Hooke’s law , Modulus of elasticity

Elastic Limit

Elastic limit is the highest deforming stress under which a material remains elastic

Hooke’s law

Hooke’s law states that the extension produced in the wire is directly proportional to the load applied within elastic limit.

i.e. within elastic limit, extension ∝ load applied.

Later on it was found that this law is applicable to all types of deformations such as compression, bending, twisting etc. and thus a modified form of Hooke’s law was given as stated below.

Within elastic limit, the stress developed is directly proportional to the strain produced in a body

i.e. stress ∝ strain or, stress = E × strain

where E is constant and known as modulus of elasticity.

Modulus of elasticity

According to Hooke’s law, within elastic limit,

stress ∝ strain

or, stress = E × strain

$ \displaystyle \frac{Stress}{Strain} = E = Constant $

Where E is known as the coefficient of elasticity or, the modulus of elasticity of a body.

It depends upon the nature of material of the body and the manner in which the body is deformed.

Thus modulus of elasticity is the ratio of the stress to the corresponding strain produced, which is a constant, within the elastic limit.

Types of moduli of elasticity

Corresponding to three types of strain, there are three elastic moduli, described below :

(a) Young’s Modulus of elasticity (Y)

It is the ratio of normal stress to the longitudinal strain within the elastic limit. Thus

$ \displaystyle Y = \frac{Normal\, Stress }{Longitudinal \, Strain} $

Consider a metal wire AB of length l, radius r and of uniform area of cross-section a. Let it be suspended from a rigid support at A, as shown in the figure below.

Let a normal force F be applied at its free end B and let its length increase by Δl (= BB’ )

$ \displaystyle Normal Stress = \frac{F}{A} = \frac{F}{\pi r^2} $

$ \displaystyle Longitudinal \, strain = \frac{\Delta l}{l} $

$ \displaystyle Y = \frac{F l}{A \Delta l} $

(b) Bulk Modulus of elasticity (k)

It is the ratio of normal stress to the volumetric strain, within the elastic limit. Thus

$ \displaystyle K = \frac{Normal\, Stress }{Volumetric \, Strain} $

Consider a spherical solid body of volume V and surface area a. In order to compress the body, let a pressure p be applied on the body and suppose that its volume decreases by ΔV as shown in figure.

Then, volumetric strain = – ΔV/V

Here negative sign shows that volume is decreasing when pressure is applied.

Normal stress = Fn/A = P

$ \displaystyle K = -\frac{P}{\frac{\Delta V}{V}} $

$ \displaystyle K = -\frac{P V}{\Delta V} $

(c) Modulus of rigidity (η)

It is the ratio of tangential stress to the shearing strain, within the elastic limit. It is also called shear modulus of rigidity.Thus

$ \displaystyle \eta = \frac{Tangential \, Stress }{Shearing \, Strain} $

$ \displaystyle \eta = \frac{F/A}{\theta} $

Shearing strain = ΔL/L

$ \displaystyle \eta = \frac{F L}{A \Delta L} $

Question : A steel wire of length 4m and diameter 5 mm is stretched by 5 kg-wt. find the increase in its length, if the Young’s modulus of steel of wire is 2.4 × 1012 dyne/cm2.

Poisson’s ratio (σ):

It is the ratio of lateral contraction strain to the longitudinal elongation strain .

$ \displaystyle \sigma = (\frac{-\Delta r}{r})/(\frac{\Delta L}{L})$

Where -Δr = decrease in radius of the wire , r= original radius

ΔL = increase in length of the wire , L = original length

Also Read :

∗ Elasticity , Stress , Strain & its types
∗ Relation b/w stress & strain for wire
∗ Elastic potential energy
∗ Elongation of Rod under its own weight

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