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The MBR Book: Principles and Applications of Membrane

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

constant pressure to constant volume <strong>and</strong> takes a value <strong>of</strong> 1.4 for air, T K,1 is the inlet<br />

temperature (K), <strong>and</strong> Q A is the volumetric flow rate <strong>of</strong> air. <strong>The</strong> blower efficiency (�)<br />

varies significantly according to the type <strong>of</strong> blower <strong>and</strong> its mechanical design, the rotational<br />

speed, <strong>and</strong> the blower rating for the task. As with pumping operations more<br />

accurate data can be found from manufacturers’ data sheets. If Equation (3.15) is<br />

divided by the total membrane module area A m to which the flow rate Q A applies,<br />

then one obtains an expression in kW/m 2 for power per unit membrane area:<br />

W<br />

(3.15b)<br />

where k is therefore a function <strong>of</strong> pressure, <strong>and</strong> thus the hydrostatic head �P h determined<br />

by the depth at which the aerator is placed in the tank, as well as temperature.<br />

If Equation (3.15) is divided by the permeate flow rate Q P, that is J netA m, where J net is the<br />

net flux (m 3 /(m 2 h)), then one obtains an expression for specific energy dem<strong>and</strong> in<br />

kWh/m 3 :<br />

W<br />

b,m<br />

b,V<br />

⎡<br />

PA,1 Tk,1l ⎢⎛<br />

P<br />

�<br />

⎢ ⎜<br />

2.73 �105 jl ( �1)<br />

⎢⎜<br />

⎝⎜<br />

⎢<br />

P<br />

⎣<br />

kQ<br />

�<br />

JA<br />

A<br />

m<br />

(3.16)<br />

Hence, whilst the hydrostatic head wholly or partly determines the flux, depending<br />

on whether suction is applied, its main contribution to energy dem<strong>and</strong> does not<br />

relate to membrane permeation directly but to its impact on aeration energy. If the<br />

flux <strong>and</strong> flow are normalised to 20°C <strong>and</strong> 101.3 kPa (i.e.J� net <strong>and</strong> Q� A respectively),<br />

then k in Equation (3.15b) simplifies to:<br />

⎡<br />

108.748l<br />

⎢⎛<br />

P ⎞<br />

A,2<br />

k � ⎢ ⎜<br />

jl ( � 1) ⎢⎝⎜<br />

101.325⎠⎟<br />

⎣⎢<br />

1� 1<br />

l<br />

(3.17)<br />

As already stated in most hollow fibre (HF) <strong>MBR</strong> technologies the membrane aeration<br />

is carried out separately from the bioreactor aeration <strong>and</strong> does not necessarily<br />

employ the same type <strong>of</strong> aerator. Some <strong>of</strong> the oxygen transfer is achieved by the<br />

membrane aeration, <strong>and</strong> the extent to which this occurs depends mainly on the type<br />

<strong>of</strong> membrane aerator employed.<br />

3.1.4 Design calculation: summary<br />

A,2<br />

A,1<br />

⎞<br />

⎠⎟<br />

⎤<br />

⎥<br />

� 1 ⎥<br />

⎦⎥<br />

1 1 �<br />

l<br />

⎤<br />

⎥ Q<br />

⎥ A kQ<br />

�1� ⎥<br />

Am<br />

A<br />

⎦<br />

Inter-relationships within an <strong>MBR</strong> process are complex (Fig. 2.26), but the most crucial<br />

relationships with respect to operating costs are those associated with aeration<br />

since this provides the largest component <strong>of</strong> the process operating cost. <strong>The</strong> impacts <strong>of</strong><br />

aeration on the various operating parameters have already been discussed <strong>and</strong> depicted<br />

in Fig. 2.18, <strong>and</strong> biological <strong>and</strong> physical parameters used for the determination<br />

<strong>of</strong> operating costs are listed in Tables 3.2 <strong>and</strong> 3.3 respectively. Note that it is most<br />

consistent to normalise against permeate product volume to produce specific energy<br />

A<br />

m

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