Question
Question: If \({C_P}\) and \[{C_V}\] denote the specific heats (per unit mass) of an ideal gas of molecular we...
If CP and CV denote the specific heats (per unit mass) of an ideal gas of molecular weight M, where R is the molar gas constant.
(A) CP−CV=R/M2
(B) CP−CV=R
(C) CP−CV=R/M
(D) CP−CV=M/R
Solution
Using the law of thermodynamics, we need to write the relations of CP and CV. Substituting the quantities of these two relations with the quantities from laws of thermodynamics, we can derive a relation between CP and CV.
Complete step by step solution:
We know the molar heat capacity of a substance at constant pressure is denoted by CP and heat transferred between a body and surrounding at constant volume is denoted by CV. Or in other words, molar heat capacity of a substance at constant volume.
From First law of thermodynamics, we know if the increase in internal energy be denoted by dUand dQ be the heat energy supplied, then work done dW is denoted by:
dQ=dU+dW
Rewriting the equation of first law by introducing the concepts Entropy and enthalpy.
Entropy of a system is the degree of disorderness of a system.
Enthalpy is defined as the sum of internal energy and product of pressure and volume.
Therefore, enthalpy is defined as:
H=U+PV
Where,
H is the enthalpy and Uis the internal energy.
Thus, we can write:
dH=dU+d(PV)
We know, that
PV=nRT
Putting this values, in the above equation, we get:
dH=dU+nRdT
We also know, from the equation of specific heat, that:
dH=mCPdT
Therefore, the equation becomes:
mCPdT=mCvdT+nRdT
Cancelling the common term from both sides,
mCP=mCv+nR
⇒mCP−mCv=nR
This can be written as:
mCP−mCv=nR=MRm
Thus, we obtain CP−Cv=MR
This is our required solution.
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Hence, option Cis correct.
Note: The value of CP is always greater thanCv. This happens because at constant pressure, when heat is added to the substance, expansion occurs in the substance and hence work is done.