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Question: Which of the following relations is true ? A. \(3Y = K(1 + \sigma )\) B. \(K = \dfrac{{9\eta Y}}...

Which of the following relations is true ?
A. 3Y=K(1+σ)3Y = K(1 + \sigma )
B. K=9ηYY+ηK = \dfrac{{9\eta Y}}{{Y + \eta }}
C. σ=(6K+η)Y\sigma = (6K + \eta )Y
D. σ=0.5Yηη\sigma = \dfrac{{0.5Y - \eta }}{\eta }

Explanation

Solution

Remember all the equations of elasticity and apply them accordingly.If you have the equations memorised, then this will be easy, else we must derive the equations accordingly. Types of modulus of elasticity are : Young’s Modulus YY, Bulk Modulus KK, Modulus of rigidity.

Complete step by step answer:
Value of Young’s modulus = longitudinal stresslongitudinal strain\dfrac{\text{longitudinal stress}}{\text{longitudinal strain}} .
Thus Y=1α(1)Y=\dfrac{1}{\alpha } - - - - (1) , where α\alpha is the longitudinal strain per unit stress.
We also know that Bulk modulus K=13(α2β)(2)K=\dfrac{1}{{3(\alpha - 2\beta )}}- - - - (2)
where β\beta is the lateral strain per unit stress.
We know that rigidity modulus η=12(α+β)(3)\eta = \dfrac{1}{{2(\alpha + \beta )}} - - - - (3) .
Also , Poisson’s ratio σ=βα(4)\sigma = \dfrac{\beta }{\alpha } - - - - (4) .

Now we can derive the relation for the above question,
η=12(α+β)\eta = \dfrac{1}{{2(\alpha + \beta )}}
η=1/α2(1+β/α)\Rightarrow \eta = \dfrac{{1/\alpha }}{{2(1 + \beta /\alpha )}}
But we know that β/α\beta /\alpha is Poisson's ratio. Hence,
η=Y2(1+σ)\eta = \dfrac{Y}{{2(1 + \sigma )}}
1+σ=0.5Yη\Rightarrow 1 + \sigma = \dfrac{{0.5Y}}{\eta }
Now moving that one to the right hand side , we get
σ=0.5Yηη\therefore \sigma = \dfrac{{0.5Y - \eta }}{\eta }

Hence, the correct answer is option D.

Note: Some important points which are to be remembered are as follows:-
-Coefficient of elasticity is always dependent on the material and its temperature and purity, and not on its stress and strain.
-The fundamental characteristic of elasticity of a material is its strain, not its stress.
-The values of the three coefficients of elasticity Y,K and ηY,K{\text{ }}and{\text{ }}\eta are always different and are related to each other.
-The potential energy due to elasticity equals 12×stress×strain\dfrac{1}{2} \times stress \times strain . -From this we can relate it to spring force and use it in required equations.