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Filter Technology31 October 20266 read

Settling, Impaction, Interception, Diffusion — How Glass Microfibre Captures Aerosols

A coalescing element does not sieve. It captures droplets and particles through four physical mechanisms, each strongest in a different size range. Understanding them explains efficiency, pressure drop and correct sizing.

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Borosilicate glass microfibre coalescing element RF-C for compressed air and gas

Summary

Glass microfibre media consist of randomly laid, in-depth fibre layers. Aerosols are captured by four mechanisms: gravitational settling (about 20–50 µm at low velocity), inertial impaction (above about 1 µm), direct interception (about 0.3–1 µm, within half a particle diameter of a fibre) and diffusion through Brownian motion (below 0.3 µm). Together they cover the range from above 50 µm to below 0.01 µm.

Glass microfibre media are made of in-depth layers of fibres laid down in a random fashion. As aerosols move through the media, they are captured on the fibres. There is no single "hole size" doing the work — four separate physical mechanisms bring droplets and particles into contact with a fibre. Each one is strongest in a different particle-size range, and together they allow borosilicate glass microfibre to remove aerosols from above 50 µm to below 0.01 µm.

4
Capture mechanisms
> 50 µm
Largest droplets captured
< 0.01 µm
Smallest aerosols captured
@ 0.01 µm
Basis of all R+F grade ratings

1. Gravitational settling

When velocities inside the filter element are very low, larger aerosols — usually 20 to 50 µm in diameter — may fall out of the gas stream before reaching the media. If they do reach the media, they continue to fall as they pass through it. This vertical motion increases the likelihood that they bump into a fibre and are captured.

1. Gravitational settling
When velocities inside the filter element are very low, larger aerosols — usually 20 to 50 µm in diameter — may fall out of the gas stream before reaching the media.

2. Inertial impaction

Aerosols larger than about 1 µm develop enough momentum that they do not follow the gas around a fibre. The gas bends away; the droplet carries straight on and impacts the fibre. Impaction becomes more effective as particle size and gas velocity increase.

3. Direct interception

Particles in the range of roughly 0.3 to 1 µm follow the gas streamlines. Some of these streamlines pass very close to a fibre. If a particle comes within half its own diameter of a fibre, it touches it and is held — this is interception.


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4. Diffusion (Brownian motion)

Particles smaller than about 0.3 µm no longer behave like small droplets. Their mass is so small that they do not obey the conventional laws governing moving bodies; they are knocked around by gas molecules and travel in random directions. This Brownian motion makes contact with a fibre more likely — and the smaller the particle, the stronger the effect. Where diffusion and interception overlap, around 0.3 µm, lies the most penetrating particle size.

MechanismTypical size rangeGets stronger with
Gravitational settling≈ 20–50 µmLow velocity, large droplets
Inertial impaction> 1 µmHigher velocity, larger particles
Direct interception≈ 0.3–1 µmFine fibres, dense media
Diffusion< 0.3 µmSmaller particles, longer residence time
Key insight: Once a particle touches a fibre it is held by intermolecular (Van der Waals) forces, which are essentially independent of the particle material, humidity and temperature. Captured liquid aerosols then coalesce into larger drops that drain away — see why water forms droplets, not a film.

Why velocity matters for sizing

The size ranges above shift with gas velocity. As velocity increases, gravitational settling plays a smaller role for large droplets, which stay suspended, while impaction becomes stronger. Diffusion needs residence time, so very fine particles are captured less well at excessive media velocity. Higher velocity also raises differential pressure and can re-entrain coalesced liquid. This is why housings and elements are sized on the actual flow at operating pressure — not on a catalogue figure in Nm³/h. Our Engineering Sizing Tool does this conversion for you.

⚠ Important: Overloading a housing does not just shorten element life — it changes the physics of capture. If a filter shows carryover despite a high-efficiency element, check the actual flow first. Our solution page on liquid carryover in gas filters lists the typical causes.
Key Takeaway
  • When velocities inside the filter element are very low, larger aerosols — usually 20 to 50 µm in diameter — may fall out of the gas stream before reaching the media.
  • Aerosols larger than about 1 µm develop enough momentum that they do not follow the gas around a fibre.
  • Particles in the range of roughly 0.
  • Particles smaller than about 0.

From mechanism to product

All R+F coalescing and particulate elements use this borosilicate microfibre principle. The standard final coalescer RF-C-51230-HE is rated at 99.99 % @ 0.01 µm; the matching particulate element RF-P-51230-HE protects against dry particles. For the 51 × 230 and 51 × 476 sizes the outer diameter is 62.5 ± 1.5 mm for coalescing and 58 ± 1.5 mm for particulate elements; standard coalescing elements operate from −50 to +150 °C, within the limit of the housing.

Download the Technical Note "Why borosilicate glass microfibre?" (PDF) for a two-page summary, or find all datasheets in the download library.

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