Biomedical Engineering Reference
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1st
2nd
80
80
200
200
G
I
G
I
60
G
II
60
150
G
II
150
40
40
100
100
20
20
50
50
0
0
0
0
0.0000
0.0025
0.0050
0.0000
0.0025
0.0050
q
L
/
q
gA
q
L
/
q
gA
1st
200
2nd
200
80
80
G
I
G
I
60
G
II
60
150
G
II
150
40
40
100
100
20
20
50
50
0
0
0
0
0.0000
0.0025
0.0050
0.0000
0.0025
0.0050
q
L
/
q
Alm
q
L
/
q
Alm
Fig. 5.19
Energy (
G
I
and
G
II
) as a function of
q
L
/
q
gA
for the gA channel (
upper panel
)or
q
L
q
Alm
for the Alm channel (
lower panel
) in lipid bilayer energetics in the first- and second-order
of lipid screening, respectively. Here,
r
LL
/
=
7
.
74597 Å
F
dis
∝
exp
(
d
0
−
l
)
(5.32)
which is very different from the dissociation force calculated based on the bilayer
elastic model [
38
,
40
,
66
,
67
] where
F
dis
on a gA channel has been reported to
change linearly with the change of
d
0
−
l
(see Eq.
5.12
for comparison) [
6
,
13
].
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