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    Calculates locally in your browser · Rankine cycle with regeneration
    Thermodynamics / power cycles

    Rankine cycle with regeneration

    Regeneration bleeds some steam out of the turbine part-way through the expansion and uses it to preheat the feedwater. The bleed gives up its latent heat to the feedwater instead of to the condenser, so less heat is thrown away at the cold end — and the mean temperature of heat addition rises without raising the boiler pressure at all.

    PlacementNear optimumGain2.9 ptBleed1.0 bar
    Efficiency
    30.6%
    +2.9 points over no bleed
    Bleed fraction
    10.0%
    of the boiler flow
    Feedwater enthalpy
    418 kJ/kg
    preheated at the extraction pressure
    Optimum bleed
    1.00 bar
    the geometric mean of the two pressures
    The heater energy balance
    The bleed steam condenses at the extraction pressure and heats the condensate to saturation there.
    10.0%
    The heater energy balance
    QuantityValueNote
    Boiler pressure10.0 baras entered
    Extraction pressure1.00 barnear the optimum
    Condenser pressure0.10 baras entered
    h₁ turbine inlet2777 kJ/kgsaturated vapour
    h₂ at extraction2445 kJ/kgafter the first expansion
    h₃ at condenser2011 kJ/kgafter the second
    Condensate enthalpy340.5 kJ/kgat the condenser pressure
    Feedwater enthalpy418 kJ/kgsaturated liquid at the extraction pressure
    Bleed fraction10.02%from the heater balance
    Turbine work722 kJ/kghigh pressure plus the remainder
    Net work721 kJ/kgless two pumps
    Efficiency30.6%simple cycle 27.7%

    Extracting 10.0% of the flow at 1.0 bar raises efficiency by 2.9 points. The optimum bleed pressure is near the geometric mean of the boiler and condenser pressures, about 1.0 bar — this one is close.

    Inspect the model
    Choose a quick result view, a scaled comparison, or the complete diagnostic set.
    Efficiency against extraction pressure
    A clear maximum: too low and the feedwater is barely heated, too high and too much work is lost.
    Efficiency against extraction pressure0.0007.2214.4521.6728.8936.120.2 bar0.2 bar0.5 bar0.5 bar1 bar1 bar2 bar2 bar4 bar4 barEfficiency %
    Mass and work
    The bled fraction never reaches the low-pressure stages, which is the cost of the gain.
    Mass and work0.000170.20340.40510.60680.80851.0010.02BledBled89.98ContinuesContinues721.19Net workNet workValue
    Canonical equations
    The exact relationships implemented by this engine.

    y = (h_fw − h_f)/(h₂ − h_f) · Heater energy balance.

    w = (h₁ − h₂) + (1−y)(h₂ − h₃) · The bleed skips the low stages.

    √(P_boiler × P_condenser) · Geometric mean.

    (w − Σ pumps)/q_in · Two pumps, weighted by flow.

    engineering methodology

    A clear path from inputs to results.

    Regeneration bleeds some steam out of the turbine part-way through the expansion and uses it to preheat the feedwater. The bleed gives up its latent heat to the feedwater instead of to the condenser, so less heat is thrown away at the cold end.

    Step-by-step methodWorked exampleAssumptions explained

    How to use

    1. Set the boiler and condenser pressures.
    2. Choose the extraction pressure.
    3. Enter the turbine and pump efficiencies.
    4. Read the bleed fraction and the efficiency gain.

    The formula

    y=hfw−hfh2−hfy = \frac{h_{fw} - h_f}{h_2 - h_f}

    Reference: Energy balance on an open feedwater heater, with saturated properties from IAPWS-IF97.

    Worked example

    10 bar boiler, extraction at 1 bar

    Inputs
    • Boiler 10 bar, extraction 1 bar, condenser 0.1 bar.
    • Turbine 85%, pump 80%.
    Calculation path
    1. 1

      The expansion to 1 bar gives 2,592 kJ/kg at the extraction point.

    2. 2

      The feedwater has to be heated from 192 to 417 kJ/kg.

    3. 3

      The bleed fraction is (417 − 192)/(2,592 − 192) = 15.4%.

    4. 4

      The remaining 84.6% continues to the condenser.

    5. 5

      Efficiency rises from 27.7% to 29.6%, about two points, from a single heater.

    Result

    15.4% bled · 29.6% · +2.0 points.

    Interpreting the result

    The optimum extraction pressure is the geometric mean of the boiler and condenser pressures, and the curve around it is fairly flat. A real plant uses five to seven heaters at different pressures and gains eight to twelve points — which is why regeneration, not reheat, is the larger of the two improvements.

    Assumptions & limitations

    • One open feedwater heater.
    • Saturated vapour extracted, heater reaching saturation at the extraction pressure.
    • Two pumps, weighted by the mass flow through each.
    • No pressure loss in the heater or the extraction line.

    Frequently asked questions

    Why does bleeding steam help?

    Because the bled steam condenses at the extraction pressure and gives its latent heat to the feedwater, raising the temperature at which heat enters the boiler — and the mean temperature of heat addition is what sets the efficiency.

    Why is the optimum at the geometric mean?

    Because the benefit falls as the extraction pressure drops and the work penalty rises; the two cross near the geometric mean of the boiler and condenser pressures.

    Does regeneration work with reheat?

    Yes, and the two are used together: the reheat raises the top temperature and the regeneration raises the average, which is why a modern plant reaches 45%.

    What does it cost?

    The bled fraction never reaches the low-pressure stages, so turbine work falls. The gain comes because the heat saved in the boiler is larger than the work lost.

    How many heaters does a real plant use?

    Five to seven, in a train of closed heaters plus a deaerator, each at a different pressure. The total gain is 8–12 points rather than the two a single heater gives.

    Methodology last reviewed 2026-10-22. Results are informational and not financial or engineering advice — see our disclaimer.