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Question: An external pressure \(P\) is applied on a cube \({0^ \circ }c\) so that it is equally compressed fr...

An external pressure PP is applied on a cube 0c{0^ \circ }c so that it is equally compressed from all sides. KK is the bulk modulus of the material of the cube and α\alpha is its coefficient of linear expansion. Suppose we want to bring the cube to its original size by heating. The temperature should be raised by:
(a)\left( a \right) 3PKα3PK\alpha
(b)\left( b \right) P3αK\dfrac{P}{{3\alpha K}}
(c)\left( c \right) PαK\dfrac{P}{{\alpha K}}
(d)\left( d \right) 3αPK\dfrac{{3\alpha }}{{PK}}

Explanation

Solution

Hint First of all we will see the bulk modulus of materials and it is equal to the VV0=PK\dfrac{{\vartriangle V}}{{{V_0}}} = \dfrac{{\vartriangle P}}{K}. And by using the thermal expansion we will get the value of VV0\dfrac{{\vartriangle V}}{{{V_0}}}and the result we will get from there we will find out the T\vartriangle T and after that, we will change it in pressure and get the required result.
Formula used
The bulk modulus of the material,
K=P(V/V0)K = \dfrac{{\vartriangle P}}{{\left( { - \vartriangle V/{V_0}} \right)}}
Here,
KK, will be the bulk modulus
V\vartriangle V, will be the change in volume
P\vartriangle P, will be the change in pressure
V0{V_0}, will be the original volume

Complete Step By Step Solution
As we know the bulk modulus will be equal to
K=P(V/V0)K = \dfrac{{\vartriangle P}}{{\left( { - \vartriangle V/{V_0}} \right)}}
And it can also be written as
VV0=PK\Rightarrow \dfrac{{\vartriangle V}}{{{V_0}}} = \dfrac{{\vartriangle P}}{K}
Since there is a rise in temperature, so due to thermal expansion
V=V0(1+γt)V = {V_0}\left( {1 + \gamma \vartriangle t} \right)
And also it can be written as
V=V0+V0γt\Rightarrow V = {V_0} + {V_0}\gamma \vartriangle t
Now taking γt\gamma \vartriangle ton one side and rest at one side, we get
VV0V0=γt\Rightarrow \dfrac{{V - {V_0}}}{{{V_0}}} = \gamma \vartriangle t
And since [γ=3α]\left[ {\gamma = 3\alpha } \right]
Therefore,
VV0V0=γt=3αt\Rightarrow \dfrac{{V - {V_0}}}{{{V_0}}} = \gamma \vartriangle t = 3\alpha \vartriangle t
So, the upper equation can be written as,
VV0=3αt\Rightarrow \dfrac{{\vartriangle V}}{{{V_0}}} = 3\alpha \vartriangle t
And therefore it can be written as
PK=3αt\Rightarrow \dfrac{{\vartriangle P}}{K} = 3\alpha \vartriangle t
And from here, we get
t=P3αK\Rightarrow \vartriangle t = \dfrac{{\vartriangle P}}{{3\alpha K}}
Or we can write it as
Since P=P\vartriangle P = Pgiven in the question.
Therefore,
t=P3αK\Rightarrow \vartriangle t = \dfrac{P}{{3\alpha K}}

Hence, Option BB is the correct choice.

Note Bulk means wholesome, in a sense it refers to the whole of the material, i.e. Volume. Simply put, any modulus is the ratio between stresses to strain. Any Modulus is a measure of the resistance to deformation. Typically brought up as in understandability, the bulk modulus may be a measure of the flexibility of a substance to face up to changes in volume once below compression on all sides.