The MBR Book: Principles and Applications of Membrane
The MBR Book: Principles and Applications of Membrane
The MBR Book: Principles and Applications of Membrane
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50 <strong>The</strong> <strong>MBR</strong> <strong>Book</strong><br />
a-factor<br />
1<br />
0.8<br />
0.6<br />
0.4<br />
0.2<br />
0<br />
a � e�0.08788 MLSS<br />
(Krampe <strong>and</strong><br />
Krauth, 2003)<br />
a � 1.5074e�0.0446 MLSS<br />
(Muller et al., 1995)<br />
0 5 10 15 20 25 30 35 40<br />
MLSS (g/L)<br />
Figure 2.19 �-factor vs. MLSS concentration<br />
a � 4.3177e�0.2331 MLSS<br />
(Muller et al., 1995)<br />
a � e�0.083 MLSS<br />
(Gunder, 2001)<br />
In a number <strong>of</strong> studies <strong>of</strong> sewage treatment, an exponential relationship between<br />
�-factor <strong>and</strong> MLSS concentration has been observed. Muller et al. (1995), recorded<br />
�-factor values <strong>of</strong> 0.98, 0.5, 0.3 <strong>and</strong> 0.2 for MLSS concentrations <strong>of</strong> 3, 16, 26 <strong>and</strong><br />
39 g/L, respectively, yielding an exponential relationship with an exponent value <strong>of</strong><br />
�0.045 <strong>and</strong> an R 2 <strong>of</strong> 0.99 (Fig. 2.19). Günder (2001) <strong>and</strong> Krampe <strong>and</strong> Krauth<br />
(2003) observed the same exponential trend with exponent values <strong>of</strong> �0.083<br />
<strong>and</strong> �0.088, respectively, whereas an even higher exponent value <strong>of</strong> �0.23 was<br />
recorded by Germain (Germain, 2004). Studies on model or simplified systems by a<br />
number <strong>of</strong> authors (Freitas <strong>and</strong> Teixeira, 2001; Ozbek <strong>and</strong> Gayik, 2001; Verlaan <strong>and</strong><br />
Tramper, 1987) appear to indicate that the principal impact <strong>of</strong> solids concentration<br />
is on the interfacial area a, which decreases with increasing solids level whilst leaving<br />
the mass transfer coefficient k L largely unaffected. This has been attributed to the<br />
promotion <strong>of</strong> bubble coalescence by suspended solids (Klein et al., 2002), <strong>and</strong> the<br />
effect is also aeration rate-dependent (Freitas <strong>and</strong> Teixeira, 2001). Since <strong>MBR</strong>s run<br />
at a high MLSS the aeration dem<strong>and</strong> for biotreatment operation <strong>of</strong> an <strong>MBR</strong> is somewhat<br />
higher than that <strong>of</strong> an ASP.<br />
<strong>The</strong> impact <strong>of</strong> particle size is more complex than particle concentration, since aeration,<br />
mass transfer <strong>and</strong> particle size are interrelated. For fine particles, �0.01 mm,<br />
k La has been shown to increase with increasing solids concentration up to a certain<br />
level <strong>and</strong> remain stable, before decreasing with further increased solids concentration<br />
(Saba et al., 1987; Smith <strong>and</strong> Skidmore, 1990). With larger particles, 1–3 mm, k La<br />
appears to decrease with concentration (Hwang <strong>and</strong> Lu, 1997; Koide et al., 1992;<br />
Komaromy <strong>and</strong> Sisak, 1994; Lindert et al., 1992; Nakao et al., 1999). Experiments<br />
examining excess sludge production, in which the DO concentration was adjusted independently<br />
<strong>of</strong> aeration intensity, indicated that higher mixing intensity <strong>and</strong> DO concentration,<br />
created by raising the airflow, had almost the same impact on floc break-up <strong>and</strong><br />
therefore on particle size. At a sludge loading <strong>of</strong> 0.53 kg BOD 5/kg MLSS day, the excess<br />
sludge production was reduced by 22% by raising the oxygen concentration from 2 to<br />
6 mg/L (Abbassi et al., 1999). However, the principal impact <strong>of</strong> particle size in an <strong>MBR</strong><br />
is on filter cake permeability, as indicated by the Kozeny Carman equation.