This topic moves from the states of matter and the elastic behaviour of solids into the world of fluids — their density, pressure and buoyancy — and finishes with the surface and flow properties of liquids such as surface tension, capillarity and viscosity. Together they explain why ships float, why raindrops are round, and why honey pours slowly.
Matter is anything that has mass (weight) and occupies space, and it exists in three common states whose shape and volume behaviour distinguish them.
| State | Shape | Volume |
|---|---|---|
| Solid | Definite shape | Definite volume |
| Liquid | No definite shape | Definite volume |
| Gas | No definite shape | No definite volume |
Matter is anything that has mass and:
Which state of matter has no definite shape but a definite volume?
Matter exists in three states — solid, liquid and .
A gas has neither a definite shape nor a definite .
A solid is the state of matter that has both a definite shape and a definite volume, because its molecules are very closely packed and tightly bound.
A solid has:
Solids are generally described as:
In a solid, the molecules are very closely together.
Diffusion of particles in solids is very .
These two opposite properties describe whether a body returns to its original shape after a deforming force is removed.
Elasticity is the property by which a body:
Which are almost perfectly elastic bodies?
is the property by which a body does NOT regain its original configuration after the deforming force is removed.
In plastic deformation, after the force is removed the body does not regain its original .
When a deforming force acts on a body it produces both strain (the change it causes) and stress (the internal force that resists it).
| Type of strain | Definition | Formula |
|---|---|---|
| Linear (longitudinal) strain | change in length | ΔL / L |
| Volume strain | change in volume | ΔV / V |
| Shear strain (γ) | change in shape | Δθ (in radians) |
| Type of stress | Symbol | Direction of force |
|---|---|---|
| Normal stress | σ | acts perpendicular to the area |
| Tangential (shear) stress | τ | acts parallel to the area |
Strain is:
Stress is the internal restoring force acting per unit:
Strain has unit, as it is a pure ratio.
Normal stress acts to the area, while tangential stress acts parallel to it.
Within the elastic limit, stress and strain are directly proportional — this is Hooke's law, and the constant of proportionality is the modulus of elasticity.
| Modulus | Ratio | Concerns |
|---|---|---|
| Young's modulus (Y) | longitudinal stress / longitudinal strain | change in length |
| Bulk modulus (K) | normal stress / volume strain | change in volume |
| Modulus of rigidity (η) | shear stress / shear strain | change in shape |
Hooke's law states that within the elastic limit:
Young's modulus is the ratio of:
Bulk modulus (K) is the ratio of normal stress to strain.
The modulus concerning change in shape is the modulus of .
Every material can stretch only so far before it stops behaving elastically and eventually breaks.
The minimum stress required to break a wire is called:
If a wire is stretched beyond the elastic limit, the strain:
The maximum deforming force up to which a body retains its elasticity is called the of elasticity.
If deformation goes further into the plastic region, the wire breaks at the point.
How a material behaves between its elastic limit and its fracture point decides whether we call it ductile or brittle.
A ductile material shows:
Which of these is a brittle material?
In a material, the wire breaks soon after the elastic limit is crossed.
Copper and iron are examples of materials.
Plotting stress (σ) on the Y-axis against strain (ε) on the X-axis gives the tension-test curve, whose key points are asked directly in exams.
| Point | Meaning |
|---|---|
| OA | Proportional region (Hooke's law obeyed) |
| A | Proportional limit |
| B | Elastic limit (end of elastic region) |
| C | Ultimate stress (maximum stress) |
| D | Breaking stress / fracture point |
On the stress-strain curve, point B represents the:
On the stress-strain curve, the breaking (fracture) point is:
On the stress-strain curve, point C represents the stress (maximum stress).
The area under OAB represents the modulus of .
Repeated loading slowly tires out an elastic body and makes it less elastic over time.
Elastic fatigue is the property by which an elastic body:
Due to elastic fatigue, old bridges are eventually:
Elastic fatigue occurs under repeated deforming force.
A new bridge is more elastic, while an old bridge under repeated load becomes less elastic and .
A fluid is anything that can flow — both liquids and gases are fluids — and a key property of any fluid is its density.
Density is the ratio of:
The density of water is maximum at:
The SI unit of density is .
A hydrometer measures the density of a liquid and works on the law of .
The normal force (thrust) a fluid exerts per unit area is its pressure, and the air above us exerts atmospheric pressure on every surface.
Fluid pressure is given by the formula:
The SI unit of pressure is the:
For a liquid column of height h, the pressure is P = h ρ .
An aneroid is used to measure atmospheric pressure and the height of a place.
Pressure applied to an enclosed fluid is passed on equally in every direction — this is Pascal's law, the basis of all hydraulic machines.
| Machine | How it works |
|---|---|
| Hydraulic lift | small force F₁ on area A₁ → large force F₂ on area A₂; F₁/A₁ = F₂/A₂ |
| Hydraulic press | small F₁ on A₁ → large F₂ on A₂; F₁/A₁ = F₂/A₂ |
| Hydraulic brakes | master cylinder transmits pressure to wheel cylinder; F₁/A₁ = F₂/A₂ |
Pascal's law states that pressure applied to a confined fluid is transmitted:
Which machine works on Pascal's law?
For two pistons in a hydraulic machine, F₁/A₁ = F₂/.
Hydraulic brakes use a master cylinder to transmit to the wheel cylinder.
When a body is dipped in a fluid, the fluid pushes it up — this upward force is the buoyant force (upthrust), and the property is buoyancy.
The buoyant force on a submerged body equals the:
The point at which the buoyant force acts is called the:
The formula for buoyant force is Fᵦ = ρₗ × V_d × .
A body floats when its weight equals the weight of the fluid it .
Archimedes' principle gives the exact size of the upthrust and explains the apparent loss of weight in fluids.
According to Archimedes' principle, a body immersed in a liquid:
The apparent weight of a submerged body is:
The loss in weight of a submerged body equals the weight of the liquid .
In Archimedes' principle, the true weight W acts while upthrust acts upward.
The free surface of a liquid behaves like a stretched elastic skin that tries to shrink to the smallest possible area — this is surface tension.
Surface tension is the property by which a liquid tries to:
How does surface tension change with rising temperature?
The minimum surface area for a given amount of liquid is a sphere, which is why raindrops are .
Surface tension becomes zero at the temperature.
The rise or fall of liquid in a very fine tube is capillarity, decided by the tug-of-war between adhesion and cohesion.
Capillarity is the:
In water, the liquid rises in a capillary tube because:
In mercury, cohesion is greater than adhesion, so the liquid in the tube.
Blotting paper soaks ink because its pores act as tubes.
Capillarity and surface tension arise from two kinds of intermolecular attraction — between like molecules, and between unlike molecules.
Cohesive force is the attraction between molecules of:
The attraction between paper and gum is an example of:
force keeps molecules of the same substance together.
Adhesive force makes substances stick together.
A fluid resists motion between its own layers — this internal friction is the viscous force, and the property is viscosity.
| Fluid | On heating (temperature ↑) |
|---|---|
| Liquids | viscosity decreases |
| Gases | viscosity increases |
Viscosity is the property of a fluid by which it opposes:
With a rise in temperature, the viscosity of liquids:
There is no viscosity in , because their particles are fixed in position.
The viscosity of a liquid is due to the force between its molecules.
Stokes' law gives the viscous drag on a small sphere moving through a fluid in terms of viscosity, size and speed.
Stokes' law gives the viscous force as:
According to Stokes' law, the viscous force acts:
In Stokes' law, η is the coefficient of .
Honey flows slowly because it is more than water.
Take 5 questions at a time — tap an option to check. After each round, revise the notes above and take the retest for 5 fresh questions, until you've mastered the whole chapter.