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Regenerative cycle: 4 MPa, 400°C, open heater

Short answer

Cycle efficiency ≈ 37.5%. Using steam table data: h1=3214.4, h2=2686.3, h3=2144.5 kJ/kg; pump work 4.23 kJ/kg; bleed fraction m=0.1654 from open FWH energy balance. Net work 976.1 kJ/kg, heat input 2605.7 kJ/kg.

On a regenerative cycle, steam leaves the boiler and enters the turbine at 4 MPa, 400°C. After expansion to 400 kPa, some of the steam is extracted from the turbine to heat the feed water in an open feed water heater. The pressure in the feed water heater is 400 kPa, and the water leaving it is saturated liquid at 400 kPa. The steam not extracted expands to 10kPa. Determine the cycle efficiency. [Refer the attached table for the properties of steam]

Assumptions: ideal regenerative Rankine cycle with one open feed water heater; turbine and pumps isentropic; exit of heater is saturated liquid at 400 kPa; pump work included. Property values are taken from the steam tables (IAPWS-IF97 values, as in Cengel's tables).

              1
  +--------+------>+---------------+   +-----+
  | Boiler |       |    Turbine    |===| Gen |
  |  + S/H |       +---------------+   +-----+
  +--------+          | m kg (2)  | (1-m) kg (3)
      ^ 7             v           v
      |         +-----------+ +-----------+
  +--------+  6 |  Open FWH | | Condenser |
  | Pump 2 |<---| (mixing)  | +-----------+
  +--------+    +-----------+       | 4
                      ^ 5           |
                 +--------+         |
                 | Pump 1 |<--------+
                 +--------+

Steam table data

Pressuretsatt_{sat} (°C)hfh_fhfgh_{fg}sfs_fsfgs_{fg}vfv_f (m³/kg)
10 kPa45.81191.812392.070.64927.49970.001010
400 kPa143.61604.722133.331.77665.11880.001084

At 4 MPa, 400 °C (superheated): h1=3214.4h_1 = 3214.4 kJ/kg, s1=6.7712s_1 = 6.7712 kJ/kg K.

State 2 (bled steam, 400 kPa, s2=s1s_2 = s_1)

x2=6.7712−1.77665.1188=0.9757h2=604.72+0.9757×2133.33=2686.3 kJ/kg\begin{aligned} x_2 &= \frac{6.7712 - 1.7766}{5.1188} = 0.9757 \\ h_2 &= 604.72 + 0.9757 \times 2133.33 = 2686.3\ \text{kJ/kg} \end{aligned}

State 3 (exhaust, 10 kPa, s3=s1s_3 = s_1)

x3=6.7712−0.64927.4997=0.8163h3=191.81+0.8163×2392.07=2144.5 kJ/kg\begin{aligned} x_3 &= \frac{6.7712 - 0.6492}{7.4997} = 0.8163 \\ h_3 &= 191.81 + 0.8163 \times 2392.07 = 2144.5\ \text{kJ/kg} \end{aligned}

Pumps

Wp1=vf(p5−p4)=0.001010(400−10)=0.39 kJ/kgh5=191.81+0.39=192.20 kJ/kgWp2=0.001084(4000−400)=3.90 kJ/kgh7=h6+Wp2=604.72+3.90=608.62 kJ/kg\begin{aligned} W_{p1} &= v_f (p_5 - p_4) = 0.001010(400 - 10) = 0.39\ \text{kJ/kg} \\ h_5 &= 191.81 + 0.39 = 192.20\ \text{kJ/kg} \\ W_{p2} &= 0.001084(4000 - 400) = 3.90\ \text{kJ/kg} \\ h_7 &= h_6 + W_{p2} = 604.72 + 3.90 = 608.62\ \text{kJ/kg} \end{aligned}

Bled steam fraction (energy balance on open FWH)

mh2+(1−m)h5=h6m h_2 + (1-m) h_5 = h_6:

m=h6−h5h2−h5=604.72−192.202686.3−192.20=0.1654 kg/kgm = \frac{h_6 - h_5}{h_2 - h_5} = \frac{604.72 - 192.20}{2686.3 - 192.20} = 0.1654\ \text{kg/kg}

Work and heat (per kg of steam at boiler exit)

WT=(h1−h2)+(1−m)(h2−h3)=528.1+0.8346×541.8=980.3 kJ/kgWP=(1−m)Wp1+Wp2=0.33+3.90=4.23 kJ/kgWnet=980.3−4.23=976.1 kJ/kgQs=h1−h7=3214.4−608.62=2605.7 kJ/kg\begin{aligned} W_T &= (h_1 - h_2) + (1-m)(h_2 - h_3) \\ &= 528.1 + 0.8346 \times 541.8 = 980.3\ \text{kJ/kg} \\ W_P &= (1-m) W_{p1} + W_{p2} = 0.33 + 3.90 = 4.23\ \text{kJ/kg} \\ W_{net} &= 980.3 - 4.23 = 976.1\ \text{kJ/kg} \\ Q_s &= h_1 - h_7 = 3214.4 - 608.62 = 2605.7\ \text{kJ/kg} \end{aligned}

Cycle efficiency

η=WnetQs=976.12605.7=0.3746\eta = \frac{W_{net}}{Q_s} = \frac{976.1}{2605.7} = 0.3746

Answer: cycle efficiency ≈37.5%\approx 37.5\% (bled fraction m=0.165m = 0.165 kg per kg of steam).

  T
  ^                    1
  |                   /|
  |      f----------g  |
  |     /              |
  |    7               |
  |    6 . . . . . . . 2  bleed (m kg)
  |   /                |
  |  5                 |
  |  4-----------------3  (1-m) kg
  +-------------------------> s
  4-5 pump 1, 5 and 2 mix in FWH -> 6,
  6-7 pump 2, 7-f-g-1 boiler,
  1-2-3 turbine, 3-4 condenser

For comparison, a simple Rankine cycle between the same limits gives about 35.3%, so one open heater raises the efficiency by about 2 percentage points.

✓ Answer checked by Claude Opus 5.5 (high effort)

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