The number of electrons available for electrical conduction is related to the arrangement of electron states or levels with respect to energy, and then the manner in which these states are occupied by electrons
Partially filled outermost band (typical of some metals like Cu), with the Fermi energy marking the highest filled state
Overlapping filled and empty bands (found in metals like magnesium), with the Fermi energy set where N states are filled, accommodating two electrons per state
Valence band - One band that is completely filled with electrons
Conduction band - Similar to three but empty. Energy band gap lies between the valence and conduction bands.
Very little energy is required to promote electrons into the low-lying empty states above the Fermi energy in metals (the energy of the electricfield is enough to excite them)
For insulators and semiconductors, emptystates adjacent to the top of the filled valence band are not available. To become free, electrons must be promoted across the energy band gap and into empty states at the bottom of the conductionband
For electrically insulating materials, electrons are tightlybound to or shared with the individual atoms, and are highly localized and not free to wander throughout the crystal
For semiconductors, valenceelectrons are not as strongly bound to the atoms and are more easily removed by thermalexcitation than they are for insulators
Result from the scattering of electrons by imperfections in the crystal lattice, including impurity atoms, vacancies, interstitial atoms, dislocations, and even the thermal vibrations of the atoms themselves
Scattering event = lose kinetic energy/change direction of motion
Scattering event = resistance to the passage of an electric current (or raises resistivity)