Skip to content
    Calculates locally in your browser · LMTD and effectiveness-NTU
    Heat transfer / exchanger design

    Heat exchanger sizing

    Size a counterflow exchanger two ways: from the mean temperature difference given the terminal temperatures, or from the effectiveness-NTU relation given the installed area. The two must agree, and the gap between them is the design margin.

    Flow arrangementCounterflowC_r0.75Terminal ΔT80.0 / 65.0 K
    Heat duty
    627.0 kW
    Transferred from hot to cold stream
    LMTD
    72.24 K
    Driving temperature difference
    Effectiveness
    0.480
    Fraction of the thermodynamic maximum
    NTU
    0.98
    Dimensionless size of the exchanger
    Exchanger operating point
    Duty, mean temperature difference and the dimensionless performance measures.
    627.0 kW duty
    Exchanger operating point
    QuantityValueBasis
    Heat duty Q627.00 kWm·cp·ΔT on the hot side
    Hot-side capacity10.450 kW/Km_h·cp
    Cold-side capacity13.933 kW/Kfrom the energy balance
    LMTD72.24 Kcounterflow terminal differences
    NTU0.976UA/C_min
    Capacity ratio C_r0.750C_min/C_max
    Effectiveness ε0.4800Q/Q_max
    Area from LMTD10.21 m²Q/(U·LMTD)
    UA installed10.20 kW/KU × A

    LMTD sizing and effectiveness-NTU answer the same question from opposite ends: one asks for area given temperatures, the other asks for duty given area.

    Inspect the model
    Choose a quick result view, a scaled comparison, or the complete diagnostic set.
    Temperature profiles
    Hot stream falls, cold stream rises; counterflow keeps the terminal differences large.
    Temperature profiles0.00033.6067.20100.80134.40168.000.00.00.20.20.40.40.60.60.80.81.01.0HotCold
    Effectiveness vs NTU
    Diminishing returns: doubling NTU beyond about 3 buys very little.
    Effectiveness vs NTU0.0000.2220.4450.6670.8901.110.250.250.500.501.001.001.501.502.002.003.003.004.004.005.005.00ε at this C_rε at C_r = 0
    Canonical equations
    The exact relationships implemented by this engine.

    Q = m·cp·ΔT · either stream gives the same answer

    (ΔT₁−ΔT₂)/ln(ΔT₁/ΔT₂) · counterflow terminal differences

    UA/C_min · dimensionless size

    Q/Q_max · Q_max = C_min(T_h,in − T_c,in)

    engineering methodology

    A clear path from inputs to results.

    Exchanger sizing is asked two ways: what area do these temperatures require, or what duty does this installed area deliver? LMTD answers the first, effectiveness-NTU the second, and a sound design reconciles them.

    Step-by-step methodWorked exampleAssumptions explained

    How to use

    1. Enter the four terminal temperatures.
    2. Set the hot-side mass flow and specific heat.
    3. Enter the overall heat transfer coefficient and the installed area.
    4. Read the duty, LMTD, NTU and effectiveness.
    5. Compare the LMTD-implied area with the installed area to see the margin.

    The formula

    Q=m˙cpΔT,LMTD=ΔT1−ΔT2ln⁡(ΔT1/ΔT2),NTU=UACmin⁡,ε=QQmax⁡Q = \dot{m}c_p\Delta T, \quad \mathrm{LMTD} = \frac{\Delta T_1-\Delta T_2}{\ln(\Delta T_1/\Delta T_2)}, \quad \mathrm{NTU} = \frac{UA}{C_{\min}}, \quad \varepsilon = \frac{Q}{Q_{\max}}

    Reference: Incropera & DeWitt, "Fundamentals of Heat and Mass Transfer", ch. 11.

    Worked example

    150 → 90 °C hot, 25 → 70 °C cold, 2.5 kg/s water

    Inputs
    • Hot 150 → 90 °C; cold 25 → 70 °C.
    • 2.5 kg/s at cp 4.18 kJ/kg·K.
    • U 850 W/m²K, area 12 m².
    Calculation path
    1. 1

      Duty: 2.5 × 4.18 × 60 = 627 kW.

    2. 2

      Counterflow terminal differences: 150 − 70 = 80 K; 90 − 25 = 65 K.

    3. 3

      LMTD: (80 − 65)/ln(80/65) = 72.2 K.

    4. 4

      NTU = 850 × 12 / (2.5 × 4.18 × 1000) = 0.976.

    5. 5

      Effectiveness: 627 / (10.45 × 125) = 0.48.

    Result

    627 kW · LMTD 72.2 K · NTU 0.98 · effectiveness 0.48.

    Interpreting the result

    An effectiveness of 0.48 means the exchanger captures less than half of the thermodynamic maximum. Doubling the area would push NTU to about 2 and effectiveness to roughly 0.7 — real but diminishing. Beyond NTU 3 the curve flattens, which is why very large exchangers are rarely economic.

    Assumptions & limitations

    • Steady state with constant fluid properties and no phase change.
    • No fouling resistance; in service, fouling can cut U by 30–50%.
    • No heat loss to ambient and no axial conduction.
    • Counterflow arrangement; parallel flow gives lower effectiveness for the same NTU.

    Frequently asked questions

    Why counterflow rather than parallel flow?

    Because counterflow keeps the terminal temperature differences larger, which raises the LMTD and the effectiveness for the same area. Parallel flow also cannot cool the hot stream below the cold outlet.

    How much fouling margin should I add?

    Typically 10–25% extra area, depending on the fluid. Fouling factors are tabulated by TEMA, and the margin should be explicit in the design rather than hidden in a fudged U.

    What is a temperature cross?

    When the cold outlet would exceed the hot inlet, which is impossible in a single-pass exchanger. It signals that the specified duty cannot be achieved with the chosen arrangement.

    What if the fluids have very different capacities?

    Then C_r is small and the effectiveness approaches 1 − exp(−NTU), the same as a condenser or evaporator where one stream is nearly isothermal.

    Methodology last reviewed 2026-10-18. Results are informational and not financial or engineering advice — see our disclaimer.