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PRINCIPLES OF OPERATION
Axopatch 200B, Copyright 1997-1999, Axon Instruments, Inc.
For an ideal op amp
1
the pipette current is the same as the current through the
feedback element (R
f
). Since the op amp in the probe acts to keep the voltage at its
two inputs equal to each other, we know that the potential at its negative input
equals V
p
(pipette potential). Thus, the voltage across R
f
is V
o
- V
p
, which is
calculated by the differential amplifier in the control box. Subsequent amplifiers
are used to scale the gain and remove voltage offsets.
A fundamental problem of this circuit when used for patch clamping is that the
output bandwidth of the probe is inherently low. To a first approximation, the
bandwidth is set by the product of R
f
and the stray capacitance across it. For
example, if R
f
is 500 M
Ω
and the stray capacitance is 0.5 pF, the bandwidth is
To overcome this limitation, the probe output is passed through a high-frequency
boost circuit. The gain of this circuit is proportional to the frequency.
Capacitor Feedback
An alternative to measuring current across feedback resistors is to measure current
as the rate of change of the voltage across a capacitor. Figure 16 shows the
essential parts of an integrating headstage.
V
p
DIFFERENTIATOR
+
-
= 1 pF
I
f
OFFSET
AND
SCALING
I
V
o
INTEGRATOR
f
c
+
-
+
-
Figure 16.
Capacitive headstage.
1 op amp - operational amplifier
Содержание Axopatch 200B
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