In this chapter empirical models describing the specific death rate due to sparging as a
function of reactor parameters are first discussed. Next, current knowledge on the
mechanism of cell death due to sparging is reviewed. For this it is necessary to have
knowledge of the mechanical properties of animal cells and the interaction of cells with
air bubbles, which are therefore discussed first. With this knowledge in mind, the
possible mechanisms of cell death are reviewed for different regions in the reactor; the
Table 15.1 Static surface tension σ0, dynamic
surface tension σd, surface viscosity
μ
s, and surface
dilatational viscosity ks of media with different
additives
Medium Cone
(%)
σo mN.
m−^1
σd
mN.m−^1
μs 10 –4
N.m−^2
ks 10 –4
N.m−^2
Ref.
HBBS 72.8 Chattopadhyay
1995b
RPMI 70 0.25 Dey 1997
TNM-FH 47.3 69.4 Chattopadhyay
1995b
SFM-L 64 Chattopadhyay
1995b
Serum free 61 70.8 5.1 0.46 Michaels 1995b
0.5 70.8 Michaels 1995b
0.5 54 Dey 1999
1.0 70.4 Michaels 1995b
3.0 68.9 18200 1.36 Michaels 1995b
5.0 69.2 Michaels 1995b
5.0 Michaels 1995b
5.0 52.4 1.5 Dey 1997
Serum
10.0 68.8 Michaels 1995b
0.1 48 57.6 2.4 0.37 Michaels 1995b
0.1 40 Dey et al. 1997
0.1 44.1 56.1 Chattopadhyay
1995b
Pluronic
F68
0.2 38 2 Dey 1997
Methocel 0.1 52 55.7 <0.1 Michaels 1995b
E50
0.3 66.1 55.5 Chattopadhyay
1995b
Lethal effects of bubbles in animal-cell culture 455