Q.What is electrical conductivity?
Concept understanding — Electrical Properties of Solids
Electrical Properties of Solids: From Atoms to Circuits
Imagine a single atom. Its electrons live in well-defined shells, each at a specific energy. Now bring two atoms close together. Their electron clouds overlap, and the sharp energy levels split into two slightly different energies — one for the bonding combination, one for the antibonding. Bring a billion atoms together in a solid, and those two levels split into a billion closely spaced levels, forming a continuous band of allowed energies.
That is the core idea: in a solid, discrete atomic energy levels broaden into energy bands, separated by gaps where no electron can exist. The highest occupied band at absolute zero is the valence band; the next empty band above it is the conduction band. The gap between them is the band gap (Eg).
The electrical conductivity of a solid is determined entirely by how easily electrons can move from the valence band into the conduction band. That ease is controlled by the size of the band gap.
Conductors, Insulators, and Semiconductors
Conductors (metals) have either no band gap — the valence and conduction bands overlap — or a partially filled conduction band. Electrons have a vast number of empty states right next to them in energy, so a tiny electric field sets them drifting. That is why copper and aluminium conduct so well.
Insulators have a large band gap, typically >3 eV. At room temperature, almost no electrons have enough thermal energy to jump the gap. The valence band is full, the conduction band is empty, and no current flows. Diamond (Eg≈5.5 eV) is a classic example.
Semiconductors sit in between. Their band gap is small — about 1.1 eV for silicon, 0.67 eV for germanium. At absolute zero they behave like insulators, but at room temperature enough electrons are thermally excited across the gap to give a small but useful conductivity. This conductivity rises sharply with temperature, opposite to metals.
σ=neμe+peμh
Conductivity depends on the number (n, p) and mobility (μe, μh) of electrons and holes.
The Hole: A Missing Electron
When an electron jumps from the valence band to the conduction band, it leaves behind a vacancy — a missing negative charge. That vacancy behaves as a positive charge carrier called a hole. Under an electric field, a neighbouring electron can move into the hole, leaving a new hole behind. The hole effectively moves in the opposite direction to the electrons, carrying positive charge.
In a pure (intrinsic) semiconductor, every electron excited leaves one hole behind, so n=p. This is called intrinsic conduction.
Doping: Engineering Conductivity
Pure silicon is not very useful. Its conductivity is too low and too sensitive to temperature. The real power comes from doping — deliberately adding impurity atoms to control the number of charge carriers.
n-type doping: Add a group-15 element (phosphorus, arsenic) to silicon. Silicon is group 14, so the impurity has five valence electrons. Four form bonds with neighbouring silicon atoms; the fifth is loosely bound and easily donated to the conduction band. The impurity is called a donor. Now n>p — electrons are the majority carriers.
p-type doping: Add a group-13 element (boron, aluminium) to silicon. It has only three valence electrons. It forms three bonds, leaving one bond incomplete — a hole. The impurity is an acceptor because it readily accepts an electron from the valence band, creating a mobile hole. Now p>n — holes are the majority carriers.
The doped semiconductor as a whole remains electrically neutral. Each impurity atom has the same nuclear charge as its neighbours, so the extra electron or hole is balanced by the fixed ionic core of the impurity.
Why This Matters
A pure silicon crystal has roughly 1010 carriers per cm³ at room temperature. Doping with one phosphorus atom per million silicon atoms raises the electron concentration to about 1016 per cm³ — a million-fold increase. That is the difference between a useless rock and the heart of every modern electronic device.
The p-n junction — a single crystal with p-type on one side and n-type on the other — is the foundation of diodes, transistors, solar cells, and LEDs. The band gap determines the colour of an LED, the efficiency of a solar cell, and the switching speed of a transistor.
To remember the doping types: n-type has negative carriers (electrons) in excess; p-type has positive carriers (holes) in excess. The donor atom gives an electron; the acceptor atom takes one.
Electrical properties of solids, including band theory and doping, are part of the NCERT/CBSE Class 12 Chemistry solid state chapter, and "electrical properties of solids: conductors insulators semiconductors" is a frequently searched revision topic. The n-type and p-type doping distinction it covers is also a common important-question topic in JEE Main and NEET.
Conductivity measures how readily a material lets electric charge flow through it.
Electrical conductivity is the ability of a material to conduct electricity -- to allow the flow of electric current through it by the movement of charged particles (electrons, or ions in electrolytes). It is the reciprocal of electrical resistivity.
Electrical conductivity is a material's ability to carry electric current; the higher the conductivity, the more easily charge flows.
Step 1. When an electric potential is applied across a material, mobile charged particles inside it -- electrons in metals, ions in molten or dissolved electrolytes -- can migrate, and that migration of charge constitutes an electric current.
Step 2. Electrical conductivity is the property that measures how readily this happens: it is the reciprocal of resistivity, and solids span an enormous range of it -- from about 10−20 Ohm−1m−1 for the best insulators to about 107 Ohm−1m−1 for good metallic conductors.
The ability of a substance to conduct electric current -- i.e. to permit the flow of charge through it via mobile electrons or ions; the reciprocal of resistivity.
- CBSE 2026Set ANNUAL1 markMCQQ.Insulator substance among the following is(a) Graphite(b) Teflon(c) Sodium(d) Silver
›Reveal solutionSolution
Electrical conduction needs mobile charge carriers (free electrons or ions); Teflon (PTFE) is a covalent polymeric solid with tightly bound electrons, so it is an insulator, unlike the metals/conductors in the other options.
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Graphite: layered covalent solid but has delocalised pi-electrons between layers -> good conductor.
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Teflon: saturated C-F covalent polymer, all electrons localised in bonds -> insulator.
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Sodium and Silver: metals, with a 'sea' of delocalised electrons -> excellent conductors.
✓Final answer(b) Teflon.
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- CBSE 2025Set X11 markMCQQ.Select non-semiconductor from the following,(a) silicon(b) carbon-black(c) gallium arsenide(d) doped silicon
›Reveal solutionSolution
Silicon, gallium arsenide and doped silicon are all semiconductors; carbon-black is not, so it is the non-semiconductor.
Checking each:
- (a) Silicon — a classic intrinsic semiconductor (Group 14).
- (b) Carbon-black — an amorphous form of carbon; it behaves as an electrical conductor, not a semiconductor.
- (c) Gallium arsenide (GaAs) — an important 13–15 (III–V) compound semiconductor.
- (d) Doped silicon — an extrinsic (n- or p-type) semiconductor.
Hence the non-semiconductor is carbon-black.
✓Final answer(b) carbon-black
- CBSE 2018Set ANNUAL1 markQ.Fill in the blank: Conductivity without resistance is called ___.
›Reveal solutionSolution
When certain materials are cooled below a critical temperature, their electrical resistance drops abruptly to zero — this phenomenon is superconductivity.
Certain metals, alloys and compounds, when cooled below a characteristic critical temperature (Tc), lose all electrical resistance and can carry an electric current indefinitely without any energy loss. This state of zero resistance is called superconductivity, and the material in that state is a superconductor.
✓Final answerSuperconductivity.
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