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200
150
100
50
0
0
200
400
600
t / min
Figure 9 Typical bubble radius R versus time t for bubbles stabilized by
b
-LG at pH
¼
7
in presence of different concentrations of colloidal silica:
&
, 0.5 wt%
b
-LG +
1.5 wt% silica;
B
, 0.5 wt%
b
-LG + 3 wt% silica;
'
, 0.05 wt%
b
-LG + 1.5
wt% silica;
E
, 0.05wt%
b
-LG + 3 wt% silica. The solid lines indicate the
expected behaviour of 0.05 wt%
b
-LG on its own
13
200
150
100
50
0
0
200
400
t / min
Figure 10 Comparison of bubble radius R as a function of time t for bubbles stabilized by
colloidal silica + DDAB or
b
-LG at pH
¼
7:
'
, 0.5 wt% silica + 8
10
4
mol dm
3
DDAB;
E
, 1 wt% silica + 0.05 wt%
b
-LG
13
200
150
100
50
0
0 200
400
t / min
Figure 11 Comparison of bubble radius R as a function of time t for bubbles stabilized by
0.05 wt%
b
-LG at pH 7 + different silica particles:
'
, 1 wt% colloidal silica;
E
, 1 wt% fumed silica. The solid lines above indicate the expected behaviour of
0.05 wt% b-LG on its own
13
In Figure 11 the effect of silica particle size is presented, where the time-
dependent radii for bubbles stabilized by 5.5-nm (colloidal) and 20-nm (fumed)
silica are compared. The behaviour of a bubble stabilized by pure b-LG is also
represented. It is obvious that the smaller colloidal silica particles can enhance
the lifetime of the bubbles to a much greater extent than does the fumed silica.
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