Cold start, gear house

Picture a cold start in a gear house. A creamy band fills the top of the sight glass, and someone asks for a can of antifoam. Two hours later, the band has gone. The glass looks clear. The pump gauge is still twitching.

Last week's particle count has jumped two codes, and the breather has been weeping a thin film down the tank all week. Nobody has asked where the air gets in, or whether the oil has changed. Those are two different questions, and the sight glass answers neither. The antifoam can wait until both have been asked.

Air is in that oil three ways. Dissolved, it is invisible, though a mineral hydraulic fluid can hold up to 9 percent by volume of it at atmospheric pressure. Entrained, it is fine bubbles, cloudy when there are enough of them. Foam is the fraction that reached the surface and stayed.

Foam is only the air you can see. The pump, the bearings and the particle counter deal with the air you cannot.

Before the antifoam

Four things to settle before anyone opens the can

  • Hold

    No antifoam, and no top-up against a foaming glass.

  • Time

    Watch the foam and the haze separately as the oil stands.

  • Walk

    Find where air gets in.

  • Test

    Ask the laboratory whether the oil has changed.

In this article

Why the fine bubbles stay

Whether a bubble reaches the surface before the oil reaches the suction depends on how fast it rises and how long it has. For a fine bubble, rise speed goes with the square of its diameter and inversely with the oil's viscosity. Halve the diameter and it rises four times slower; cool the oil and it slows again.

A typical ISO VG 320 gear oil sheet lists 320 mm²/s at 40 °C and 25 at 100 °C. The ASTM D341 viscosity and temperature relation carries that to near 1,300 mm²/s at 20 °C and near 110 at 60 °C.

Treat the bubble as a rigid sphere, and the arithmetic is short: a 0.5 mm bubble climbs about 30 mm in five minutes at 20 °C, and about 370 mm at 60 °C.

The same arithmetic explains the morning. Oil tends to foam when it is cold, and cold oil holds its fine air longest. As the tank warms, the large bubbles leave, the surface layer collapses and the glass clears. The fine fraction lingers, and while the machine runs, every pass through the gears, pump and return line can make more.

Five minutes in the tank

Now give it the time a tank gives it. A 200 litre console tank circulating 40 litres a minute turns over every five minutes, and at 40 °C a 0.2 mm bubble in the gear oil needs more than an hour to rise 300 mm from return to suction.

So it goes round again, and the air release standard spells out what that can do: oil pressure that cannot be held and incomplete films in bearings and gears. That is the twitching needle.

A tank pass is not long enough for every bubble

Large bubbles rise quickly. Fine bubbles can return to the pump before they reach the surface.

How long one bubble needs to rise 300 mmLog-log chart of the time a single bubble needs to rise 300 mm against its diameter, from 0.05 to 1 mm, for ISO VG 320 gear oil and ISO VG 46 hydraulic oil at 20 and 60 degrees. All four lines fall steeply as the bubble grows, and VG 320 at 60 degrees and VG 46 at 20 degrees fall almost on one line. A five-minute line marks one tank pass and a ten-minute line the end of a standstill before a level reading. In one pass only bubbles above about 0.45 mm clear in warm gear oil, and above about 0.19 mm in warm hydraulic oil; in cold gear oil even a 1 mm bubble needs about 12 minutes.0.050.10.20.5110 s1 min10 min1 h10 h100 hBubble diameter, mmTime to rise 300 mm0.19 mm clears in one pass0.45 and0.48 mmVG 320, 20 °C10 min: level reading5 min: one tank passVG 320 at 60 °C andVG 46 at 20 °C:nearly the same lineVG 46, 60 °C How long one bubble needs to rise 300 mmLog-log chart of the time a single bubble needs to rise 300 mm against its diameter, from 0.05 to 1 mm, for ISO VG 320 gear oil and ISO VG 46 hydraulic oil at 20 and 60 degrees, with VG 320 at 60 degrees and VG 46 at 20 degrees almost on one line. A five-minute line marks one tank pass: only bubbles above about 0.45 mm clear it in warm gear oil, and above about 0.19 mm in warm hydraulic oil; in cold gear oil even a 1 mm bubble needs about 12 minutes.0.050.10.20.5110 s1 min10 min1 h10 h100 hBubble diameter, mmTime to rise 300 mm5 min0.19 mmVG 320, 20 °CVG 46 at 20 °CVG 320 at 60 °CVG 46, 60 °C

Sources: Q8 Goya 320 and Q8 Henry 46 data sheets (typical values); ASTM D341.

Figure 1. Cold, heavy oil holds a 0.1 mm bubble for most of a day; warm, light oil lets it go in minutes, and a five-minute tank pass only ever clears the large ones.
about 1 mm
how far a 0.1 mm bubble climbs in five minutes in ISO VG 320 gear oil at 20 °C
about 15 mm
the same bubble in the same oil at 60 °C

One five-minute pass clears nothing much under half a millimetre, even from warm gear oil. A typical ISO VG 46 hydraulic oil does no better at 20 °C, and at 60 °C it still keeps everything under about 0.2 mm.

Where the air gets in

Usually it is the machine. Air typically enters a hydraulic circuit through the suction line when seals and fittings are not tight. The suction side runs below atmospheric pressure, so a loose joint there pulls air in without letting oil out; it stays dry and nobody sees it.

Returns and drains that end above the oil beat air in with every litre. One pump maker's reservoir guidance asks for drain and bleed lines ending at about half the fluid level, the suction inlet at least eight pipe diameters below the surface, and baffles that give the bubbles time to rise.

Trace the air back to its entry point

A dry suction joint can still draw air in. A return above the oil can beat air into it.

Where the air is, and where it gets inSection through a lube oil tank. On the left a return pipe discharges above the oil, with a foam band on the surface and a field of fine bubbles below it; a drain line ends at half depth; a baffle divides the tank; on the right the suction pipe draws from near the floor and leaves through a flanged joint. Gold marks show where air gets in: the return falling through the vapour space and a loose suction joint; a high level pushes foam out of the breather, with the sight glass full to the top.dat least 8 dbelow the level2 d abovethe floorbreatherreturn,above the oildrain and bleed,half depthloose suction joint:air in, no oil outfoamentrained airbaffledissolved air(invisible)suction inletoil pathsight glass,full to the top Where the air is, and where it gets inSection through a lube oil tank: a return pipe discharges above the oil on the left with foam on the surface and fine bubbles below; a sight glass outside the left wall shows the foam band at the oil level; a baffle divides the tank; the suction pipe on the right draws from near the floor and leaves through a flanged joint. Gold marks show air entering with the falling return and air drawn in at a loose suction joint; an arrow at the breather shows foam leaving it.breatherreturnloose joint:air in, no oil outfoamentrained airsight glassbaffledissolved air(invisible)
Figure 2. Air entering on the return side has to rise before the oil is drawn again; the fine bubbles do not, and the sight glass shows only the layer that did.

Level and cold starts decide where the foam goes. A sump filled to the top of the glass leaves the foam nowhere to go but the breather. One gear maker's fault table files oil at the breather under frequent cold starts or a high oil level, and the remedy it lists is mechanical: an expansion tank.

The oil can change too. In Flender's trend table, cloudy oil points to water or other foreign fluids, and a falling silicon value to an anti-foaming additive used up. The same manual forbids mixing oil types or makers. Each is a question for the laboratory.

Air corrupts two readings you already trust

The level. Flender's manual allows it to be read only at standstill, with the oil foam-free, after 5 to 10 minutes shut down. The rule is not fussiness: a foaming glass gives a false level, and a top-up made against it can overfill the sump, which feeds the breather and the foam in turn.

The particle count. The same manual has the laboratory thin the sample so that no air bubbles are counted. A light-extinction counter registers whatever blocks its beam, and the counting method, ISO 11500, is written for single-phase liquids; a bubble is a second phase. Before a jumped cleanliness code sends a filter cart out, ask whether that sample was degassed.

At the next stop, with a stopwatch

At the next planned stop, with the machine isolated under the site procedure, collect five things.

  • The sample, taken running before the stop or within the manual's window after it, with the new-oil reference, noting that the oil was aerated.
  • Oil temperature at the stop.
  • Foam band height and the haze below it at the stop, then at 1, 5 and 10 minutes.
  • Standstill level at 10 minutes, logged with the temperature.
  • Every return and drain against that level, the baffle, the suction depth and any disturbed suction joint.

Foam that collapses within minutes while the haze stays tells you the fine fraction is large. Trust the level only against the mark and the last standstill reading. A level taken while running carries the air and, on a circulating system, misses the oil still out in the lines.

Two tests, two questions

Foam and air release are separate properties, and a good result on one says nothing about the other. ASTM D892 blows air through the oil at 24 °C and 93.5 °C and rates the foam it builds and the foam left after settling. ASTM D3427 times how long entrained air takes to fall to 0.2 percent by volume.

Two tests answer different questions

One measures foam at the surface. The other times how quickly air leaves the oil.

Two tests, two questionsTwo apparatus drawings at one scale. Left, a graduated cylinder for the ASTM D892 foam test, with air blown through a diffuser at the bottom and a foam head above the oil whose height is dimensioned. Right, the ASTM D3427 air release vessel drawn twice, first with fine air dispersed through the oil and then with the air down to 0.2 percent by volume, with the air release time dimensioned between the two.Foam, ASTM D892 (ISO 6247)Air release, ASTM D3427 (ISO 9120)air infoam after blowingfoam left after settlingair dispersed0.2 percent airby volumeair release time Two tests, two questionsTwo apparatus drawings, one above the other. Top, a graduated cylinder for the ASTM D892 foam test, with air blown through a diffuser at the bottom and a foam head above the oil whose height is dimensioned. Below, the ASTM D3427 air release vessel drawn twice side by side, first with fine air dispersed through the oil and then with the air down to 0.2 percent by volume, with the air release time dimensioned between the two.Foam, ASTM D892air infoam after blowingfoam leftafter settlingAir release, ASTM D3427air dispersed0.2 percent airby volumeair release time
Figure 3. The foam test reads the volume of foam above the oil; the air release test reads the time the fine air takes to clear from within it.

Some data sheets carry only one: the gear oil sheet above lists foam figures and no air release line at all. The air release method may not rank oils where residence times are short and gas contents high, so read both results as a change against the new-oil reference, not as a pass mark.

Ask for both, with the test temperature on the report, plus viscosity at 40 °C against the nominal grade, water by Karl Fischer and the element trend, silicon included.

Air path or changed oil

What you seeWhat it may meanNext step
Foam gone in minutes, haze staysA large fine fractionWalk the tank; compare air release with the reference
Haze after hours of warm standstillWater or another fluid, not only airWater by Karl Fischer
Standstill level above the markWater or another liquid, or a top-up against foamLast standstill reading; water test
Oil at the breather after cold startsA high level, or cold foamLevel at standstill; an expansion tank
Particle count up on an aerated sampleBubbles counted as particlesAsk whether it was degassed; resample
Foam or air release off the referenceWater, a mixed product or a depleted additiveFind the cause; the oil's maker decides usability

If foam and air release match the new-oil reference, the oil's air handling has not changed, and the air path you found on the walk is the job.

The creamy band was the easy part. The air that never reached the surface is what the pump has been running on since the cold start, and a stopwatch at the next shutdown will tell you more about it than another can of additive.

Primary references

  1. Flender GmbH, Assembly and operating instructions 7300en: Gear unit lubrication and gear unit preservation, version 07/2026, pp. 21, 23, 47 to 48, 50, 52 and 54.
  2. SEW-EURODRIVE, X..e series helical and bevel-helical gear units: Possible malfunctions/remedy, edition 04/2026.
  3. HAWE Hydraulik, B 7960, Operation instructions for axial piston variable displacement pumps type V30D, January 2001, pp. 2 to 3.
  4. Danfoss Power Solutions, Technical Information 520L0463, Hydraulic Fluids and Lubricants, July 2016, p. 10.
  5. ASTM International, D892-25, Standard Test Method for Foaming Characteristics of Lubricating Oils, scope and significance.
  6. ASTM International, D3427-26, Standard Test Method for Air Release Properties of Hydrocarbon Based Oils, scope and significance.
  7. ASTM International, D341-20(2025), Standard Practice for Viscosity-Temperature Equations and Charts for Liquid Petroleum or Hydrocarbon Products, scope.
  8. ISO, ISO 6247:1998, Petroleum products: Determination of foaming characteristics of lubricating oils.
  9. ISO, ISO 9120:1997, Petroleum and related products: Determination of air-release properties of steam turbine and other oils, Impinger method.
  10. ISO, ISO 11500:2022, Hydraulic fluid power: Determination of the particulate contamination level of a liquid sample by automatic particle counting using the light-extinction principle.
  11. Q8Oils, Q8 Goya 320 product data sheet, typical values.
  12. Q8Oils, Q8 Henry 46 product data sheet, typical values.
  13. NPTEL, Viscous Incompressible Flows, lecture 27: Low Reynolds number flow around a sphere.
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