The PV diagram shows the compression of 60.1 moles of an
ideal monoatomic gas from state A to state B. Calculate Q,
the heat added to the gas in the process A to B. Data: PA=
1.84E+5 N/m2 VA= 1.97E+0 m3 PB= 1.15E+5 N/m2 VB=
9.30E-1 m3
Q = deltaU + W
What is deltaU?
Well, Ua and Ub...
deltaU = Ub - Ua
To find the value of U at both states, use the calorically perfect assumption:
Ua = n*cv*Ta
Ub = n*cv*Tb
What is molar cv in terms of more easy to remember values?
cv = R/(k - 1)
where k is the adiabatic index. Later we will assign k=5/3 because it is a monatomic gas.
Thus:
deltaU = n*R*(Tb - Ta)/(k - 1)
Recognize ideal gas law, such that:
Ta = Pa*Va/(n*R)
Tb = Pb*Vb/(n*R)
Thus:
deltaU = (Pb*Vb - Pa*Va)/(k - 1)
So we can develop our expression for Q:
Q = (Pb*Vb - Pa*Va)/(k - 1) + 1/2*(Pb + Pa)*(Vb - Va)
If you care, our resulting expressions for work and internal energy change:
W = 1/2*(Pb + Pa)*(Vb - Va)
deltaU = (Pb*Vb - Pa*Va)/(k - 1)
Data:
Pa:= 183 kPa; Pb:=115 kPa; Va:=1.97 m^3; Vb:=0.930 m^3;
W= -154.96 , deltaU= -380.34
Result:Q = -535.3 kiloJoules, negative sign indicates gas rejects heat to the surroundings
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