Current Density in Metal and SemiconductorPublished on 24/2/2012 and last updated on Thursday 21st of June 2018 at 09:00:12 PM
Current Density in MetalSuppose, we have taken one conductor of cross-section 2.5 square mm. Now due to applied electric potential, the conductor carries a current of 3 A. Now the electric current carried by the conductor per square mm of its cross-section is 3/2.5 = 1.2 A. Here we considered that the current in the conductor is uniformly distributed throughout its cross-section. Now this 1.2 ampere is the current density of the conductor, and obviously, it is measured in ampere per square millimetre or more theoretically ampere per unit area. Hence, the current density can be defined as the electric current carried by conductor per unit cross-sectional area of the conducting medium.
We denote the current density with J and J equals I/A. Here, 'I' is the uniformly distributed current being carried by the conductor of the cross-sectional area A. If total N number of electrons passing through a cross-section of a conductor in time T, then Ne is the charge transferring through this cross-section in same time T. Where e is the charge of an electron in coulomb Now the amount of charge passing the cross-section per unit time is
Again if N number of electrons lie in the L length of the conductor, then the electron concentration is Now, from equation (1) we can write,
Since, N number of electrons lie in the length L and they all pass the cross-section in time T, the drift velocity of the electrons will be, Hence, equation (2) can also be rewritten as Now if applied electric field to the conductor is E, then drift velocity of the electrons increases proportionally, Where, μ is defined as the mobility of electrons
Current Density of SemiconductorsFor calculating current density of semiconductor, some factors to be considered.
- In semiconductor current flows not only due to electrons instead it is due to drift of electrons as well as holes.
- Movement of holes is always in opposite to that of corresponding electrons.
- Holes contribute current to their direction of movement whereas electrons contribute current opposite to their direction of movement. Hence both currents will be in same direction.
- Electrons involved in causing current in semiconductor, move through conduction band whereas holes causing current in semiconductor move through valance band. That is why mobility of electrons and holes are different in semiconductor.