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Question: If stress-strain relation for volumetric change is in the form \(\dfrac{{\Delta V}}{{{V_0}}} = KP\) ...

If stress-strain relation for volumetric change is in the form ΔVV0=KP\dfrac{{\Delta V}}{{{V_0}}} = KP where PP is applied uniform pressure, then KK stands for
A) shear modulus
B) compressibility
C) Young's modulus
D) bulk modulus

Explanation

Solution

When a uniform pressure is applied on a body, you can see a deformation of the body. The deformation in terms of volume causes a volume strain or bulk strain on the body. This bulk strain is related to the pressure by an elastic modulus.

Formulae Used:
If a uniform pressure PP causes a deformation of volume ΔV\Delta V where the total volume of the body was initially V0{V_0}, then we have the relation
Stress == Elastic Modulus ×\times Strain
P=B×ΔVV0P = B \times \dfrac{{\Delta V}}{{{V_0}}}
where, BB is the bulk modulus.
The compressibility KK is defined as the reciprocal of the bulk modulus BB
K=1BK = \dfrac{1}{B}

Complete step by step solution:
Given, The volumetric change is in the form ΔVV0=KP\dfrac{{\Delta V}}{{{V_0}}} = KP.

Step 1:
There is no mention of shear happening in the given problem.
Hence you can discard the elastic modulus of shearing that is the shear modulus from the consideration.
So, the option (A) is incorrect

Step 2:
The Young modulus is the elastic modulus which acts in the process of linear deformation.
But here, a volumetric change is happening hence the KK in the equation can not be Young’s modulus.
So, the option (C) is incorrect

Step 3:
From eq (1), you can see that a volumetric change is expressed, where the elastic modulus is the bulk modulus BB and the stress applied is the pressure PP.
Express eq (1) in terms of the given form of the volumetric change.
P=B×ΔVV0 ΔVV0=1BP  P = B \times \dfrac{{\Delta V}}{{{V_0}}} \\\ \Rightarrow \dfrac{{\Delta V}}{{{V_0}}} = \dfrac{1}{B}P \\\
So, evidently comparing this with the given form you can get
K=1BK = \dfrac{1}{B}
Hence this is not the bulk modulus but its reciprocal.
So, option (D) is also not correct.
By definition from eq (2), you can realize that the correct option is (B) which is the compressibility.

If stress-strain relation for volumetric change is in the form ΔVV0=KP\dfrac{{\Delta V}}{{{V_0}}} = KP where PP is applied uniform pressure, then KK stands for compressibility. Hence, option (B) is correction.

Note:
The bulk modulus is the ratio of the volumetric stress by volumetric strain. So, the bulk modulus will be proportional to the volumetric stress that is the uniform pressure rather than the volumetric strain. This problem also can be argued as the increase in volumetric strain means a change in the volume rather than the elastic property to keep it unchanged. So, the bulk modulus which represents the elastic property of the body that tries to resist the deforming stress can not be proportional to the strain. Hence compressibility would be the more correct option which represents the ability of the body to be compressed with certain stress applied.