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Diffusion Pump
Emma

Created by

Emma

26. August 2026SE
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Diffusion Pump

A rotary vane pump stops improving at the vapour pressure of its own oil, and no amount of running gets it lower. Wolfgang Gaede's diffusion pump of 1915 goes far below that by abandoning mechanical pumping entirely. Oil is boiled at the bottom, its vapour rushes up a central chimney and out through angled nozzles as a high-speed downward jet. Gas molecules wandering into that jet are struck and knocked downward, carried to the bottom where a backing pump removes them, while the vapour condenses on the cooled walls and runs back to the boiler. There are no moving parts whatsoever — the only thing moving is vapour — and it reaches pressures a million times lower than the pump backing it.
Advanced
5 hours 30 minutes

Instructions

1

Understand why it cannot work alone

A diffusion pump discharges into a pressure, not into the atmosphere. Get this wrong and nothing works.

  1. Connect a rotary vane pump to the diffusion pump's outlet — this is the backing pump.
  2. Note that the diffusion pump must never be started until the backing pump has pulled the system down.
  3. Establish the rough vacuum FIRST, then apply heat to the boiler.
  4. On shutdown, reverse: cool the boiler completely before stopping the backing pump.

The vapour jet has almost no compression ability. It can move molecules from a very low pressure to a moderately low one, but it cannot push against atmosphere — the jet simply collapses. So the two pumps are not alternatives, they are a series: the rough pump handles atmosphere down to a fraction of a millibar, and the diffusion pump takes it from there. Starting the boiler at atmospheric pressure oxidises the oil and ruins it.

This staged architecture is universal in vacuum work. Every high-vacuum system in this batch, including the turbomolecular pump, needs a backing pump beneath it for exactly this reason.

Materials for this step:

Boiled Linseed OilBoiled Linseed Oil1 bottle
Glass Tubing KitGlass Tubing Kit1 kit

Tools needed:

Digital Caliper 6-InchDigital Caliper 6-Inch
StopwatchStopwatch
2

Build the boiler, chimney and nozzle stack

Vapour must be forced out sideways and DOWNWARD, never upward toward the vessel.

  1. Make a body from a wide steel or glass tube, closed at the bottom as an oil boiler.
  2. Fit a central chimney rising from the boiler.
  3. Cap it with two or three umbrella-shaped nozzles at different heights, each directing vapour outward and DOWN at a steep angle.
  4. Leave an annular gap between each nozzle and the wall.
  5. Fit a heater under the boiler and a cooling jacket or fins around the outside.

The downward angle is the entire mechanism. A molecule entering the jet receives momentum in the jet's direction, so the jet must point toward the backing pump. Angle a nozzle upward and it drives gas back into the vessel, which is worse than no pump at all. Multiple stages exist because each one can only compress by a limited ratio.

The cooling jacket is not optional. Vapour must condense on the walls and drain back to the boiler; if the walls are warm the vapour escapes into the vessel instead, which is the backstreaming problem in step 4.

Materials for this step:

Aluminum Round BarAluminum Round Bar1 piece
Aluminium Plate (10mm)Aluminium Plate (10mm)1 piece
Copper Round BarCopper Round Bar1 piece

Tools needed:

Cordless Drill/Driver (20V)Cordless Drill/Driver (20V)
Drill Bit SetDrill Bit Set
File SetFile Set
Hacksaw Frame with Blades (10-Pack)Hacksaw Frame with Blades (10-Pack)
Digital Caliper 6-InchDigital Caliper 6-Inch
Bench ViseBench Vise
3

Start it in the right order and watch the pressure fall

Sequence matters more than in any other pump in this batch.

  1. Run the backing pump until the Pirani gauge shows the rough vacuum is established.
  2. Only then switch on the boiler heater.
  3. Watch the Pirani reading and note when it goes off the bottom of its range.
  4. Record the time from heater-on to that point.
  5. Shut down in reverse order and note what happens if you stop the backing pump first.
The Pirani gauge from the previous blueprint saturates at its low end — which is the direct demonstration that you have entered a pressure region it cannot see. That is the moment you need the ionisation gauge later in this batch. Each instrument's blind spot is the next instrument's reason for existing.

Tools needed:

Digital Multimeter (Lab Grade)Digital Multimeter (Lab Grade)
StopwatchStopwatch
Digital Caliper 6-InchDigital Caliper 6-Inch
4

Find the backstreaming, and trap it

The pump's working fluid is also its main contaminant.

  1. Run the pump for an hour with a clean glass slide mounted above the inlet.
  2. Examine the slide for an oil film.
  3. Now fit a cold trap or a chevron baffle between the pump and the vessel.
  4. Repeat with a fresh slide and compare.
Some oil vapour always escapes upward against the jet — that is backstreaming, and in a vacuum system it contaminates everything: optical surfaces, semiconductor wafers, experimental samples. A cold trap condenses it before it arrives, and a chevron baffle gives it no straight-line path. Both cost pumping speed, which is the standard trade: cleanliness against throughput.

Materials for this step:

Acrylic SheetAcrylic Sheet1 sheet
Aluminum Flat Bar (1x1/4 inch, 36-inch)Aluminum Flat Bar (1x1/4 inch, 36-inch)1 piece

Tools needed:

Digital Caliper 6-InchDigital Caliper 6-Inch
StopwatchStopwatch
File SetFile Set
5

Pumping with vapour, and history

Wolfgang Gaede invented the diffusion pump in 1915, using mercury vapour; Irving Langmuir improved it at General Electric shortly after, and later designs replaced mercury with low-vapour-pressure oils, removing the toxicity while keeping the principle. Gaede is the central figure of this whole batch — he also produced the rotary and molecular pumps that bracket this one.

What it made possible. High vacuum on demand, cheaply and continuously, is the precondition for the vacuum tube industry, for X-ray tubes, for electron microscopy, for thin-film coating and eventually for semiconductor manufacture. The Coolidge X-ray tube and the Fleming valve in this catalogue both depend on vacuums this pump can reach and the Sprengel pump could only approach after hours of work.

The mechanism is worth stating plainly: at these pressures molecules rarely collide with each other, so you cannot push gas the way you push a fluid. Instead you hit individual molecules and give them momentum in the direction you want. Every high-vacuum pump does some version of this — the diffusion pump hits them with vapour, the turbomolecular pump at the end of this batch hits them with solid blades.

Its honest limits: backstreaming, the need for a backing pump, warm-up and cool-down times measured in tens of minutes, and a catastrophic failure mode — lose cooling water or admit air while hot and the oil oxidises and coats the entire system. Turbomolecular pumps displaced it in clean applications for exactly these reasons, while diffusion pumps remain common where robustness and low cost matter more than cleanliness.

Materials

7

Tools Required

8

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