biofisika membran-11-2009 eng.ppt
TRANSCRIPT
8/10/2019 Biofisika Membran-11-2009 eng.ppt
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REVIEW AND Theoretical
Modeling membrane
Basically, to explain the transportphenomena in the membrane. then
conducted a review of theoretical
and modeling.
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Electrochemical Reviews
• Based on the membraneelectrochemical potential canbe formulated as follows:
• i
=
i
o
kT ln C
i
Z
i
q
Reviews electric force and
electric field:
•Ei = -
•Fi = qi Ei
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Current of ionic
• J i = q Di ZiCiEi/(kT)
• With substituted Ei,
• Get Nerns – planck equation
dx
d
kT
CDqZ
x
CqDZJ ii
22
iiiii
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IMPEDANCE
The conductance value can be obtained Norcapacitance :
m
~
m
~
CIG
1Z
LICDZ
kTL
q
1Z
0~
ii
2
i
2
~
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conduktance
Capacitance
ii
2
i
2
CDZkTL
q
L
0
• This is to explain the theoretical
formulation of the impedance,
capacitance and inductance of themembrane that interact with the
solution ionic or ion
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Membrane modelling• Tues membrane can be modeled by
electric circuits consisting of a
combination of capacitors and
inductors (coster)
C C
G G G
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Analisis impedansi
•
Combined series between Z1 and Z2and see ZM formulation, it willgenerate value membraneconductance and capacitance.
1
~
1
~
CIG
11Z
2
~
2
2
~
CIG
1Z
m
~
m
m
~
CIG
1Z
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222
222
)2C1C()2G1G(
)1G2C2G1C()2G1G(2G1GGm
222
222
)2C1C()2G1G(
)2C1C(2C1C2C1G1C2GCm
Cm Gm
f
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TRANSPORT OF ION
• If we consider a charged ion, and hehas the energy itself.
• Overall ions basically do not want to
be in the area of energy exceeds theenergy itself.
• Energy self-ions are formed due tothe electrostatic energy has to do
with the dielectric constant
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• In view of the basic electrical
theory of self-electrostatic
energy is the integral of theelectric field
~
0r
r 4
2
0
2
0
dr )4(
)zq(5.0
u 4
2
)d8(
)zq(u
0
2
• Z ion valency
• d pore size
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Membran
• u
• u
The membrane has a dielectric constant
lower than the water, then the energy itself
is higher than in water.Ions in the membrane transport of energy is
needed or something that makes the energy
ions increases. Or lower energy membranes
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This is lower energy self-ions
when passing through the
membrane• A. thickness Factor
• L = thickness
• The contribution of the membrane
thickness is very small
)2
ln()l4(
)zq(u
mw
w
0m
2
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• B. Ion kristal
• Ions across the membrane is considered
an ionic crystal (crystal form), notcovered in water ions
Ketoka ion energy Pebedaan are the
inner and outer membrane is:
Slightly larger than the thickness factor
)11
()d8(
)zq(u
wm0
2
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C. hydrated ions
•
with the ions of water covered the ionradius will tend to dilate which causesa small ion energy.
• With the arising water interfacetension between water and membrane
(I). Thus the addition of energy (u2)due to these interface
• U2=4Ib2,
• b is hydrated ion radius
• Thus the total energy differencebecomes
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D. Ion pairs
• Ions in the opposite sign to form a pair
and then move together through themembrane
If d + and d-represents the radius of the
positive and negative ions, and j the
distance between them, then the
electrostatic energy of this ion pair is
) j4(
)zq(
)d8(
)zq(
)d8(
)zq(u
m0
2
m0
2
m0
2
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• J d+ + d _
•If considered these ionstogether then
• J = d+ + d _ ,
• For d+ = d _
• it is the same as
• before
)dd(4()zq(
)d8()zq(
)d8()zq(u
m0
2
m0
2
m0
2
)d8(
)zq(u
m0
2
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E. Ion Transport through pore
• if there are pores in the membrane
is the membrane area which there
is a high dielectric constant, so
that the ions would prefer to gothrough the area
)r 4(K )zq(dum0
2