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Introduction. • Conductors: mostly metals • Insulators: mostly nonmetal materials • Semiconductors: metalloids. Conductor. It is a meterial which has a large number of free electrons so,the current can easily flow through it
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Introduction • • Conductors: mostly metals • • Insulators: mostly nonmetal materials • • Semiconductors: metalloids
Conductor • It is a meterial which has a large number of free electrons so,the current can easily flow through it • All meterials with resistivity less than 10^(-3) ohm.meter behave as conductor……..
....cont • For example silver,copper,aluminium,carbon and almost all metals
Insulators • If the outer electrons of a meterial are very tightly bound to nucleus,it becomes very difficult to remove their orbits. Hence current no flow through such materials and they known as insulators……
…….cont. • All meterial with ressistivity above 10^(5) ohm.m • E.g mica,porcelain,glass, rubber,oil ,plastics,etc
Semi-conductors • Materials like germanium and silicon are neither good conductor nor insulators. They are called semi-conductor • Normally their outer electrons are bound to the nucleus but the electron can be made free by some means…..
……cont. • For example ,adding some impurity to germanium or silicon can make the outer elecrons free by increasing the temperature also the electrons can be made free. • Such material have resistivities between 10^(-3) and 10^(5) ohm.m
Semiconductors • • Metalloids: semiconducting elements • – low electrical conductivity at room temperature • – Electrical conductivity increases with temp. • • Gap between valence and conduction band is intermediate in size
• Semiconducting elements form the basis of solid state electronic devices. • Metalloids (such as silicon or germanium) are semiconducting elements whose electrical conductivity increases as temperature increases. • A striking property of these elements is that their conductivities increase markedly when they are doped with small quantities of other elements
Fig. 1. Calculated energy levels in the diamond structure as a function of assumed atomic spacing at T = 0o K. (From “Introduction to Semiconductor Physics”, Wiley, 1964)
Energy Band View of Semiconductors Fig. 1 shows the calculated allowed energy levels for electrons (vertical axis) versus distance betwee atoms (horizontal axis) for materials like silicon.
