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Using the Patch Clamp
be essential if you will be giving voltage pulses in your experiment. It is a good idea to start out with
V-membrane
set to zero, as we specified above; an alternative is to start with
V-membrane
set to the holding potential you
desire (e.g., -70 mV). If no voltage jumps are required, turn the stimulus off to avoid introducing artifacts. If
voltage jumps are to be applied, switch the
Gain
and
Filters
to the values you will be using (the settings may be
programmed under
SEAL
). Be sure to use
Gain
settings of 50 mV/pA or above for lower noise in single-channel
recordings. Keep the
Filter 1
switch set at 10 kHz unless you actually will need the 100 kHz full bandwidth for some
reason; otherwise you might drive the current monitor output or your recorder’s input amplifiers into saturation
with the very large amount of high-frequency noise. Should you use the full bandwidth, you should avoid
Gain
settings above 100 mV/pA for the same reason. If you are applying voltage pulses to the patch membrane, you
probably will want to subtract control traces from the traces containing the channels of interest in order to remove
the capacitive transients. Nevertheless, it is important to try to cancel the capacitive transients as well as you can
in order to avoid saturating any amplifiers, the recording medium or the AD converter. It is a good idea to set
the
C-fast
and
τ
-fast
controls while you observe the signal without any filtering beyond the internal 10 kHz filter.
Then, during the recording, watch to see if the clipping light blinks. When it does, it means that internal amplifiers
in the
EPC 10 USB
are about to saturate, and/or that the current monitor output voltage is going above 10 V
peak, on the peaks of the transients, and you should readjust the transient cancellation controls. Otherwise, it is
likely that the recording will be non-linear and subtraction will not work correctly. The fast transient cancellation
is not sufficient to cancel all of the capacitive transients in a patch recording. This is partly because the pipette
capacitance is distributed along the length of the pipette; therefore, each element of capacitance has a different
amount of resistance in series with it, so that a single value of
τ
-fast
will not provide perfect cancellation. The time
course of the transients also reflects dielectric relaxation in the plastic of the pipette holder and in the pipette glass.
These relaxations are not simple exponentials, but occur on time scales of about 1 ms. If you use pipette glass
with low dielectric loss (e.g., aluminosilicate glass) or if you are careful to coat the pipette with a thick coating and
near to the tip, the relaxations will be smaller. You can cancel part of these slow relaxations by using the
C-slow
controls, with the
C-slow Range
set to 3 pF.
Note:
For cell-attached or inside out patch configuration, positive pipette voltages correspond to a
hyperpolarization of the patch membrane, and inward membrane currents appear as positive signals
at the current monitor outputs. The
Patchmaster
program compensates for this by inverting digital
stimulus and sampled values in these recording configurations such that the stimulation protocols, holding
voltages, and displays of current records in the
Oscilloscope
all follow the standard electrophysiological
convention. In this convention, outward currents are positive and positive voltages are depolarized.
However, the analog current and voltage monitor outputs are not inverted in these recording modes.
10.3
Whole-Cell Recording
10.3.1
Breaking the Patch
After a gigaseal is formed, the patch membrane can be broken by additional suction or, in some cells, by high
voltage pulses (600-800 mV, see
Zap
function). Electrical access to the cell’s interior is indicated by a sudden
increase in the capacitive transients from the
Test Pulse
and, depending on the cell’s input resistance, a shift in
the current level. Additional suction sometimes lowers the access resistance, causing the capacitive transients to
become larger in amplitude but shorter. Low values of the access (series) resistance are desirable and, when Rs-
compensation is in use, it is important that the resistance be stable as well. A high level of Ca
2+
buffering capacity
in the pipette solution (e.g., with 10 mM EGTA) helps prevent spontaneous increases in the access resistance due
to partial resealing of the patch membrane.
10.3.2
Capacitive Transient Cancellation
If the fast capacitance cancellation was adjusted (as described above) before breaking the patch, then all of the
additional capacitance transient will be due to the cell capacitance. Canceling this transient using the
C-slow
and
R-series
controls will then give estimates of the membrane capacitance and the series resistance. The easiest way
of cancellation is provided by the
Auto C-slow
function which may be activated by selecting the
Auto
button or
the
Whole Cell
button (if included in the protocol function). In cases where the
C-slow
transient has a short time
constant (100
µs
or smaller), some improvement of the overall compensation may be achieved by alternating cycles
of
Auto C-fast
and
Auto C-slow
(if this doesn’t work satisfactorily you may fine-tune the compensation controls
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Содержание EPC 10 USB
Страница 1: ...Hardware Manual Version 2 8 EPC 10 USB Computer controlled Patch Clamp Amplifier...
Страница 6: ......
Страница 10: ...4 Introduction http www heka com...
Страница 16: ...10 Description of the Hardware http www heka com...
Страница 22: ...16 Installation http www heka com...
Страница 32: ...26 Verifying and Testing the EPC 10 USB http www heka com...
Страница 44: ...38 The control software http www heka com...
Страница 48: ...42 Operating Modes http www heka com...
Страница 54: ...48 Compensation Procedures http www heka com...
Страница 58: ...52 Patch Clamp Setup http www heka com...
Страница 64: ...58 Using the Patch Clamp http www heka com...
Страница 74: ...68 Appendix II Probe Adapters http www heka com...
Страница 76: ...70 Appendix III S Probe http www heka com...
Страница 81: ......