Lesson A8 left a question hanging: what do you do with flash steam when there is no low-pressure user to give it to? The industrial answer is a machine with no motor, no rotor and no seals to speak of — a steam-jet thermocompressor, which uses a little high-pressure steam to drag low-pressure steam back up to a useful pressure. This deep-dive explains how it works, and then examines the one design choice that decides whether an installation keeps performing when the plant's load moves: the choice between a fixed nozzle and a variable (spindle-controlled) nozzle. It is a 300° lesson: we will name products, cite manufacturers' published literature, and state exactly what is proven and what is not.
How a steam jet compresses steam
Three phases, one thermodynamic cycle:
- Expansion. Motive steam enters a converging–diverging nozzle, reaches the speed of sound at the throat (the choked-flow physics from the leak-cost lesson — here put to work), and leaves the diverging section at several times the speed of sound. Pressure energy has become a supersonic jet.
- Entrainment. The jet's low-pressure wake draws in the suction steam — your flash — and drags it up to speed in the mixing section, transferring momentum kilogram by kilogram.
- Compression. The mixed stream decelerates through a diffuser; a train of shock waves converts velocity back into pressure, delivering the whole flow — motive plus suction — at the discharge pressure, ready for the header.
Two ratios describe every duty: the compression ratio K = Pd ÷ Ps (absolute), and the entrainment ratio — kilograms of suction steam carried per kilogram of motive. Every kilogram entrained is a kilogram the boiler does not raise.
The threshold that rules the machine: K ≈ 1.8
Above a compression ratio of about 1.8:1, the flow in the diffuser throat itself goes sonic and the machine operates in critical mode. This threshold is not a marketing figure — it is published, as the same number, by two independent ejector manufacturers (Croll Reynolds; Transvac). In critical mode the motive flow is locked by nozzle geometry and motive pressure — and most real recovery duties, such as lifting atmospheric flash into a 3.5 kg/cm²g header (K ≈ 4.5), are deeply critical.
Critical mode also has a cliff. The shock system standing in the diffuser can only hold so much back-pressure: push beyond it — or weaken the jet — and the shocks are expelled, entrainment collapses, and the unit breaks: suction pressure spikes and recovery stops. Worse, the recovery is not symmetric: ejector literature documents the hysteresis — after a break, conditions must be restored beyond the failure point before the machine picks up load again. On a running plant that means venting steam or operator intervention after every upset.
The fixed nozzle: a single-point machine
A fixed-nozzle thermocompressor is three stationary parts — nozzle, mixing section, diffuser — with no moving element at all. Its virtue is genuine: simplicity, low price, nothing to maintain. Its constraint follows from the choked-flow law: fixed throat + fixed motive pressure = fixed motive consumption. The makers state it themselves: Croll Reynolds — optimal efficiency "at a single set of suction, discharge and motive pressure conditions"; Schutte & Koerting — fixed-nozzle compressors are for "a steady load"; Spirax Sarco's technical information for its fixed-orifice SJT puts suitability at roughly ±10% around the design point.
Away from that point, the behaviour is documented in the same makers' literature:
- Falling load: the machine still swallows full motive steam whether or not there is flash to entrain — high-value steam spent on nothing, or the suction vessel pulled needlessly deep.
- Throttling the motive (the only external handle) destroys the very pressure energy the nozzle exists to convert; the jet weakens and the margin to the break point shrinks. Above the 1.8 threshold, Spirax's own document rules its motive-control options out entirely for sonic operation.
- Off-design pressure: Croll Reynolds' published figures for a 100 psig-design nozzle: 21.7% less steam at 75 psig — and +43.5% consumption at 150 psig. Boilers sag rather than surge, so a fixed unit spends much of its life on the weak side of its design point.
- The published workarounds concede the point: banks of parallel fixed units switched in steps (Transvac; S&K), or venting the surplus. A bank steps; a load moves.
None of this is a criticism of fixed-nozzle machines on genuinely steady duties. A continuous, single-product, flat-load process is exactly where the simpler machine is the better engineering — and an honest offer says so in writing.
The variable nozzle: making the restriction the control element
The variable-nozzle machine — supplied in India as the Jetomat, the Bälz 590 controllable-nozzle steam ejector, engineered and supported by i-Kcal as Bälz's Indian partner — puts a precision-tapered spindle inside the nozzle throat. An external actuator strokes the spindle; the throat area follows; the choked-flow law turns from a lock into a control handle:
- Kilograms change, energy per kilogram does not. The motive line stays at full pressure at every load; the spindle meters how many kilograms pass. Each kilogram still expands from full line pressure to full jet velocity — the jet gets smaller, not weaker.
- The shock system stays home. Closing the throat at low load keeps the nozzle-to-diffuser area ratio matched to the flow — precisely the condition that holds the machine inside its stable regime, where a throttled fixed unit drifts toward its break point.
- To the control system it is just a valve. Positioner, 4–20 mA setpoint, continuous modulation on discharge pressure, suction pressure or flow — no anti-break floor logic, no step transitions, no reset procedure after upsets.
Turndown: the number nobody publishes
Here the honest reporting matters. A survey of the steam-ejector industry's published literature (August 2026) finds no manufacturer publishing a motive-nozzle turndown figure. (A "100% to 0%" figure sometimes quoted is suction-side turndown — a different quantity.) What the i-Kcal delivered record documents — factory documents and running installations — is up to 10:1 motive turndown on a single DN80 body:
- a factory-measured cone-contour curve for one delivered DN80 machine, metering motive steam continuously from 26 to 3,010 kg/h across a 40 mm spindle stroke — 41 measured points at constant motive pressure;
- maker's selector verification of the same duty at both 300 and 3,000 kg/h motive on a DN80 at identical pressures, with healthy entrainment at both ends;
- delivered machines running today: a DN80 modulating 500–2,500 kg/h (5:1) on a plywood-press duty; a DN65 modulating 400–1,500 kg/h (3.75:1) on a corrugator line;
- third-party corroboration: a Gujarat agrochemical plant's public CII National Energy Award submission (2019) records that a fixed-nozzle thermocompressor could not be used for its intermittent flash duty, and reports 422 kg/h recovered with a variable-nozzle machine.
And the limit of the claim, stated plainly: these are selection and factory-test figures, not site measurements of turndown-in-service — which is why current projects build in motive and suction flow metering, so the recovery is proven in operation, not on paper.
One duty, across its load range
| Load | Fixed nozzle | Variable nozzle |
|---|---|---|
| 100% | Peak efficiency — this is the point it was bought for | Peak efficiency — spindle at design position. Parity. |
| 75% | Motive throttled; jet weakens; break-point margin shrinks | Spindle closes; full pressure kept; entrainment healthy on less steam |
| 50% | On high-lift duties, typically venting / bypassing / on-off to stay online | Continuous modulation; shock system held; recovery continues |
| ~10% | Effectively offline — full motive spent doing nothing, or bypassed | Still metering — the delivered DN80's factory curve reaches 26 kg/h |
Five questions to put to any thermocompressor offer
- 1. What is my duty's compression ratio, and is the unit sonic there? Pd ÷ Ps in absolute. Above ~1.8, a fixed nozzle's motive flow is locked.
- 2. If it is sonic, how exactly is capacity controlled when my load changes? Motive throttling is not an answer above the threshold — the makers' own literature says so. On/off, venting or a stepped bank are the honest fixed-nozzle answers; ask which is proposed and what it costs in steam.
- 3. What happens when my motive pressure sags below design? It will — busy plants sag. For a fixed orifice: less flow AND less energy per kilogram, sliding toward the break point. Ask for the compensation mechanism.
- 4. Show me the motive-side turndown curve of the actual machine. A factory-measured stroke-versus-flow curve — not a suction-side percentage. If none exists, the machine has one design point.
- 5. How will the promised recovery be verified after commissioning? Metering — motive and suction — reported against the sizing. Insist on it, from every vendor, including this one.
- A thermocompressor upgrades flash with motive steam: expansion → entrainment → recompression, no moving machinery in the flow path.
- K = Pd/Ps absolute. Above ≈1.8 (published: Croll Reynolds, Transvac) the machine is sonic: fixed motive flow, hard break point, hysteresis.
- Fixed nozzle = right for genuinely steady loads. Moving loads: it wastes motive, steps, vents, or drops out — per its own makers' literature.
- A spindle in the throat meters kilograms at full jet energy: delivered record up to 10:1 motive turndown on a single DN80 body.
- Selection is a statement about your load profile. Measure the load first; demand the factory curve; meter the result.
This lesson condenses an i-Kcal technical white paper that develops the physics, the manufacturers' published data and the delivered record in full, with references — available to customers on request via i-kcal.com. Published sources cited above: Croll Reynolds thermocompressor bulletin; Transvac thermocompressor pages; Schutte & Koerting Bulletin 4F and performance papers; Spirax Sarco TI for the fixed-orifice SJT; the 2019 CII National Energy Award submission of the plant concerned.
The ejector's family tree starts in 1858 with Henri Giffard — balloonist, engineer — who needed to feed water into a locomotive boiler against the boiler's own pressure without a pump. His "injector" used the boiler's steam to throw feedwater into the boiler that made the steam — a machine so counter-intuitive that engineers initially refused to believe it worked. It worked on every steam locomotive built for the next century, and its grandchildren are compressing steam in your plant today.