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PRINCIPLES OF OPERATION
Axopatch 200B, Copyright 1997-1999, Axon Instruments, Inc.
Uncompensated series resistance (R
s
) has several effects on the fidelity of whole-cell
voltage clamp measurements. In the absence of series resistance compensation, these are:
1) Following a step change in command potential, V
c
, the actual cell membrane potential,
V
m
, will respond with an exponential time course (V
m
= V
c
(1-e
-
t/
τ
s
)) with a time constant
given by
τ
s
= R
s
C
m
, where C
m
is the cell membrane capacitance. This time constant is
330 µs for the model cell provided with the Axopatch 200B (R
s
= 10 M
Ω
, C
m
= 33 pF).
This means that the actual membrane potential response to a step voltage command will
have a 10-90% risetime of more than 0.7 ms and will not settle to within 1% of its final
value until about 1.5 ms after the start of a step command. It is typical that after
achieving a whole-cell recording, the access (series) resistance is approximately twice
as large as the original pipette resistance; a three-fold or higher resistance increase is
not uncommon. Thus, series resistances of 20 M
Ω
or more may be encountered. With
a 100 pF cell a series resistance of 20 M
Ω
will result in a membrane-charging time
constant of 2 ms. Settling of the true membrane potential to within 1% of its final
value will require nearly 10 ms after the start of a step command. Note that the
uncompensated whole-cell capacity transient has the shape of the derivative of the true
membrane potential and both will have the same time constant.
2) Uncompensated series resistance will also cause the membrane potential to deviate
from the command potential when ionic membrane current, I
m
, flows. The magnitude
of this error is given by R
s
I
m
;
e.g.
, for R
s
= 10 M
Ω
and I
m
= 2 nA, a 20 mV error will
result. In extreme situations in the presence of voltage gated channels, complete loss of
control of membrane potential can occur.
3) The first two types of errors associated with series resistance described above are well
known to most investigators. The third type of error is less commonly recognized.
Series resistance in conjunction with membrane capacitance forms a one-pole RC filter
with a corner (-3 dB) frequency given by f=1/2
π
R
s
C
m
for the measurement of
membrane currents. This filter will distort currents regardless of their amplitude. For
the parameters of the whole-cell model provided with the Axopatch 200B (R
s
= 10 M
Ω
,
C
m
= 33 pF) this filter restricts true measurement bandwidth to 480 Hz without series
resistance compensation. For a situation with R
s
= 20 M
Ω
and C
m
= 100 pF (as, for
example, may be encountered with isolated cardiac myocytes), the actual bandwidth of
current measurement is only about 80 Hz with no compensation for series resistance.
Содержание Axopatch 200B
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