Definitions [20]
A body that regains its original shape and size after removal of the deforming force is called an elastic body, and the property is called elasticity.
Answer in one sentence.
Define elasticity.
If a body regains its original shape and size after removal of the deforming force, it is called an elastic body and the property is called elasticity.
A body that does not regain its original shape and size and retains its altered shape or size upon removal of the deforming force is called a plastic body, and the property is called plasticity.
A body that regains its original shape and size completely and instantaneously upon removal of the deforming force is said to be perfectly elastic.
Answer in one sentence.
Define strain.
The strain is defined as the ratio of change in dimensions of the body to its original dimensions.
Strain = `"change in dimensions"/"original dimensions"`
The internal restoring force per unit area of a body is called stress.
Strain is defined as the ratio of the change in dimensions of the body to its original dimensions.
The modulus of elasticity of a material is the ratio of stress to the corresponding strain. It is defined as the slope of the stress-strain curve in the elastic deforming region and depends on the nature of the material.
\[\frac {stress}{strain}\] = Constant
The constant is called the modulus of elasticity.
"Shear modulus or modulus of rigidity: It is defined as the ratio of shear stress to shear strain within elastic limits."
Define thrust.
The force which produces compression is called thrust. Its S.I unit is the newton.
Define the SI unit of pressure.
SI unit of pressure is the pascal (Pa) or Nm−2
One Pascal: When a force of one newton acts normally on an area of one square metre (1 m2) then the pressure acting on the surface acting on the surface is called one Pascal.
Define velocity gradient.
The rate of change of velocity (dv) with distance (dx) measured from a stationary layer is called velocity gradient.
∴ Velocity gradient = `(dv)/dx`
Define the coefficient of viscosity of a liquid.
The coefficient of viscosity of a liquid is defined as the viscous force acting tangentially per unit area of a liquid layer having a unit velocity gradient in a direction perpendicular to the direction of flow of the liquid.
Define terminal velocity.
The maximum constant velocity acquired by a body while falling freely through a viscous medium is called the terminal velocity VT.
The constant maximum velocity acquired by a body while falling through a viscous fluid is called terminal velocity.
Define the surface tension of a liquid.
Surface tension is defined as the force acting on a unit length of an imaginary line drawn on the free surface of the liquid, the direction of the force being perpendicular to the line so drawn and acting parallel to the surface.
Define surface tension.
Surface tension is defined as the force per unit length acting at right angles to an imaginary line drawn on the free surface of the liquid.
Define the angle of contact for a given pair of solid and liquid.
The angle between tangents drawn at the point of contact to the liquid surface and the solid surface inside the liquid is called the angle of contact for a pair of solid and liquid. It is denoted by θ.
Define angle of contact.
When a liquid is in contact with a solid, the angle between the tangent drawn to the free surface of the liquid and the surface of solid at the point of contact measured inside the liquid is called the angle of contact.
Formulae [4]
- \[|\vec{F}|\] is the magnitude of the internal restoring force (which is equal to the external applied deforming force).
- A is the area over which the force acts.
- SI unit of stress: N m-2 or pascal (Pa).
- Dimensions of stress: [L-1M1T-2].
The formula for modulus of rigidity is:
η = \[\frac{\text{Shear Stress}}{\text{Shear Strain}}=\frac{F/A}{\theta}=\frac{F}{A\cdot\theta}\]
Where:
- η = Modulus of rigidity (Pa or N/m²)
- F = Tangential force applied (N)
- A = Cross-sectional area on which force acts (m²)
- θ = Shear strain = Δl/l (in radians)
- Δl = Displacement of the upper surface relative to the lower surface (m)
- l = Original height of the block (m)
SI Unit: Pascal (Pa) or N/m²
Dimensional Formula: M¹L⁻¹T⁻²
v = \[\frac{2}{9}\cdot\frac{r^2(\rho-\sigma)g}{\eta}\]
where:
- v = terminal velocity
- r = radius of the body
- ρ = density of the body
- σ = density of the fluid
- g = acceleration due to gravity
- η = coefficient of viscosity of the fluid
Theorems and Laws [2]
Statement:
"The increase in pressure at one point of the enclosed liquid in equilibrium or at rest is transmitted equally to all other points of the liquid and also to the walls of the container, provided the effect of gravity is neglected."
OR
A solid sphere moves at a terminal velocity of 20 m s−1 in air at a place where g = 9.8 m s−2. The sphere is taken in a gravity-free hall having air at the same pressure and pushed down at a speed of 20 m s−1.
(a) Its initial acceleration will be 9.8 m s−2 downward.
(b) It initial acceleration will be 9.8 m s−2 upward.
(c) The magnitude of acceleration will decrease as the time passes.
(d) It will eventually stop
(b) There is no gravitational force acting downwards. However, when the starting velocity is 20 m/s, the viscous force, which is directly proportional to velocity, becomes maximum and tends to accelerate the ball upwards.
\[\text{ When the ball falls under gravity, }\]
\[\text{ neglecting the density of air: } \]
\[\text{ Mass of the sphere = m }\]
\[\text{ Radius = r }\]
\[\text{ Viscous drag coeff . }= \eta\]
\[\text{Terminal velocity is given by}: \]
\[\text{ mg }= 6\pi\eta r v_T \]
\[ \Rightarrow \frac{6\pi\eta r v_T}{m} = g . . . (1)\]
\[\text{ Now, at terminal velocity, the acceleration of the ball due to the viscous force is given by: } \]
\[a = \frac{6\pi\eta r v_T}{m}\]
\[\text{ Comparing equations (1) and (2), we find that : } \]
\[ \text{ a = g }\]
Thus, we see that the initial acceleration of the ball will be 9.8 ms - 2 .
(c) The velocity of the ball will decrease with time because of the upward viscous drag. As the force of viscosity is directly proportional to the velocity of the ball, the acceleration due to the viscous force will also decrease.
(d) When all the kinetic energy of the ball is radiated as heat due to the viscous force, the ball comes to rest.
Key Points
- Hydraulic Press — Two cylinders (C & D) filled with liquid; small force applied on piston P₁ (smaller area A₁) is converted into a very large upward force on piston P₂ (larger area A₂), since A₂ > A₁.
- Hydraulic Lift — Works on Pascal's Law to lift or support heavy objects such as cars and trucks using liquid pressure.
- Hydraulic Brakes — Small force on the brake pedal is instantly transmitted equally through brake fluid to all cylinders, producing a large thrust on the wheels to stop the vehicle.
- A highly soluble impurity increases surface tension, while a partially soluble impurity (e.g., detergent) decreases it; a waterproofing agent increases it.
- Surface tension decreases with increase in temperature, given by T = T0(1 − αθ), where T0 is surface tension at 0°C and α is the temperature coefficient.
- When a soap bubble is charged (positively or negatively), force acts outward on the surface, increasing its radius — thus electrification always decreases surface tension.
Concepts [16]
- Elastic Behavior of Solids
- Stress and Strain
- Hooke’s Law
- Elastic Modulus>Modulus of Rigidity
- Elastic Energy
- Thrust and Pressure
- Pascal’s Law
- Effect of Gravity on Fluid Pressure
- Viscous Force or Viscosity
- Terminal Velocity
- Streamline and Turbulent Flow
- Critical Velocity
- Applications of Bernoulli’s Equation
- Surface Tension
- Excess of Pressure Across a Curved Surface
- General Characteristics of Fluid Flow
