First published online June 29, 2007
Journal of Experimental Biology 210, 2489-2500 (2007)
Published by The Company of Biologists 2007
doi: 10.1242/jeb.006361
Properties and possible function of a hyperpolarisation-activated chloride current in Drosophila
Uwe Rose1,*,
Christian Derst2,
Mario Wanischeck1,
Christiane Marinc1 and
Christian Walther3
1 Institute of Neurobiology, University Ulm, Albert-Einstein-Allee 11, Ulm
89160, Germany
2 Institute for Integrative Neuroanatomy, Charite, Berlin,
Germany
3 Institute of Physiology and Pathophysiology, Philipps University Marburg,
Marburg, Germany

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Fig. 1. Currents recorded from a muscle fibre during prolonged hyperpolarising
voltage commands. (A) Current electrode filled with 2 mol l1
K-acetate. After the instantaneous jump, a small inward current develops
within seconds. The superimposed traces, recorded 1 and 10 min after impaling
the fibre, are nearly identical. Note that the lower trace represents the
recorded voltage imposed by the pulse protocol. (B) Currentvoltage
relationships for the fibre in A. The instantaneous current (open symbols) is
linear whereas the late current (filled symbols) exhibits slight inward
rectification. (C) Recording from another fibre where current electrode filled
with 3 mol l1 KCl was used; voltage jump as in A. Although
the current recorded is initially similar to that in A, the slow inward
component is clearly increased 10 min after impalement. (D)
IV plot for the fibre recorded in C. The
instantaneous current is practically linear, as in B, but the inward
rectification of the late current is enhanced 10 min after impalement. Note
inward-going tail currents after jumping from 110 to 60 mV. In
both A and B the voltage electrode contained 3 mol l1
KCl.
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Fig. 2. Hyperpolarisation-induced current in a Cl-loaded muscle
fibre. (A) Currents elicited by the hyperpolarising voltage commands shown in
the inset. Note the pronounced tail currents after deactivating jumps to
60 mV. Small, short inward currents are miniature excitatory junctional
currents. The recordings were performed after holding the fibre for 5 min at
50 mV with a holding current of 5 nA. The current electrode
was filled with 3 mol l1 KCl. (B) Current clamp recordings
subsequently performed from the same fibre; currents were injected according
to the protocol shown in the inset.
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Fig. 3. Reversal potentials of K+ current and hyperpolarisation-induced
current. (A) Sample traces of tail currents recorded subsequently in one
fibre. Left: deactivating K+ currents, mainly consisting of A
currents. For K+ current activation the fibre was first depolarised
from 70 to +10 mV for 80 ms, then the voltage was stepped to different
levels as seen in B. Right: deactivation of hyperpolarisation-dependent
currents. For activation the voltage was stepped from 50 mV to
120 mV for 4 s, followed by deactivating jumps to 50 mV or more
positive levels as seen in B. (B) Mean currentvoltage relationships of
peak tail-currents obtained, as in A, from paired recordings of four fibres
from two animals. Note that the ordinate gives relative sizes of the currents,
i.e. normalised to IK at V=30 mV and to
hyperpolarisation-dependent current at 50 mV, respectively.
[K+]o and [Cl]o were
standard, i.e. 10 mmol l1 and 95 mmol l1,
respectively. The mean reversal potential was 55.2±4.1 mV for
the K+ current and 20.5±4.0 mV for the
hyperpolarisation-activated current (l=2, f=4). The current electrode
contained 3 mol l1 KCl; recordings of the
hyperpolarisation-dependent currents were performed 5 to 10 min after impaling
the fibre.
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Fig. 4 The reversal potential of the hyperpolarisation-induced current depends on
the external Cl concentration. Currentvoltage
relationships of tail currents as shown in
Fig. 3A, right-hand side.
Averages of paired measurements in three fibres, performed first with
[Cl]o=65 mmol l1 and then with
[Cl]o=20 mmol l1. The reduction
of [Cl]o led to a positive shift of the reversal
potential, i.e. from 18.2±3.8 mV to +2.2±1.8 mV.
K+ currents were blocked by means of 20 mmol l1
TEA, 1 mmol l1 4-aminopyridine (4AP) and 0.1 mmol
l1 quinidine.
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Fig. 5. Steady-state activation of the chloride-conductance,
GCl,H. (A) Mean GV relationship
at two different internal Cl concentrations. Paired
measurements of currents and of ECl were performed in six
fibres after moderate and strong Cl loading of the fibre
(the respective recordings were performed 1 and 5 min after impalement; for
details of the approach and for the voltage-clamp protocols employed, cf.
Materials and methods). Currents were converted to conductance, G.
The conductance is greatly enhanced at raised
[Cl]i. This effect is largely because of the
increase in maximal conductance. (B) Normalised GV
relationships for the data shown in A. The rise in [Cl]i led to
some positive shift of the curve on the voltage axis. Curves in A and B are
Boltzmann-fits. For further analysis, cf.
Table 2. Error bars indicate
s.e.m.
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Fig. 6. Effects of pH changes on time course and amplitude of
ICl,H. (A) A change from pH 7.2 to 8.4 leads to a faster
time course of the hyperpolarisation-induced Cl current. The
amplitude, obtained by extrapolating the current until it reached steady
state, was somewhat reduced. Voltage jump was as shown in B. (B) At pH 6.0 the
amplitude became greatly reduced. The time course of the current appears to be
slowed, yet in fact it remained unaffected, as found on fitting double
exponentials to the current traces. Both pH effects were rapid; they were
recorded 1 min after changing the bath solution. The recordings labelled
`wash' were made 3 to 5 min after changing back to pH 7.2. For a more detailed
analysis of these effects see Table
1.
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Fig. 7. Potentiation of ICl,H in hypotonic saline. (A) Currents
recorded from one fibre on jumping the voltage from 50 to 120
mV. The intervals between the different recording conditions lasted 810
min. (B) Amplitudes of tail currents following hyperpolarising prepulses as in
A. Data from the same fibre as in A. The lines connecting the data points
represent Boltzmann-fits with the following parameters, presented in the
sequence control-hypotonic wash: Imax: 5.2, 8.5, 3.4 (nA);
V0.5: 110, 106, 106 (mV); k
(slope factor): 13.1, 11.8, 10.0 (mV). (C) Mean osmotically induced increase
in tail currents recorded after 120 mV prepulses as shown in A (f=4,
l=2, N=4).
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Fig. 8. Effect of 9-AC. (Ai) Representative recordings from one fibre performed 3
min (control), 8 min (9-AC) and 17 min after impaling the muscle fibre. 9-AC,
at 120 mV, blocks ICl,H in a time-dependent manner
and reduces the tail current on jumping back to 50 mV. Prolonged
washing led to almost full recovery of ICl,H. (Aii) Means
and their standard errors of normalized ICl,H from four
experiments. (B) The effect of 1 mmol l1 9-AC on the resting
membrane conductance measured by voltage ramps. 9-AC significantly lowered the
membrane conductance of muscle fibres by approximately 20%. (C) Synaptic
currents were consistently decreased by 1 mmol l1 9-AC to
approximately 70% of the control value (N=4). This effect was
reversed by washing with saline.
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Fig. 9. Effect of 9-AC on stimulus evoked muscular contraction. (A,B) Muscular
contractions were consistently augmented when 1 mmol l1 9-AC
was applied to the bath. Washing with saline almost reversed this effect. The
9-AC effect was basically similar for single contractions (twitch) or tetanus
(5 Hz, 10 Hz) contractions, although it seemed to be less pronounced for
twitch contractions. However, no significant difference was detected between
twitch and tetanus. 9-AC did not change the time course (50% relaxation time)
of twitch contractions.
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© The Company of Biologists Ltd 2007