Water is the working fluid in an ideal Rankine cycle. Steam enters the turbine at 1400 lbf/in2 and 1000°F. The net power output of the cycle is 1 x 109 Btu/hr. Cooling water experiences a temperature increase from 60°F to 76°F, with negligible pressure drop, as it passes through the condenser.

a) The mass flow rate of steam, in lb/h
b) The rate of heat transfer, in Btu/h, to the working fluid passing through the steam generator
c) The thermal efficiency
d) The mass flow rate of cooling water, in lb/h

Respuesta :

Answer:

(a) The mass flow rate of the steam is approximately 1.803×10⁶ lb/h

(b) The rate of heat transfer is approximately 2.52×10⁹ BTU/h

(c) The thermal efficiency  is approximately 39.68%

(d) The mass flow rate of cooling water is approximately 9.478 × 10⁷ lb/h

Explanation:

(a) The parameters are;

T₁ = 1000 F, P₁ = 1400 psi

By using an online application, we have;

h₁ = 1494 BTU/lb = 3,475 kJ/kg

s₁ = 1.61 BTU/(lb·R) =  6.741 kJ/(kg·K)

Therefore, due to isentropic expansion from state 1 to state 2, we have;

s₁ = s₂ = 1.61 BTU/(lb·R)

P₂ = 2 psi

T₂ =

[tex]s_f[/tex] = 0.17498 BTU/(lb·R)

[tex]h_{f2}[/tex] = 94.02 BTU/(lb)

[tex]h_g[/tex] = 1116 BTU/lb

[tex]s_g[/tex] = 1.919 BTU/(lb·R)

We have;

x₂ = (1.61 - 0.17498)/(1.919 - 0.17498) ≈ 0.823

h₂ = [tex]h_f[/tex] + x₂×([tex]h_g[/tex] -

P₃ = P₂ = 2 psi

h₃ = [tex]h_{f2}[/tex] = 94.02 BTU/(lb)

v₃ = 0.01605 ft³/lb

h₄ = h₃ + v₃ × (P₄ - P₃)

h₄ = 94.02 + 0.01605 × (1400 - 2) ×144/778 = 98.17 BTU/lb

The mass flow rate of the steam, [tex]\dot m[/tex] = [tex]\dot W[/tex]/((h₁ - h₂) - (h₄ - h₃)) = 1 * 10^9/((1494 -935.11) - (98.17 -94.02)) ≈ 1.803×10⁶ lb/h

[tex]\dot m[/tex] ≈ 1.803×10⁶ lb/h

The mass flow rate of the steam ≈ 1.803×10⁶ lb/h

(b)The rate of heat transfer, [tex]\dot Q_{in}[/tex] = [tex]\dot m[/tex] × (h₁ - h₄) = 1.803×10⁶×(1494 -98.17) ≈ 2.52×10⁹ BTU/h

[tex]\dot Q_{in}[/tex]  ≈ 2.52×10⁹ BTU/h

(c) The thermal efficiency =  [tex]\dot W_{cyc}[/tex]/[tex]\dot Q_{in}[/tex] = 1×10⁹/(2.52×10⁹) = 0.3968 ≈ 39.68%

The thermal efficiency ≈ 39.68%

(d) The mass flow rate of cooling water [tex]\dot m_w[/tex] = [tex]\dot m[/tex](h₂- h₃)/([tex]c_w \Delta T[/tex])

[tex]c_w[/tex] = 1 BTU/(lb·°F)

[tex]\dot m_w[/tex] =  1.803×10⁶ (935.11- 94.02)/(1 * (76 - 60)) ≈ 9.478 × 10⁷ lb/h

[tex]\dot m_w[/tex] ≈ 9.478 × 10⁷ lb/h

The mass flow rate of cooling water ≈ 9.478 × 10⁷ lb/h.

A) The mass flow rate of steam, in lb/h is; 1.803 × 10⁶ lb/h

B) The rate of heat transfer, in Btu/h, to the working fluid passing through the steam generator is; 2.52 × 10⁹ btu/h

C) The thermal efficiency is; 39.68%

D) The mass flow rate of cooling water, in lb/h is; 9.478 × 10⁷ lb/h

Thermal Efficiency and Mass Flow rate

We are given;

  • Inlet Temperature; T₁ = 1000 F
  • Inlet Pressure; P₁ = 1400 psi
  • Power Output; W' = 1 * 10⁹ btu/hr

From online thermodynamic property table, we have;

enthalpy at inlet; h₁ = 1494 Btu/lbm

entropy at inlet; s₁ = 1.61 Btu/lbm·R

Now, since there is an isentropic expansion from state 1 to state 2, then we can say that;

s₁ = s₂ = 1.61 Btu/lbm·R

Also at s₂ = 1.61 Btu/lbm·R, from thermodynamics steam property table online, we have;

P₂ = 2 psi

Entropy of saturated Liquid; s_f = 0.17498  Btu/lbm·R

Enthalpy of saturated liquid; h_f₂ = 94.02 Btu/lbm

Enthalpy of evaporation liquid; h_g = 1116 Btu/lbm

Entropy of saturation vapour; s_g = 1.919 Btu/lbm.R

A) Thus, quality of steam at second state is calculated from;

x₂ = (s₂ - s_f)/(s_g - s_f)

x₂ = (1.61 - 0.17498)/(1.919 - 0.17498)

x₂ = 0.823

formula for enthalpy at second state;

h₂ = h_f + x₂(h_g - h_f)

h₂ = 94.02 + 0.823(1116 - 94.02)

h₂ = 935.11 Btu/lbm.R

Similar to the first to second state, we can equally say that;

P₃ = P₂ = 2 psi

h₃ = h_f₂ = 94.02 Btu/lbm

From online thermodynamic steam tables, for those values at state 3, we have;

Specific Volume; ν₃ = 0.01605 ft³/lb = 0.0029707 btu/lb

Enthalpy at state 4 is;

h₄ = h₃ + (v₃(P₄ - P₃))

h₄ = 94.02 + 0.0029707(1400 - 2)

h₄ = 98.17 Btu/lbm

Mass flow rate of the steam is calculated from;

m' = W'/[(h₁ - h₂) - (h₄ - h₃)]

m' = (1 × 10⁹)/((1494 -935.11) - (98.17 -94.02))

m' = 1.803 × 10⁶ lb/h

B) Rate of the heat transfer is calculated from;

Q' = m'(h₁ - h₄)

Q' = 1.803 × 10⁶ ×(1494 - 98.17)

Q' = 2.52 × 10⁹ btu/h

C) Thermal efficiency is gotten from the formula;

η = W'/Q'

η = (1 × 10⁹)/(2.52×10⁹)

η = 39.68%

D) The mass flow rate of cooling water is calculated from;

m'_w = m'(h₂- h₃)/(c_w * Δt)

c_w is specific heat capacity of cool water = 1 Btu/(lb·°F)

Thus;

m'_w = 1.803 × 10⁶(935.11 - 94.02)/(1 × (76 - 60))

m'_w ≈ 9.478 × 10⁷ lb/h

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