To learn about forward and reverse biasing of a p-n junction diode, let’s break down the concept step by step:

1. Unbiased p-n Junction

• When a p-n junction is formed, electrons from the n-side combine with holes from the p-side, creating a depletion region where no free charge carriers exist.

• This forms a barrier potential, stopping current flow unless an external voltage is applied.

2. Forward Biasing

Definition: When the p-side (positive) is connected to the positive terminal of a DC power supply and the n-side (negative) is connected to the negative terminal of the supply.

Mechanism:

  1. The negative terminal pushes electrons from the n-side towards the junction, and the positive terminal pushes holes from the p-side towards the junction.

  2. This reduces the width of the depletion region.

  3. As the barrier potential decreases, more charge carriers (electrons and holes) cross the junction, allowing a large current to flow.

  4. When the external voltage exceeds the barrier potential, the depletion region collapses, further enabling current flow.

3. Reverse Biasing

Definition: When the p-side is connected to the negative terminal of a DC power supply and the n-side is connected to the positive terminal.

Mechanism:

  1. Electrons in the n-region are attracted to the positive terminal, and holes in the p-region move towards the negative terminal.

  2. This causes an increase in the width of the depletion region, increasing the barrier potential.

  3. As a result, current flow through the junction is blocked except for a tiny leakage current due to minority carriers.

  4. No steady current flow is observed, as there is no continuous movement of charge carriers across the junction.