, the answer is option (4).
A Zener diode is a special kind of diode which allows current to pass in the reverse direction only if a particular voltage known as the Zener breakdown voltage is reached. While typical diodes prevent reverse current flow, a Zener diode is meant to function under the reverse bias condition. Hence it becomes useful in voltage regulation in electronic circuits where the output voltage should be kept constant despite changes in input voltage level or power consumption.
Frequently Asked Questions (FAQs)
A Zener diode is a semiconductor device that permits current to flow both forward and backward.
Zener diodes are commonly employed as constant-voltage devices because of this feature. When the voltage is above the required Zener voltage, a Zener diode allows Zener current, Iz, to flow. As a result, a Zener diode can be used to measure voltage by sensing Zener current with another device.
When the Zener diode is reverse biased and reaches Zener voltage, it begins to allow a considerable amount of electric current. A minor increase in reverse voltage will dramatically increase the electric current at this moment. Zener breakdown happens as a result of the abrupt increase in electric current.
The flow of current is the major distinction between a Zener diode and a regular diode. A typical diode can only flow in one direction, whereas a Zener diode can flow in both directions.
A shunt voltage regulator is a Zener diode. To reverse bias the load, a Zener diode is connected parallel to it, and after the Zener diode exceeds knee voltage, the voltage across the load becomes constant.