The process of a closed, rigid tank that contains Refrigerant 134a initially at 100°C is shown in the T-v diagram attached below.
Given that:
At 20° C from the property tables of R-134a
Final pressure p₂ = 5.176 bar
u₂ = 237.91 kJ/kg
T₁ is present in its vapor state since it is 100⁰ C
As such, by iteration from superheated property tables
[tex]\mathbf{p_1 = 7+(8-7) (\dfrac{0.0358-0.04064}{0.03519 -0.04064})}[/tex]
Initial pressure [tex]\mathbf{p_1 = 7.89 \ bar}[/tex]
Similarly;
[tex]\mathbf{u_1 = 309.74 +(308.93-309.74) (\dfrac{7.89-7}{8-7})}[/tex]
[tex]\mathbf{u_1 = 309.74 +(-0.81) (\dfrac{0.89}{1})}[/tex]
[tex]\mathbf{u_1 = 309.019 \ kJ/kg }[/tex]
(c) According to the first law of thermodynamics, heat energy is the change in the internal energy of an object.
Q - W = Δu
Q = u₂ - u₁ (since K.E and P.E are ignored, Volume = constant)
Q = 309.019 kJ/kg - 237.91 kJ/kg
Q = -71.109 kJ/kg
Thus, heat is lost in the process.
Therefore, we can conclude that the initial and final pressures are 7.89 bar and 5.176 bar respectively.
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