Respuesta :
Answer:
408 J/kg
662696.7 J/kg
Explanation:
Workdone by compression process in a pump can be isothermally expressed as :
[tex]W = P_1V_1 \ In \frac{P_2}{P_1}[/tex]
For water at inlet pressure 1. 0 bar;
the specific values for :
saturated vapor [tex]v_g = 1.694 m^2 kg[/tex]
saturated liquid [tex]v_f = 0.001043 \ m^2 kg[/tex]
∴ we have
[tex]P_1[/tex] = 1.0 bar = 1. 0 × 10⁵ N/m²
[tex]P_2[/tex] = 50 bar = 50 × 10⁵ N/m²
For saturated water output from condenser work; we have
W = [tex]P_1V_f \ In (\frac{P_2}{P_1})[/tex]
W = [tex](1.0*10^{-5})(0.001043) In ( \frac{50}{10} ) J/kg[/tex]
W = 408 J/kg
For saturated vapor output from condenser
Work required :
[tex]W = P_1V_g \ In ( \frac{P_2}{P_1} )[/tex]
W = [tex]1.0*10^5*1.694 \ In ( \frac{50}{1.0}) J/kg[/tex]
W = 662696.7 J/kg
Answer:
The work per unit mass required for the liquid is 4.9 MJ
The work per unit mass required for the vapor is 0.639 MJ.
Explanation:
Per unit mass of vapor, we have
p₁ = 1 bar = 0.1 MPa
p₂ = 50 bar = 5 MPa
mass of saturated water = 1 kg
Volume of saturated water = 1 m³
Since the water is incompressible, we have
Pump work = v×(p₂ - p₁) = 1 m³ × (5 MPa - 1 MPa) = 4.9 MJ
For the steam, we have. 1 kg steam at 1 bar we have the specific volume v₁ = 1.694 m³/kg also
1 kg steam at 50 bar has a specific volume v₂ = 0.039 m³/kg
Since the internal energy is constant, that is ΔU = 0, then, the temperature can be assumed to be constant. Therefore, we have
Work done in moving from p₁ to p₂ is given by;
[tex]W_{p_1 \rightarrow p_2}[/tex] = [tex]nRTln\frac{V_{p1}}{V_{p2}}[/tex] = [tex]p_1 \cdot v_1\cdot ln\frac{V_{p1}}{V_{p2}}[/tex] = 1.694 × 0.1 MPa ×[tex]ln\frac{1.694}{0.039}[/tex] = 638855.89 J
= 0.639 MJ.