Biomedical Engineering Reference
In-Depth Information
Based on
Eqns (16.48) and (16.49)
, we can determine the ratio of plasmid-free cells as
X
X
þ
þX
y
¼
y
0
exp½ðm
G
m
G
þ
þP
y
þ0
ðm
G
m
G
þ
þP
=þ
m
G
þ
ÞþP
=þ
m
G
þ
=þ
m
G
þ
ÞtP
=þ
m
G
þ
y
0
y
þ0
ðm
G
m
G
þ
þP
=þ
m
G
þ
ÞþP
=þ
m
G
þ
exp½ðm
G
m
G
þ
þP
=þ
m
G
þ
Þt
¼
m
G
m
G
þ
þ
(16.50)
If we let
m
=þ
¼ P
=þ
m
G
þ
(16.51a)
Dm ¼ m
G
m
G
þ
þP
=þ
m
G
þ
(16.51b)
The
Eqn (16.50)
can be simplified to yield
y
0
1y
0
Dmþm
=þ
m
=þ
expðtDmÞ
y
0
1y
0
Dmþm
=þ
þðDmm
=þ
ÞexpðtDmÞ
y
¼
(16.52)
Eqn
(16.52)
can be applied directly to determine the specific rates and probability of loosing
plasmid if a series of experimental data are available.
Fig. 16.17
illustrates the instability
profile for three limiting cases:
(1) m
G
m
G
þ
>>
P
/
þ
m
G
þ
growth-rate-dependent instability dominant
(2) m
G
m
G
þ
P
/
þ
m
G
þ
segregational instability dominant
(3) m
G
þ
>>m
G
þ
P
/
þ
m
G
þ
effective selective pressure
The difference in specific growth rates can be altered by medium and host
e
vector design.
(a)
(b)
(c)
1
1
1
0.75
0.75
0.75
y
-
y
-
y
-
0.5
0.5
0.5
y*
0.25
0.25
0.25
0
0
0
0
0
0
time
time
time
µ
G-
-
µ
G+
>>
P
-/+
µ
G+
µ
G-
-
µ
G+
≤
P
-/+
µ
G+
µ
G+
>>
µ
G-
+
P
-/+
µ
G+
FIGURE 16.17
The shape of plasmid-free cell fraction versus time for three limiting cases of specific growth
rates.
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