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Question: A uniform pressure \[p\] exerted on all sides of a solid cube at temperature \[0^\circ \,{\text{C}}\...

A uniform pressure pp exerted on all sides of a solid cube at temperature 0C0^\circ \,{\text{C}}. In order to bring the volume of the cube to the original volume, the temperature of the cube must be increased by tCt^\circ \,{\text{C}}. If α\alpha is the linear coefficient of thermal expansion and KK is the bulk modulus of the material of the cube, then tt is equal to
A. 3PKα\dfrac{{3P}}{{K\alpha }}
B. P2αK\dfrac{P}{{2\alpha K}}
C. P3αK\dfrac{P}{{3\alpha K}}
D. PαK\dfrac{P}{{\alpha K}}

Explanation

Solution

Use the formulae for the bulk strain, linear expansion of the material and the relation between the linear strain and bulk strain. These equations give the relation between the change in volume, change in length of the edge, original length, original volume, bulk modulus, thermal expansion coefficient and pressure on the cube.

Formula used:
The bulk modulus KK of a material is given by
K=PΔVVK = \dfrac{P}{{\dfrac{{\Delta V}}{V}}} …… (1)
Here, PP is the bulk stress of the material, ΔV\Delta V is the change in volume of the material and VV is the original volume of the material.
The change in the length Δl\Delta l of a material due to thermal expansion is
Δl=l0αΔT\Delta l = {l_0}\alpha \Delta T …… (2)
Here, is the original length of the material, is the linear thermal coefficient and is the change in the temperature.
The relation between the bulk strain and linear strain is
Bulk strain=3(Linear strain){\text{Bulk strain}} = 3\left( {{\text{Linear strain}}} \right) …… (3)

Complete step by step answer:
A uniform pressure pp exerted on all sides of a solid cube at temperature 0C0^\circ \,{\text{C}}. In order to bring the volume of the cube to the original volume, the temperature of the cube is increased by tCt^\circ \,{\text{C}}.
Rewrite equation (1) for the linear thermal expansion of the cube.
Δl=l0αt\Delta l = {l_0}\alpha t
Here, l0{l_0} is the original length of the edge of the cube, Δl\Delta l is the change in length of edge of the cube and tt is the change in temperature of the cube.
Rearrange the above equation for Δll0\dfrac{{\Delta l}}{{{l_0}}}.
Δll0=αt\dfrac{{\Delta l}}{{{l_0}}} = \alpha t
Rewrite equation (1) for the bulk modulus KK of the material of the cube.
K=PΔVV0K = \dfrac{P}{{\dfrac{{\Delta V}}{{{V_0}}}}}
Here, V0{V_0} is the original volume of the cube.
Rearrange the above equation for ΔVV0\dfrac{{\Delta V}}{{{V_0}}}.
ΔVV0=PK\dfrac{{\Delta V}}{{{V_0}}} = \dfrac{P}{K}
The linear strain of the cube is the ratio of the change in length Δl\Delta l of the edge of the cube to the original length l0{l_0} of the edge of the cube.
Linear strain=Δll0{\text{Linear strain}} = \dfrac{{\Delta l}}{{{l_0}}}
The bulk strain of the cube is the ratio of the change in volume ΔV\Delta V of the cube to the original volume V0{V_0} of the cube.
Bulk strain=ΔVV0{\text{Bulk strain}} = \dfrac{{\Delta V}}{{{V_0}}}
Substitute Δll0\dfrac{{\Delta l}}{{{l_0}}} for Linear strain{\text{Linear strain}} and ΔVV0\dfrac{{\Delta V}}{{{V_0}}} for Bulk strain{\text{Bulk strain}} in equation (3).
ΔVV0=3Δll0\dfrac{{\Delta V}}{{{V_0}}} = 3\dfrac{{\Delta l}}{{{l_0}}}
Substitute αt\alpha t for Δll0\dfrac{{\Delta l}}{{{l_0}}} in the above equation.
ΔVV0=3αt\dfrac{{\Delta V}}{{{V_0}}} = 3\alpha t
Substitute PK\dfrac{P}{K} for ΔVV0\dfrac{{\Delta V}}{{{V_0}}} in the above equation.
PK=3αt\dfrac{P}{K} = 3\alpha t
Rearrange the above equation for the change in temperature tt.
t=P3αKt = \dfrac{P}{{3\alpha K}}
Therefore, the change in temperature must be P3αK\dfrac{P}{{3\alpha K}}.
Hence, the correct option is C.

So, the correct answer is “Option C”.

Note:
Since the volume of a cube is three times the length of the edge of the cube.
The volume strain for the cube is three times the linear strain of the cube.