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The MBR Book: Principles and Applications of Membrane

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124 <strong>The</strong> <strong>MBR</strong> <strong>Book</strong><br />

3.1 <strong>Membrane</strong> bioreactor system operational parameters<br />

<strong>The</strong>re are essentially three main elements <strong>of</strong> a membrane bioreactor (<strong>MBR</strong>) contributing<br />

to operating costs, ignoring membrane replacement. <strong>The</strong>se are:<br />

1. liquid pumping<br />

2. membrane maintenance<br />

3. aeration<br />

Of these by far the most significant, especially for immersed technologies, is aeration.<br />

As already discussed in Chapter 2, aeration is used both for scouring an immersed<br />

membrane <strong>and</strong> for suspending <strong>and</strong> maintaining a viable biomass. Design <strong>of</strong> an <strong>MBR</strong><br />

therefore dem<strong>and</strong>s knowledge both <strong>of</strong> the feedwater quality, which principally determines<br />

the oxygen dem<strong>and</strong> for biotreatment, <strong>and</strong> the aeration dem<strong>and</strong> for fouling<br />

control, which relates to a number system characteristics as summarised in Fig. 2.18.<br />

<strong>The</strong> various governing principles have been discussed in Chapter 2. Design equations<br />

are summarised below.<br />

3.1.1 Liquid pumping<br />

<strong>The</strong> key hydraulic operating parameters for <strong>MBR</strong> operation are obviously flux J litres<br />

per m 2 per hour (LMH) <strong>and</strong> transmembrane pressure (TMP) �P m (bar or Pa), from<br />

which the permeability K (J/�P m in LMH/bar), kg/(m 2 s) is obtained. In sidestream<br />

<strong>MBR</strong>s the specific energy dem<strong>and</strong> (the energy dem<strong>and</strong>ed per unit permeate product<br />

volume) for continuous membrane permeation relates primarily to the pressure <strong>and</strong><br />

conversion, <strong>and</strong> is roughly given by:<br />

WhP � � �<br />

1<br />

rj ∑<br />

(3.1)<br />

where � is the density (kg/m 3 ), Θ is the conversion achieved by a single passage <strong>of</strong><br />

fluid along the length <strong>of</strong> the module (nominally 100% for submerged systems) <strong>and</strong><br />

� is the pumping energy efficiency. In the above equation ��P refers to the sum <strong>of</strong> all<br />

individual pressure losses which, for a sidestream system, comprises �P m <strong>and</strong> the<br />

pressure losses in the retentate channels, �P r, all pressure values being in SI units.<br />

As explained in Section 2.3.1, maximising Θ to reduce W h relies on increasing the<br />

total length <strong>of</strong> the flow path through the membrane channel <strong>and</strong> increasing the<br />

shear rate, but this has the effect <strong>of</strong> increasing �P r. <strong>The</strong> optimum operating conditions<br />

for a given channel dimension (tube diameter or parallel flow channel separation) is<br />

therefore determined by relatively straight-forward hydraulic considerations, perhaps<br />

complicated slightly by the non-Newtonian nature <strong>of</strong> the sludge (Section 2.2.5.3).<br />

For submerged <strong>MBR</strong>s, the total pressure loss is <strong>of</strong> lesser importance, since it is necessarily<br />

very low to sustain operation. In this configuration the pressure loss, principally<br />

the TMP, reflects state <strong>of</strong> membrane fouling, through K, but contributes very<br />

little to the energy dem<strong>and</strong>. Instead, the specific aeration energy dem<strong>and</strong> is mainly<br />

governed by the aeration intensity (Section 3.1.3.2).

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