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[Heat Integration]
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Pinch Analysis

Find the minimum hot and cold utility your process actually needs, the pinch temperature, and how much heat you could recover by matching your own streams instead of buying utility.

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Process streams

Add each hot stream (needs cooling) and cold stream (needs heating). CP is the heat-capacity flowrate — mass flow × specific heat, in kW/°C.

StreamTypeSupply T (°C)Target T (°C)CP (kW/°C)Remove stream
Energy targets
Min hot utility
20kW
Min cold utility
60kW
Pinch temperature
90 / 80°C
Max heat recovery
450kW

Hot / cold pinch (shifted 85 °C).

Without vs with heat integration

UtilityNo integrationWith integrationSaving
Heating (kW)47020450
Cooling (kW)51060450
Total utility (kW)98080900

Heat integration can recover 450 kW — cutting total utility demand by about 92%.

Composite curves

Where the curves overlap horizontally is recoverable heat. The gap at the hot end is the hot utility; the gap at the cold end is the cold utility.

Composite curves. Hot composite from 30 to 170 °C, cold composite from 20 to 140 °C. The curves overlap over 450 kW of recoverable heat, with 20 kW of hot utility at the hot end and 60 kW of cold utility at the cold end.50100150-0100200300400500Net heat load (kW)Temperature (°C)
Hot compositeCold composite
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Results are indicative

Figures assume typical conditions and the stated method. For measured, guaranteed numbers on your plant, our engineers run site surveys, heat loss audits, and full process models.

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You are probably heating and cooling at the same time

Somewhere on your site a stream is being cooled while, a few metres away, another is being heated. Both cost money. The first needs a cooler, water and power; the second needs a burner and fuel. Put them together through an exchanger and both bills fall.

Pinch analysis is how you find out, before designing anything, exactly how much of that is available — and, just as usefully, how much is not.

What the targets are worth

Take the four-stream process this calculator opens with: a reactor feed and a recycle needing heat, a hot product and a flue quench needing cooling.

  • Served entirely by utilities: 470 kW of heating and 510 kW of cooling — 980 kW of utility in total.
  • Fully integrated at a 10 °C approach: 20 kW of heating and 60 kW of cooling.

That is 450 kW of recovered heat and a 92 % cut in utility demand, from rearranging what you already have. On 6,000 operating hours at 5 p/kWh of gas, the heating side alone is around £135,000 a year.

The number that matters is not the saving, though — it is that 20 kW is a floor. No exchanger network, however clever, beats it. If someone proposes a heat-recovery scheme that claims to get you below it, the proposal is wrong.

How the targets are found

The engine is the Problem Table Algorithm, the standard method.

  1. Every stream is shifted onto a common temperature scale — hot streams down by ΔTmin/2, cold streams up by the same — so that any hot and cold stream overlapping on the shifted scale is guaranteed a feasible ΔTmin in a real exchanger.
  2. The shifted temperatures cut the problem into intervals. In each, the net heat is (CPhotCPcold)×ΔT.
  3. Heat cascades down the intervals. Where the cascade goes negative it is asking heat to flow uphill, which it will not do, so the whole cascade is lifted by the most negative residual.

That lift is the minimum hot utility. What falls out of the bottom is the minimum cold utility. The interval where the lifted cascade touches zero is the pinch.

Why the pinch is the important answer

The pinch splits your process in two, and the split has three rules that decide whether a retrofit works:

  • Do not transfer heat across the pinch. Every kW moved across it adds a kW to both utility bills.
  • No cold utility above the pinch. Cooling above the pinch means you paid to heat something and then paid again to cool it.
  • No hot utility below the pinch. Heating below the pinch wastes recoverable heat that was already available.

Most disappointing heat-recovery projects break one of these three. The exchanger works exactly as designed, and the site's fuel bill barely moves, because the recovered heat was simply displacing heat that was free anyway.

ΔTmin is a capital decision, not a physical constant

ΔTmin is the smallest approach you allow in any exchanger, and it is the dial between energy and capital:

  • Small (5 °C) — more heat recovered, but area goes up sharply as the driving force shrinks, and fouling has less margin to eat into.
  • Large (20–30 °C) — cheap, compact exchangers, more utility bought forever.

Typical starting points are 10 °C for liquid–liquid duties, 20–30 °C where a gas is involved, and 3–5 °C in cryogenic service where utility is expensive enough to justify the area. Sweep the value in the calculator and watch the targets move — the shape of that curve is the real answer, and where it flattens is usually where the sensible design sits.

What this does not do

These are targets, and targets are the beginning of a heat-integration study, not its conclusion. The model assumes a constant heat-capacity flowrate per stream and steady state. It does not:

  • design the exchanger network, or tell you how many exchangers you need;
  • cost anything, or check that the pipework can physically be run;
  • handle phase change with a varying CP, streams that only run part of the year, start-up and shutdown, controllability, or the fact that two units may be fifty metres and a road apart;
  • know which of your streams are genuinely available for matching.

A target of 450 kW says the prize exists. Whether it is 450, 300 or 180 once layout, operability and capital are real is what the study answers — and a retrofit that ignores those is how heat-recovery projects get a bad name.

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Frequently asked questions

CP is the heat-capacity flowrate — mass flow multiplied by specific heat, in kW per °C. For a stream of 2 kg/s of water (cp ≈ 4.18 kJ/kg·K) it is about 8.4 kW/°C. It is the slope of the stream on a temperature–enthalpy plot: a stream with a high CP moves a lot of heat for a small temperature change. Use an average value over the stream's temperature range; if the specific heat varies a lot, split the stream into two entries.

Start at 10 °C for liquid–liquid duties, 20–30 °C where a gas is on one side, and 3–5 °C only in cryogenic service where utility is expensive enough to pay for the area. But do not treat it as a constant — sweep it and look at how the targets respond. It is an economic trade-off between exchanger area and utility bought forever, and the point where the curve flattens is usually where the sensible design sits.

No. A threshold problem needs only one kind of utility — heating or cooling, not both. It happens when your streams do not overlap enough in temperature for the cascade ever to close, which is common when you enter only hot streams or only cold ones. The utility target shown is still correct; there is simply no pinch temperature to report, because nothing is constraining the design at an intermediate temperature.

Rarely all of it. The target is thermodynamic — it assumes any hot stream can be matched with any cold stream. Real sites have plot layout, operability, start-up cases, control requirements and streams that are not running at the same time. A well-executed retrofit typically captures a good share of the target, and the gap between target and achievable is exactly what a heat-integration study quantifies. What the target does give you is a hard ceiling and a way to tell a good proposal from a bad one.

Because it costs you twice. Above the pinch the process is a net heat sink; below it, a net heat source. Move a kW of heat from above the pinch to below it and you have to replace it with a kW of hot utility above, and reject an extra kW of cold utility below. The exchanger looks like it is recovering heat, and the site's utility bill goes up. This is the single most common reason a heat-recovery project underdelivers.

No. The whole calculation runs in your browser — nothing about your streams is sent to a server.