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Question: What is the relationship between \[{C_p}\] and \[{C_v}\] for an Ideal Gas?...

What is the relationship between Cp{C_p} and Cv{C_v} for an Ideal Gas?

Explanation

Solution

Cp{C_p} is the specific heat at constant pressure and Cv{C_v} is the specific heat at constant volume.
At constant pressure we getCP>CV{C_P} > {C_V}.
Formula used: We will use the following formula in the solution,
q=nCΔTq = nC\Delta T
Where qq is the heat
CC is the specific heat and
ΔT\Delta T is the temperature change.

Complete step by step solution:
We have the formula q=nCΔTq = nC\Delta T
So at constant pressure P we can write
qp=nCpΔT{q_p} = n{C_p}\Delta T
The above formula is equal to the change in enthalpy.
Therefore,
qp=nCpΔT=ΔH{q_p} = n{C_p}\Delta T = \Delta H
Now at constant volume V we can write
qV=nCVΔT{q_V} = n{C_V}\Delta T
The above formula is equal to the change in internal energy that is,
qV=nCVΔT=ΔU{q_V} = n{C_V}\Delta T = \Delta U
For an ideal gas equation we have n = 1 for 1 mole
ΔH=ΔU+Δ(PV)\Delta H = \Delta U + \Delta (PV)
ΔH=ΔU+Δ(RT)\Rightarrow \Delta H = \Delta U + \Delta (RT)
Hence we can write,
ΔH=ΔU+RΔ(T)\Rightarrow \Delta H = \Delta U + R\Delta (T)
Now putting value of ΔH\Delta H and ΔU\Delta U in the above equation we get,
CPΔT=CVΔT+RΔT{C_P}\Delta T = {C_V}\Delta T + R\Delta T
Cancelling ΔT\Delta Tfrom the above equation we get
CP=CV+R{C_P} = {C_V} + R
Which gives,
CPCV=R{C_P} - {C_V} = R
Therefore the relationship between Cp{C_p} and Cv{C_v}for an Ideal Gas equation is:
CPCV=R{C_P} - {C_V} = R
Additional information: Cp{C_p}, the specific heat at constant pressure, is the amount of heat energy released or absorbed by a unit mass of the substance with the change in temperature at constant pressure.
Cp=(ΔHΔT)P{C_p} = {(\dfrac{{\Delta H}}{{\Delta T}})_P}
Where ΔH\Delta H is the change in enthalpy and ΔT\Delta T is the change in temperature at constant pressure.
Cv{C_v} is the heat energy transfer between a system and its surrounding without any change in the volume of the system.
CV=(ΔUΔT)V{C_V} = {(\dfrac{{\Delta U}}{{\Delta T}})_V}
Where ΔU\Delta U is the change in internal energy ΔT\Delta T is the change in temperature at constant volume.
At constant pressure Cp{C_p}>Cv{C_v}

Note: We should remember that Cp{C_p} is linked with change in enthalpy and Cv{C_v} is linked with change in internal energy, because if these are swapped then, we will not get the correct relation between both.