Fouling accounts for 30–40 per cent of membrane operating cost, and cake-resistance models describe the symptom rather than the cause. The cause is adhesion between extracellular polymeric substances and the membrane surface — an interfacial problem, and one that predicts which cleaning chemistry will work.

EPS is defined by how you extract it

There is no single substance called EPS. The term covers whatever the extraction method releases, and the fractions behave quite differently in a membrane system.

FractionTypical extractionCompositionFouling role
Soluble microbial products (SMP)Centrifugation, then 0.45 µm filtrationProteins, polysaccharides, humics in solutionPore blocking; the irreversible component
Loosely bound EPSMild chemical or thermal releasePolysaccharide-rich, protein-poorCake layer bulk and its compressibility
Tightly bound EPSHeat extraction, ~80 °CProtein-rich, hydrophobic amino acidsAdhesion to the surface; biofilm initiation
The protein-to-polysaccharide ratio is the single most useful number. Below about 0.5 the foulant is polysaccharide-dominated and forms a bulky but weakly adhered cake. Above about 2.0 it is protein-dominated, adheres strongly through hydrophobic interaction, and resists hydraulic cleaning entirely.

Interaction energy: why DLVO is not enough

Classical DLVO theory adds van der Waals attraction to electrostatic double-layer repulsion. In water that is insufficient — it omits the polar interaction that dominates at short range in hydrogen-bonding media. The extended form adds a Lewis acid–base term:

Utotal = ULW + UEL + UABLW = Lifshitz–van der Waals (apolar); EL = electrostatic double layer; AB = Lewis acid–base (polar, hydrogen bonding)

Each surface is characterised by an apolar component and a pair of polar parameters, obtained from contact angle measurement with three probe liquids:

γ = γLW + 2√(γ+γ)γ+ = electron-acceptor parameter; γ = electron-donor parameter (mJ m−2)

Representative surface energies

MaterialγLWγ+γ
PVDF43.20.029.8
PES44.00.0511.2
Ceramic (Al2O3)35.61.245.0
PTFE19.80.10.5

Values in mJ m−2. Note the electron-donor column: the ceramic is an order of magnitude more electron-donating than the polymers, and that single difference drives the result below.

Free energy of adhesion predicts irreversible fouling

The free energy of adhesion between foulant and membrane, mediated by water, is the sum of the apolar and polar contributions evaluated for the three-phase system:

ΔGadh = γfm − γfw − γmwf = foulant, m = membrane, w = water. Negative means adhesion is spontaneous.

Evaluating this for tightly bound EPS at 25 °C gives the practically important contrast:

MembraneΔGadh with TB-EPSInterpretation
PVDF≈ −8.4 mJ m−2Spontaneous adhesion; irreversible fouling expected
Ceramic Al2O3≈ +2.1 mJ m−2Net repulsive; fouling largely hydraulically reversible
This is the thermodynamic explanation for ceramic membranes’ fouling resistance. It is not that ceramics are smoother or stronger. It is that a strongly electron-donating surface holds a bound water layer that protein must displace before it can attach, and displacing it costs more energy than adhesion returns.

Critical flux follows from adhesion energy

Critical flux is the flux below which no appreciable fouling occurs. It is not an arbitrary operating rule — it is the point at which the hydrodynamic drag carrying a particle to the membrane balances the interfacial force resisting attachment. For unmodified PVDF against protein-rich tightly bound EPS, that balance lands at roughly 18 L m−2 h−1, which is consistent with operating experience on municipal MBRs.

Hydrophilic surface modification — PEGylation, plasma treatment, blended hydrophilic additives — raises the membrane electron-donor parameter, makes ΔGadh less negative, and lifts critical flux to the 25–30 LMH range. That is the mechanism behind every “low-fouling” membrane claim; ask suppliers for contact-angle data, not just flux curves.

Operating below critical flux is cheaper than cleaning above it. The energy penalty of extra membrane area is linear; the cost of irreversible fouling is not.

Flux, TMP and aeration trade-offs are covered in membrane bioreactor design and ultrafiltration system design.

Matching the cleaning chemistry to the foulant

Blanket hypochlorite cleaning is the commonest error in MBR operation. Hypochlorite attacks protein; it does little to a polysaccharide cake, and it oxidises the membrane polymer while failing to solve the problem.

Dominant mechanismEPS fractionAgentMode of actionTypical conditions
Pore blockingSMP, proteinsSodium hypochloriteOxidative cleavage of protein structure500–2,000 mg/L, ambient, 2–4 h
Cake layerLoosely bound, polysaccharideCausticSaponification and solubilisation0.5–1.0% w/v, ~35 °C, 4–6 h
Adhesive biofilmTightly bound, protein and lipidCitric acid plus surfactantChelation of bridging Ca2+ and Mg2+~2% citric, ~40 °C, 6–8 h

Characterise before you specify

Four measurements on a fouled coupon settle the protocol:

  • Contact angle goniometry with three probe liquids — gives the surface energy components and hence ΔGadh.
  • FTIR — the protein amide I band near 1,650 cm−1 against the polysaccharide C–O band near 1,030 cm−1.
  • XPS — surface N/C ratio indicates protein; O/C indicates polysaccharide.
  • AFM force spectroscopy — direct measurement of adhesion force, if the interfacial calculation is being challenged.
Decision rule. High surface nitrogen with strongly negative adhesion energy points to the chelation and surfactant route. Oxygen-rich foulant with cake-dominated resistance points to caustic. Pore blocking with a fast TMP rise and little cake points to oxidative cleaning — and only then is hypochlorite the right answer.

Design rules

  • Measure the protein-to-polysaccharide ratio before selecting a membrane material or a cleaning regime. It predicts fouling propensity better than MLSS, SRT or flux alone.
  • Specify hydrophilic or ceramic surfaces where the mixed liquor is protein-rich. The adhesion energy, not the pore size, governs the irreversible fraction.
  • Set operating flux below critical flux rather than designing to a supplier’s peak. Roughly 18 LMH for unmodified PVDF, 25–30 LMH for hydrophilically modified.
  • Match CIP chemistry to the dominant fraction. Hypochlorite on a polysaccharide cake wastes reagent and consumes membrane life.
  • Re-characterise after any process change — a shift in SRT, load or industrial input moves the PN/PS ratio, and the CIP protocol should move with it.

Frequently asked questions

Why do ceramic membranes foul less than polymeric ones?

Because their surfaces are strongly electron-donating, which makes the free energy of adhesion with protein-rich EPS slightly positive rather than negative. Attachment is not spontaneous, so most of the fouling stays hydraulically reversible. It is an interfacial property, not a matter of smoothness or strength.

Is hypochlorite always the right cleaning agent for an MBR?

No, and defaulting to it is the commonest operating error. It attacks protein but does little to a polysaccharide cake, while still oxidising the membrane polymer. Identify the dominant fraction by FTIR or XPS first — caustic for cake, chelant plus surfactant for adhered biofilm, hypochlorite for pore blocking.

What is a realistic critical flux for a municipal MBR?

Around 18 LMH for unmodified PVDF against protein-rich mixed liquor, rising to 25–30 LMH for hydrophilically modified surfaces. Treat supplier peak-flux figures as a ceiling that assumes favourable feed, not as a design point.

Can I predict fouling from MLSS alone?

Poorly. MLSS sets cake thickness but not adhesion. Two plants at identical MLSS can differ several-fold in irreversible fouling if one runs protein-dominated EPS and the other polysaccharide-dominated. The PN/PS ratio is the more informative measurement.

Sources & further reading