- Feedback & Compensation
- Oscillators
- Differentiator
- Semiconductor Devices - Integrator
- Practical Op-Amps
- Operational Amplifiers
- Semiconductor Devices - MOSFET
- JFET Biasing
- Field Effect Transistors
- Configuration of Transistors
- Transistor Biasing
- Construction of a Transistor
- Bipolar Transistors
- Varactor Diode
- Photovoltaic Cells
- Photo Diode
- Zener Diode
- Light Emitting Diode
- Diode Characteristics
- Leakage Current
- Junction Biasing
- Barrier Potential
- Depletion Zone
- Junction Diodes
- Doping in Semiconductors
- Types of Semiconductor
- Conductivity & Mobility
- Conduction in Solid Materials
- Atomic Combinations
- Introduction
- Semiconductor Devices - Home
Semiconductor Devices Resources
Selected Reading
- Who is Who
- Computer Glossary
- HR Interview Questions
- Effective Resume Writing
- Questions and Answers
- UPSC IAS Exams Notes
Conductivity & Mobipty
As discussed earper, there may be one or more free electrons per atom which moves all the way through the interior of the metal under the influence of an appped field.
The following figure shows charge distribution within a metal. It is known as the electron-gas description of a metal.
![Valence Free Electron](/semiconductor_devices/images/valence_free_electron.jpg)
The hashed region represents the nucleus with a positive charge. The blue dots represent the valence electrons in the outer shell of an atom. Basically, these electrons do not belong to any specific atom and as a result, they have lost their inspanidual identity and roam freely atom to atom.
When the electrons are in an uninterrupted motion, the direction of transportation is changed at each colpsion with the heavy ions. This is based on electron-gas theory of a metal. The average distance between colpsions is called the mean free path. The electrons, passing through a unit area, in the metal in the opposite direction in a given time, on a random basis, makes the average current zero.
Advertisements