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Question: How do I calculate the new pressure of liquid water using its isothermal compressibility \(\kappa \)...

How do I calculate the new pressure of liquid water using its isothermal compressibility κ\kappa and expansion coefficient α\alpha

Explanation

Solution

In this question, we need to find the new pressure of liquid water using its isothermal compressibility κ\kappa and expansion coefficient α\alpha . Isothermal compressibility κ\kappa helps to determine the compressibility properties of the reservoir. The Expansion coefficient α\alpha is also known as thermal expansion, The volume of a material increases with an increase in temperature.

Complete answer:
Isothermal compressibility κ\kappa measures the fractional change in volume with a change in pressure.
κ=(PartialVP)TV\kappa =\,\dfrac{{{(\dfrac{Partial\,V}{\partial P})}_{T}}}{V}= 1V(VP)T-\dfrac{1}{V}{{(\dfrac{\partial V}{\partial P})}_{T}} In this (VP)T\dfrac{\partial V}{\partial P}{{)}_{T}} is considered as the partial derivative of volume w.r.t Pressure and the temperature is constant.
κPT=1VVT\kappa \partial {{P}_{T}}=\,-\dfrac{1}{V}\partial {{V}_{T}}
Expansion coefficient α\alpha is the change in the volume of the substance as soon as there is an increment in the temperature.
α=(PartialVT)PV\alpha \,=\,\dfrac{{{(\dfrac{Partial\,V}{\partial T})}_{P}}}{V}= 1V(VT)P\dfrac{1}{V}{{(\dfrac{\partial V}{\partial T})}_{P}} In this (VT)P{{(\dfrac{\partial V}{\partial T})}_{P}}is considered as the partial derivative of volume w.r.t Temperature and pressure is constant.
αTP=1VVP\alpha \,\partial {{T}_{P}}=\,\dfrac{1}{V}\partial {{V}_{P}}
Derivative of the differential equation is
dV=(VT)PdT+(VT)TdPdV=\,{{(\dfrac{\partial V}{\partial T})}_{P}}dT\,+\,{{(\dfrac{\partial V}{\partial T})}_{T}}dP
Dividing the equation by partial differential temperature where the volume is constant
(PT)V=(VT)P(VP)T{{(\dfrac{\partial P}{\partial T})}_{V}}\,=\,\dfrac{-{{(\dfrac{\partial V}{\partial T})}_{P}}}{{{(\dfrac{\partial V}{\partial P})}_{T}}}
Substituting this withκ\kappa and α\alpha
(PT)V=ακ{{(\dfrac{\partial P}{\partial T})}_{V}}=\,\dfrac{\alpha }{\kappa }
By Partial differentiation, we get
P2P1=ακ(T2T1){{P}_{2}}-{{P}_{1\,}}=\,\dfrac{\alpha }{\kappa }({{T}_{2}}-{{T}_{1}})
The final equation would be
P2=ακ(T2T1)+P1{{P}_{2}}_{\,}=\,\dfrac{\alpha }{\kappa }({{T}_{2}}-{{T}_{1}})\,+\,{{P}_{1}}
So, Isothermal compressibility κ\kappa of water is 4.7×105atm14.7\,\times \,{{10}^{-5}}\,at{{m}^{-1}}
And Expansion coefficient α\alpha of water is 1.7×104k11.7\,\times \,{{10}^{-4}}\,{{k}^{-1}}
P2=1atm+1.7×104K14.7×105atm1(6k){{P}_{2\,}}=\,1atm\,+\,\dfrac{1.7\,\times \,{{10}^{-4}}\,{{K}^{-1}}}{4.7\times {{10}^{-5\,}}at{{m}^{-1}}}(6k)
= 23 atm
So, the new pressure of liquid water using its isothermal compressibility κ\kappa and expansion coefficient α\alpha is 23 atm.

Note:
The compressibility factors have many applications like It forms a liquid when we compress petroleum gas. In oxygen cylinders that are used for medical facilities. It forms CNG. Methane gets compressed and used as fuel in vehicles.