LMTD Calculator (Log Mean Temperature Difference & HX Area)

The log mean temperature difference is the true average driving force for heat transfer between two fluids in a heat exchanger. This LMTD calculator works out the LMTD from the four terminal temperatures for counterflow or parallel flow, then sizes the exchanger with Q = U·A·LMTD — see the types of heat exchangers and how a plate heat exchanger works.

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Type in any field to change it. Press × on a value to calculate that field instead.

How to use the LMTD calculator

Choose counterflow or parallel flow and enter the inlet and outlet temperatures of both fluids. The calculator returns ΔT₁, ΔT₂ and the LMTD. Enter the overall heat transfer coefficient U and the heat duty Q to get the required area — or clear Q and enter an area to find how much heat an existing exchanger can transfer.

LMTD formula

LMTD = (ΔT₁ − ΔT₂) ÷ ln(ΔT₁ ÷ ΔT₂)  ·  Q = U × A × LMTD

Worked example

Hot oil cools from 150 °C to 90 °C, water heats from 30 °C to 70 °C, counterflow, U = 500 W/m²·K, duty 250 kW:

  • ΔT₁ = 150 − 70 = 80 K, ΔT₂ = 90 − 30 = 60 K
  • LMTD = (80 − 60) ÷ ln(80 ÷ 60) = 69.52 K
  • A = 250,000 ÷ (500 × 69.52) = 7.19 m²

In parallel flow the same temperatures give ΔT₁ = 120 K, ΔT₂ = 20 K and LMTD = 55.81 K, so 8.96 m² would be needed.

LMTD vs arithmetic mean

ΔT₁ ΔT₂ Arithmetic mean LMTD
80 K 60 K 70 K 69.52 K
60 K 40 K 50 K 49.33 K
50 K 10 K 30 K 24.85 K
40 K 20 K 30 K 28.85 K
30 K 15 K 22.5 K 21.64 K
20 K 5 K 12.5 K 10.82 K
100 K 50 K 75 K 72.13 K
10 K 9 K 9.5 K 9.49 K

The arithmetic mean always overstates the driving force; the error is small only when ΔT₁ and ΔT₂ are close.

Notes

  • If ΔT₁ = ΔT₂ the formula is 0 ÷ 0 — the LMTD then equals that common ΔT.
  • A temperature cross (ΔT ≤ 0 at one end) is impossible for the chosen arrangement — check the temperatures.
  • Typical U values: water–water plate exchanger 2,000–6,000 W/m²·K, shell-and-tube water–water 800–1,500, oil–water 100–400, gas–gas 10–50.

Frequently asked questions

What is the LMTD formula?

LMTD = (ΔT₁ − ΔT₂) ÷ ln(ΔT₁ ÷ ΔT₂), where ΔT₁ and ΔT₂ are the hot-to-cold temperature differences at the two ends of the exchanger.

How are ΔT₁ and ΔT₂ defined for counterflow?

For counterflow, ΔT₁ = hot inlet − cold outlet and ΔT₂ = hot outlet − cold inlet. For parallel flow, ΔT₁ = hot inlet − cold inlet and ΔT₂ = hot outlet − cold outlet.

Why is counterflow better than parallel flow?

With the same terminal temperatures counterflow gives a larger LMTD, so it needs less area, and it lets the cold outlet temperature rise above the hot outlet temperature.

What about shell-and-tube exchangers with several passes?

Multiply the counterflow LMTD by a correction factor F (usually 0.75–1.0 from TEMA charts) — Q = U·A·F·LMTD. Designs with F below about 0.8 are normally avoided.

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