Home / Notes / Class 12 / Physics / Physics of solids
Classification of solids, crystalline and amorphous structure, mechanical properties such as stress, strain and Young's modulus, Hooke's law, elastic energy, band theory of conductors, insulators and semiconductors, and magnetic and superconducting materials.
Solids keep a fixed shape and volume because their atoms or molecules are held in position by strong forces and can only vibrate about fixed points. Solids can be crystalline, amorphous or polymeric.
Crystalline and amorphous solids:
A single crystal has one continuous lattice throughout, while a polycrystalline solid is made of many tiny crystals joined together. Most metals are polycrystalline. Crystals show cleavage, which means they split along certain planes.
Deforming force: when an external force acts on a solid, its shape or size can change. Stress is the force acting per unit area, stress = F/A, in N/m² (pascal). Strain is the fractional change in size, with no unit. Longitudinal strain = ΔL/L, volumetric strain = ΔV/V and shear strain is the angle of shear.
Hooke's law: within the elastic limit, stress is directly proportional to strain. The ratio is a constant called the modulus of elasticity. Young's modulus Y = stress/strain = (F/A)/(ΔL/L) = FL/(AΔL). It measures the stiffness of a material. Its unit is N/m² (Pa). Steel has a higher Young's modulus than rubber, so it is stiffer.
A stress against strain graph for a ductile metal wire is straight up to the proportional limit. Beyond the elastic limit the wire does not return to its original length and keeps a permanent set. At the yield point the strain rises quickly with little extra stress. Then the wire is stretched until the ultimate tensile stress and finally breaks at the fracture point. Materials that break soon after the elastic limit are brittle, such as glass. Those that stretch a lot are ductile, such as copper.
Strain energy: when a wire is stretched, work is stored as elastic potential energy. Energy stored = ½ × F × ΔL. The energy per unit volume is ½ × stress × strain.
Band theory: in a single atom, electrons occupy sharp energy levels. In a solid the levels of many atoms merge into bands. The valence band holds the outer electrons and the conduction band holds free electrons. The gap between them is the forbidden gap (energy gap) Eg.
Conductors, insulators and semiconductors by bands:
Magnetic materials: diamagnetic substances (such as bismuth and copper) are weakly repelled by a magnet. Paramagnetic substances (such as aluminium) are weakly attracted. Ferromagnetic substances (such as iron, nickel and cobalt) are strongly attracted and can become permanent magnets. They lose ferromagnetism above the Curie temperature. Hysteresis is the lag of magnetisation behind the magnetising field. Soft iron has a narrow loop, so it is used in transformer cores and electromagnets. Steel has a wide loop, so it is used for permanent magnets.
Superconductivity: some materials lose all electrical resistance when cooled below a certain critical temperature. A superconductor also expels magnetic fields from its inside (Meissner effect). Uses include powerful electromagnets in MRI machines and maglev trains.
Study tip: Learn the stress strain graph and label the proportional limit, elastic limit, yield point, ultimate stress and fracture point. For band theory questions, draw three small band diagrams and write the gap values. In numericals, convert to SI before substituting.
Say the meaning first, then open the card to check.
The regular three dimensional arrangement of atoms in a crystalline solid.
A solid with no regular long range order of atoms, such as glass.
The force acting per unit area of a body, in pascal.
The fractional change in length, volume or shape; it has no unit.
The ratio of tensile stress to tensile strain within the elastic limit.
The maximum stress up to which a body returns to its original size when released.
The energy gap between the valence and conduction bands.
The lag of magnetisation behind the magnetising field in a ferromagnet.
A material that has zero resistance below its critical temperature.
| Name | Formula | What it means |
|---|---|---|
| Stress | σ = F / A | Force per unit area. |
| Longitudinal strain | ε = ΔL / L | Extension per unit original length. |
| Young's modulus | Y = (F / A) / (ΔL / L) = FL / (AΔL) | For a wire stretched by force F. |
| Elastic energy | U = ½ F ΔL | Work stored in a stretched wire. |
| Energy per unit volume | u = ½ × stress × strain | Elastic energy density. |
These are the kind of questions asked for 2, 3 and 5 marks. Try each one before opening the answer.
A crystalline solid has a regular repeating arrangement of atoms, a sharp melting point and a definite shape. Some properties depend on direction. An amorphous solid has no long range order, softens over a range of temperature and has the same properties in all directions.
Within the elastic limit, the stress applied to a body is directly proportional to the strain produced in it.
Young's modulus is the ratio of longitudinal stress to longitudinal strain within the elastic limit. Its unit is newton per square metre, or pascal.
A ductile material, such as copper, stretches a great deal and shows a large plastic region before it breaks. A brittle material, such as glass, breaks soon after the elastic limit with very little plastic deformation.
In a conductor the valence band overlaps the conduction band, so many electrons are free to move and the resistance is low. In an insulator the forbidden gap is large, about 5 eV or more, so electrons cannot jump to the conduction band at ordinary temperature and the conductivity is nearly zero. In a semiconductor the gap is small, about 1.1 eV for silicon. At absolute zero the valence band is full and the conduction band is empty, so it acts as an insulator. At room temperature some electrons gain enough thermal energy to cross the gap, leaving holes behind, so it conducts a little. More electrons cross as the temperature rises.
Soft iron has a narrow hysteresis loop, so it is easy to magnetise and demagnetise and little energy is lost in each cycle. Steel has a wide loop, so it keeps its magnetism strongly once magnetised, which is needed for a permanent magnet.
Answer: ΔL = 2.0 × 10⁻³ m (2 mm)
Answer: Stress = 2.0 × 10⁸ Pa
Answer: U = 0.2 J
Answer: Strain = 5.0 × 10⁻⁴ (no unit)