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Reheat Rankine cycle: 20 MPa, 500°C

Short answer

By matching isentropic expansions: LP inlet entropy from exhaust dryness forces reheat pressure ≈ 1.5 MPa via interpolation. Net work = 1735.7 kJ/kg, heat added = 3906.7 kJ/kg, giving thermal efficiency ≈ 44.4%.

A steam power plant running on Rankine cycle has steam entering HP turbine at 20 MPa, 500°C and leaving LP turbine at 89.6 % dryness. Considering condenser pressure of 0.005 MPa and reheating occurring upto the temperature of 500°C determine: a) the pressure at which steam leaves HP turbine b) the thermal efficiency. [Refer the attached table for the properties of steam]

Assumptions: ideal reheat Rankine cycle, isentropic turbines and pump, pump work included. Values from steam tables (IAPWS-IF97).

States: 1 = 20 MPa, 500 C (HP inlet); 2 = HP exit at reheat pressure prp_r; 3 = prp_r, 500 C (LP inlet); 4 = 0.005 MPa, x=0.896x = 0.896; 5 = saturated water at 5 kPa; 6 = pump exit.

Steam table data

StateData
5 kPa sat.t=32.88t = 32.88 C, hf=137.77h_f = 137.77, hfg=2423.0h_{fg} = 2423.0, sf=0.4763s_f = 0.4763, sfg=7.9177s_{fg} = 7.9177, vf=0.001005v_f = 0.001005
20 MPa, 500 Ch1=3241.2h_1 = 3241.2, s1=6.1445s_1 = 6.1445

(a) Pressure at which steam leaves the HP turbine

State 4:

s4=0.4763+0.896×7.9177=7.5705 kJ/kg Kh4=137.77+0.896×2423.0=2308.8 kJ/kg\begin{aligned} s_4 &= 0.4763 + 0.896 \times 7.9177 = 7.5705\ \text{kJ/kg K} \\ h_4 &= 137.77 + 0.896 \times 2423.0 = 2308.8\ \text{kJ/kg} \end{aligned}

LP expansion is isentropic, so s3=s4=7.5705s_3 = s_4 = 7.5705 at 500 C. From the superheated table at 500 C: s=7.6045s = 7.6045 at 1.4 MPa and s=7.5407s = 7.5407 at 1.6 MPa. Interpolating:

pr=1.4+0.2×7.6045−7.57057.6045−7.5407=1.507≈1.5 MPap_r = 1.4 + 0.2 \times \frac{7.6045 - 7.5705}{7.6045 - 7.5407} = 1.507 \approx 1.5\ \text{MPa}

Taking pr=1.5p_r = 1.5 MPa: at 1.5 MPa, 500 C, h3=3473.6h_3 = 3473.6 kJ/kg.

Answer (a): steam leaves the HP turbine at about 1.5 MPa.

State 2 (1.5 MPa, s2=s1=6.1445s_2 = s_1 = 6.1445)

At 1.5 MPa: hf=844.7h_f = 844.7, hfg=1946.3h_{fg} = 1946.3, sf=2.3147s_f = 2.3147, sfg=4.1284s_{fg} = 4.1284.

x2=6.1445−2.31474.1284=0.9277h2=844.7+0.9277×1946.3=2650.2 kJ/kg\begin{aligned} x_2 &= \frac{6.1445 - 2.3147}{4.1284} = 0.9277 \\ h_2 &= 844.7 + 0.9277 \times 1946.3 = 2650.2\ \text{kJ/kg} \end{aligned}

Pump

Wp=0.001005(20000−5)=20.10 kJ/kgh6=137.77+20.10=157.87 kJ/kg\begin{aligned} W_p &= 0.001005 (20000 - 5) = 20.10\ \text{kJ/kg} \\ h_6 &= 137.77 + 20.10 = 157.87\ \text{kJ/kg} \end{aligned}

(b) Thermal efficiency

WT=(h1−h2)+(h3−h4)=(3241.2−2650.2)+(3473.6−2308.8)=591.0+1164.8=1755.8 kJ/kgWnet=1755.8−20.1=1735.7 kJ/kgQs=(h1−h6)+(h3−h2)=(3241.2−157.87)+(3473.6−2650.2)=3083.3+823.4=3906.7 kJ/kgη=1735.73906.7=0.4443\begin{aligned} W_T &= (h_1 - h_2) + (h_3 - h_4) \\ &= (3241.2 - 2650.2) + (3473.6 - 2308.8) \\ &= 591.0 + 1164.8 = 1755.8\ \text{kJ/kg} \\ W_{net} &= 1755.8 - 20.1 = 1735.7\ \text{kJ/kg} \\ Q_s &= (h_1 - h_6) + (h_3 - h_2) \\ &= (3241.2 - 157.87) + (3473.6 - 2650.2) \\ &= 3083.3 + 823.4 = 3906.7\ \text{kJ/kg} \\ \eta &= \frac{1735.7}{3906.7} = 0.4443 \end{aligned}

Answer (b): thermal efficiency ≈44.4%\approx 44.4\% (net work 1735.7 kJ/kg).

  T
  ^                  1          3
  |                 /|         /|
  |                / |        / |
  |     f--------g'  |       /  |
  |    /             2------'   |
  |   /                         |
  |  6                          |
  |  5--------------------------4
  +--------------------------------> s
  5-6 pump, 6-f-g'-1 boiler (heat,
  boil, superheat), 1-2 HP turbine,
  2-3 reheater, 3-4 LP turbine,
  4-5 condenser

✓ Answer checked by Claude Opus 5.5 (high effort)

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