To find the forward and reverse bias characteristics of a given Zener diode.
S.No. | Name | Range | Quantity |
1 | R.P.S | (0-30)V | 1s |
2 | Ammeter | (0-30)mA | 2 |
3 | Voltmeter | (0-10)V (0-1)V | 1 1 |
S.No. | Name | Range | Quantity |
1 | Zener Diode | FZ5.1 | 1 |
2 | Resistor | 1KΩ | 1 |
3 | Bread Board | - | 1 |
4 | Wires | Required |
A properly doped crystal diode, which has a sharp breakdown voltage, is known as Zener diode.
On forward biasing, initially no current flows due to barrier potential. As the applied potential increases, it exceeds the barrier potential at one value and the charge carriers gain sufficient energy to cross the potential barrier and enter the other region. The holes, which are majority carriers in p-region, become minority carriers on entering the N- regions and electrons, which are the majority carriers in the N-regions become minority carriers on entering the P-region. This injection of minority carriers results current, opposite to the direction of electron movement.
When the reverse bias is applied, due to majority carriers small amount of current (i.e.,) reverse saturation current flows across the junction. As the reverse bias is increased to breakdown voltage, sudden rise in current takes place due to Zener effect.
Normally, PN junction of Zener Diode is heavily doped. Due to heavy doping the depletion layer will be narrow. When the reverse bias is increased the potential across the depletion layer is more. This exerts a force on the electrons in the outermost shell. Because of this force the electrons are pulled away from the parent nuclei and become free electrons. This ionization, which occurs due to electrostatic force of attraction, is known as Zener effect. It results in large number of free carriers, which in turn increases the reverse saturation current.
Forward Bias
Forward Bias
S.No. | Voltage (In Volts) | Current (In mA) |
1 | ||
2 | ||
3 | ||
4 | ||
5 |
Reverse Bias
S.No. | Voltage (In Volts) | Current (In mA) |
1 | ||
2 | ||
3 | ||
4 | ||
5 |
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