Introductory Electronics

Semiconductors

Semiconductors are materials whose electrical conductivity lies between that of conductors and insolators. Examples include Silicon (sand), Germanium, Arsenide, Carbon, Gallium, Selenium, and compounds like Lead Sulphide.

Properties of Semiconductors

  1. They act as insulators at low temperatures.
  2. Their resistance decreases as temperature increases.
  3. Their electrical conductivity can be enhanced by adding impurities, a process known as doping.

Types of Semiconductors

  1. Intrinsic
  2. Extrinsic

Intrinsic Semiconductor (Pure Semiconductor)

Structure

Intrinsic semiconductors have a crystalline structure, meaning their atoms are arranged in an orderly manner. They belong to Group IV of the periodic table and have four valence electrons.

Conductivity

At temperatures below room temperature, pure germanium is a poor electrical conductor.

At room temperature, the thermal energy of valence electrons may exceed the binding energy holding them to the nucleus. When this happens, an electron becomes free, leaving behind a vacancy called a hole. A neighboring electron can then move into this hole.

The conductivity of a semiconductor increases when:

Carriers of Electricity

In an intrinsic semiconductor, there are two types of charge carriers:

Application of an Electric Field

When an electric field is applied, charge carriers move in opposite directions:

Extrinsic Semiconductors

These semiconductors are produced through doping, which enhances their electrical conductivity.

Types of Extrinsic Semiconductors

  1. P-type Semiconductor: This type has more holes than free electrons. It is created by adding trivalent impurities such as indium or boron. Boron has three valency electrons, to form covalent bond with germanium, it can take electron from germanium, leaving a hole in germanium. This hole acts as a positive charge that can move through the crystal, The boron is called the acceptor. Conduction is due to movement of holes. The majority carrier of current are holes.
  2. N-type Semiconductor: This type contains more free electrons than holes. It is doped with pentavalent elements such as phosphorus or arsenic, which increases conductivity. Germanium has four valency electrons so, four of the valency electron of Arsenic forms a covalent bond with germanium. The fifth valency electron is very loosely bound, it does not participate in covalent bond. Conductivity is due to the movement of electron. The majority carrier of current are negative electrons while the minority carrier are holes.

Semiconductor Devices

Rectifier (p-n Junction Diode)

A p-n junction is created by depositing an n-type material onto a clean surface of a p-type material. It functions as a current rectifier, allowing current to flow in one direction (forward bias) while permitting little to no flow in the reverse bias. This makes it useful for converting alternating current (AC) into direct current (DC).

Forward Bias

When the positive terminal of a battery is connected to the p-region and the negative terminal to the n-region:

Reverse Bias

When the negative terminal of the battery is connected to the p-region and the positive terminal to the n-region:

The p-n junction diode exhibits low resistance in forward bias and high resistance in reverse bias, making it an effective rectifier for converting AC to DC.

Advantages of p-n Junction Diode over Thermionic Diode

  1. Smaller in size.
  2. Operates with a small potential difference in radio receivers.
  3. No warm-up time required to generate charge carriers.
  4. Cheaper to manufacture and more durable.

Half-Wave Rectifier

A half-wave rectifier uses a single diode. When an AC supply is applied:

Half Wave Rectifier Diagram Credit: Circuitstoday

Full-Wave Rectifier

A full-wave rectifier uses two diodes (D1 and D2):

To smooth out these fluctuations, a filter circuit is used. This circuit consists of a high inductance in series with a large capacitor, which minimizes voltage variations.

Full wave rectifier diagram Credit: testbook