inhibition of human kv3.1 current expressed in xenopus oocytes by the toxic venom fraction of...
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RESEARCH ARTICLE
Inhibition of human Kv3.1 current expressed in Xenopus oocytesby the toxic venom fraction of Androctonus australis hector
Amani Cheikh • Rym Benkhalifa • Zied Landoulsi •
Imen Chatti • Mohamed El Ayeb
Received: 29 January 2013 / Accepted: 3 June 2013
� The Pharmaceutical Society of Korea 2013
Abstract AahG50, the toxic fraction of Androctonus aus-
tralis hector venom, was studied on human Kv3.1 channels
activation, stably expressed in Xenopus oocytes using the two-
electrode voltage clamp technique. AahG50 reduced Kv3.1
currents in a reversible concentration-dependent manner, with
an IC50 value and a Hill coefficient of 40.4 ± 0.2 lg/ml and
1.3 ± 0.05, respectively. AahG50 inhibited IKv3.1 without
modifying the current activation kinetics. The AahG50-
induced inhibition of Kv3.1 channels was voltage-dependent,
with a gradual increase at lower concentrations and over the
voltage range of channels opening. However, at higher con-
centrations, the inhibition exhibited voltage dependence only
in the first range of channels opening from -20 to ?10 mV,
but demonstrates a low degree of voltage-dependence when
channels are fully activated. In the literature, toxins have
previously been isolated from AahG50, KAaH1 and KAaH2
and were reported not to have any effect on IKv3.1. The
present article’s findings suggest that AahG50 may contain a
peptidic component active on Kv3.1 channels, which inhibits
IKv3.1 in a selective manner.
Keywords Potassium channel � Kv3.1 � Toxins �Androctonus australis hector � Kv3.1channel blocker
Introduction
Potassium channels form a large family of transmembrane
proteins that are present in almost living cells. They play
crucial roles in many different cellular functions, including
cell excitability, neurotransmitter release, signal transduction
and neuronal integration (Coetzee et al. 1999). Their wide
distribution in many tissues is associated with important
functions in excitable and non excitable cells that are now
better understood thanks to the discovery of animal toxins.
Kv3.1, one of the Shaw-type K? channel, is abundantly
expressed in neurons that have the ability to fire at high fre-
quencies (Perney et al. 1992; Wang et al. 1998). It is
expressed at particularly high levels in brainstem. Kv3.1 has
a number of features that distinguish it from other potassium
channels: a high activation threshold and very rapid activa-
tion and deactivation kinetics (Kanemasa et al. 1995). On the
other hand, the lack of Kv3.1 channel subunits is mainly
responsible for behavioral alterations that include impaired
motor performance, hyperactivity and sleep loss (McMahon
et al. 2004). Besides, potassium-channel-blocking scorpion
toxins have been shown to be valuable tools for the study of
potassium channels and so to understand many physiological
and pathophysiological processes (Salkoff et al. 1992). Sev-
eral toxins target Kv1 subunits and are useful in identifying
the function of low threshold channels (Geiger and Jonas
2000; Southan and Robertson 2000; Dodson et al. 2003).
There is a shortage of Kv3 subfamily specific-toxins, but
Diochot et al. (1998) reported that sea anemone toxins BDS-I
and BDS-II (blood depressing blockers) were highly specific
blockers for Kv3.4 in expression systems. According to Ye-
ung et al. (2005), these toxins are also able to inhibit Kv3.1
and Kv3.2 subunits. Nevertheless, some chemical molecules
have been reported to be active on Kv3.1 channels and used
in different therapeutic fields. Among which, the Prozac is
Imen Chatti—Former member in the laboratory.
A. Cheikh (&) � R. Benkhalifa (&) � Z. Landoulsi � I. Chatti �M. E. Ayeb
Laboratoire des Venins et Molecules Therapeutiques, Institut
Pasteur de Tunis, BP 74, 1002 Tunis, Tunisia
e-mail: [email protected]
R. Benkhalifa
e-mail: [email protected]
123
Arch. Pharm. Res.
DOI 10.1007/s12272-013-0176-5
known by its antidepressant activity (Choi et al. 1999) and the
psoralen by its anticonvulsant activity (Sung et al. 2009).
They are all blocking Kv3.1 channel, but also other different
channels subtypes, such as sibutramine (Kim et al. 2007) and
Riluzole (Ahn et al. 2005). In our laboratory, we are inter-
ested by the biochemical characterization of bioactive sub-
stances in scorpion venoms that have a potentially therapeutic
value. As a matter of fact, scorpion venoms are mixtures of
many polypeptides active on ion channels, in which only a
small proportion is lethal to mammals. Previous studies on
Androctonus australis hector (Aah) scorpion venom allowed
us to isolate toxins that were active on Kv1 subunit types,
such as KAaH1 active on Kv1.1 and Kv1.3 channels (Srairi-
Abid et al. 2005).
In the present work, we have studied the effect of the
toxic fraction of Aah venom (AahG50) on Kv3.1 channel
activity, expressed in Xenopus oocytes. We reported that
this fraction inhibited the Kv3.1 currents in a potent manner,
without modifying the kinetics of activation. The same
fraction was also shown to block Kv1.1 and Kv1.3 currents,
at lower concentrations. Since AahG50 is a mixture of
neurotoxins, we reported the toxins active on Kv3.1 chan-
nels to be different from those acting on Kv1.1 and Kv1.3.
Materials and methods
Purification of Aah venom
The venoms of Androctonus australis hector (Aah) was
collected from Beni Khedach (Tunisia) by the veterinary
department of Pasteur Institute—Tunisia and kept frozen at
-20 �c, in its crude form until used. The crude venom was
dissolved in water and loaded on Sephadex G50 gel filtration
chromatography column (K26/100, Pharmacia) to separate
the toxic fraction named AahG50. The column was equili-
brated and eluted at 15 �C with 0.1 M acetic acid buffer (pH
4.7), with a flow rate of 0.5 ml/min. Following (Miranda
et al. 1970), the detection was carried out at 280 nm, by a
spectrophotometer, namely BECKMAN DU 640. After
freeze-drying, the toxic fraction is stored at -20 �C until use.
Synthesis of Kv3.1 mRNA
The plasmid containing cDNA encoding for the Kv3.1 wild
type channel was graciously provided by Dr. Marcel Crest
(Research Center in Neurobiology and Neurophysiology of
Marseille). The DNA matrix was linearized by HpaI, and
capped cRNA was transcribed in vitro, using the SP6
mMessage mMachine kit (Ambion).
Electrophysiological measurements
Mature Xenopus laevis female were anaesthetized with
0.17 % solution of Tricaine (Ethyl 3-aminobenzoate
methanesulfonate salt, Sigma) during 45 min. Experiments
on Xenopus were approved by the Institutional Research
Board of Pasteur Institute—Tunis and carried out follow-
ing the European Community Council Directive (86/609/
EEC), for experimental animal care and procedures. Parts
of ovaries were then surgically removed from the abdom-
inal cavity and bathed in a calcium-free modified Barth’s
Solution (MBS: NaCl 88 mM, KCl 1 mM, MgCl20.41 mM, NaHCO3 2.4 mM, MgSO4 0.82 mM, HEPES
10 mM, pH 7.4). Oocytes were defolliculated enzymati-
cally by incubation in collagenases A and B (2 mg/ml,
Boehringer Roche), then stages V and VI oocytes were
selected by mechanical defolliculation, using forceps.
Individual oocytes were injected with 5–8 ng of mRNA,
using an automatic nano-injector (Nanoject, Drummond);
then incubated in MBS sterile solution: calcium-free MBS
added with CaCl2 2.4 mM, Ca (NO3)2 0.33 mM, Genta-
mycin (Sigma) 50 mg/l), pH 7.4, during 48 h at 18 �C and
before electrophysiological measurements were performed.
The MBS was changed once a day.
Electrophysiological measurements of Kv3.1 current
were recorded with the two electrodes voltage-clamp
method using a Gene Clamp 500 amplifier (Molecular
Devices, USA). Oocytes were immersed in Ca2? free MBS
and impaled with 2 intracellular glass electrodes filled with
3 M KCl. The resistance of the pulled electrodes (P-97
puller; Sutter Instruments, Novato, CA, USA) was 1–2 MW.
The perfusion system was controlled by a Manifold Solution
Changer (MSC-200; Bio-Logic; Grenoble, France). Data
acquisition and analysis were performed using Clampex and
Clampfit from pclamp8 software (Molecular Devices, Sun-
nyvale, CA, USA). Leak and capacitive currents were sub-
tracted during analysis. The study of AahG50 effect (10, 25,
50 and 100 lg/ml) was carried out on the Kv3.1 currents
recorded, using 250 ms depolarizing pulses from -40 to
?40 mV.
Electrophysiological results analyses
Obtained results are recorded and analyzed by the Pclamp 8.2
software (Molecular Devices). Activation curve is estimated
in terms of the relative conductance g/gmax (g = I/V - Vinv).
With Vinv as the inversion potential, curves are fitted by
Boltzmann equation: g/gmax = 1/(1 ? exp[(E0.5 - Em)/k],
where Em is the membrane potential, E0.5 is the half-activa-
tion potential and k is the slope factor.
A. Cheikh et al.
123
Results
Sephadex gel filtration of scorpion venoms
Sephadex gel filtration of scorpion venoms is carried out
according to Miranda et al. (1970) protocol. The profile of
purification of the venom of Androctonus australis hector
highlights the existence of four non-toxic fractions (M1–
M4) and one toxic fraction named AahG50 (Fig. 1).
Concentration-dependent effects on Kv3.1 currents
by AahG50
The effect of the toxic fraction of Androctonus australis
hector venom (AahG50) was tested on Kv3.1 channels
stably expressed in Xenopus oocytes and studied by means
of the two electrodes voltage-clamp technique. Figure 2a
shows the superimposed control Kv3.1 current traces under
control conditions and in the presence of different con-
centrations of AahG50 (5, 10, 25, 50 and 100 lg/ml),
obtained after a depolarizing step of ?20 mV, during
250 ms. AahG50 (5 lg/ml) was applied for *2 min and
the Kv3.1 currents were decreased to ?20 mV from 3.2 to
2.8 lA, whereas a more pronounced effect was obtained
with higher concentrations. The current amplitude
decreased from 3.2 to 2.2 lA (10 lg/ml) and from 3.2 to
1.7 lA (25 lg/ml) respectively; then reached 0.9 lA after
the perfusion of 50 lg/ml of AahG50.
The inhibition of Kv3.1 currents induced by AahG50
affect the current amplitude in a concentration-dependent
manner. Figure 2b shows the concentration dependence of
Kv3.1 current inhibition by AahG50. The concentration–
response curve was obtained by plotting the decrease of
currents at the end of a 250 ms pulse of ?40 mV in terms
of AahG50 concentration. The normalized currents were
fitted with the Hill equation, which yielded an IC50 value of
40.4 ± 0.2 lg/ml and a Hill coefficient of 1.3 ± 0.05
(n = 3–8).
To study the evolution of current inhibition as a time
function, the time-course of AahG50 (50 lg/ml) effect was
generated as shown in Fig. 2c. The inhibition appeared
after 10 s of the toxic fraction perfusion and the current
decreased gradually and reached a steady state within
3 min. Following a 1-min washout by means of MSB
perfusion, the current recovered nearly the control value
with a faster time course, indicating that the effect of
AahG50 is largely reversible upon washout.
Voltage-dependent effect on Kv3.1 currents,
by AahG50
The inhibitory effect of AahG50 was estimated according
to the variation of the outward potassium current by gen-
erating current–voltage (I–V) relationships in the range
-40 to ?40 mV. Currents were induced from a holding
potential of -80 mV, with potentials steps in 10 mV
increments, during 250 ms. Under control conditions, the
Kv3.1 expressing oocytes display outward fast-activating
potassium currents that rapidly deactivate (Fig. 3a left
panel). The perfusion of AahG50 50 lg/ml in the oocyte
bath strongly reduces the Kv3.1 current (Fig. 3a right
panel).
The voltage dependence of steady-state activation was
studied in both the absence and the presence of AahG50
(50 lg/ml) (Fig. 3b). Conductance–voltage (G–V) relation-
ships for Kv3.1 were calculated and the activation curve
obtained under control conditions was drawn by fitting the
normalized conductance to the Boltzmann equation. The
current activation threshold was approximately -20 mV, the
potential for half-maximum activation (V1/2) and the slope
factor value (k) were respectively 8.4 ± 0.5 and
8.3 ± 0.4 mV (n = 16). After the perfusion of AahG50
(50 lg/ml), the threshold of activation did not yield any
change. The activation curve shifted to more positive
potentials, the value of V1/2 was 13.7 ± 1.3 mV and k was
9.8 ± 1.2 mV (n = 9). The shift in the depolarizing direc-
tion in activation is about 5 mV even if the change in the
slope factor is not significant. In presence of AahG50, the
G–V curve saturated at a lower conductance level. In Fig. 3c,
the K? currents carried by Kv3.1 channels, displayed acti-
vation kinetics, which were best fitted by biexponential
function (Grissmer et al. 1992). The activation time constant
s was slightly voltage-dependent in potential range values
ranging from -10 to ?40 mV. In presence of AahG50
(50 lg/ml), the slowing of activation rate was more pro-
nounced at potentials ranging from -10 mV (s = 70 ±
9.7 ms) to ?10 mV (s = 28 ± 3.3 ms). At potentials higher
than ?10 mV, the slowing of activation rate is less noted
Fig. 1 Purification of Androctonus australis hector scorpion venom.
Dialyzed venom was loaded into a Sephadex G50 column and five
fractions were collected (M1, M2, AahG50, M3 and M4)
Inhibition of human Kv3.1 current
123
(s varies from 28 ± 3.3 ms at ?10 mV to 21.16 ± 4.4 ms at
?40 mV).
Figure 3d showed relative normalized current (IAahG50/
Icontrol) as a function of potential. The toxic fraction
decreased the current amplitude starting at 0 mV, when
applied at lower concentrations (10 and 25 lg/ml). From
-20 to 0 mV, the percentages of inhibition variations vary
not significantly, as a function of potentials. At these
concentrations, AahG50 decreased Kv3.1 current in a
voltage dependent manner at potential positive to ?10 mV.
At 10 lg/ml, the maximal inhibition rates observed at ?10
and ?40 mV were respectively 15.5 ± 3 and 31.6 ± 4 %,
when currents are fully activated.
At higher concentration (50 lg/ml), this inhibitory effect
includes the whole voltage range of channel opening
(Fig. 3d), but not in the same manner. The curve shape pre-
sents a biphasic evolution. From -20 to ?10 mV the
inhibitory effect increased in a rapid manner. Between -10
and ?10 mV, the current inhibited by 47.5 % from 14.5 ± 3
to 62 ± 5 %, which corresponds to a fourfold decrease.
However, in the range of ?10 to ?40 mV, we noted that the
inhibitory effect reached a steady state. The current inhibited
by 6.8 %, from 65.2 ± 4 % at ?20 mV to 72.2 ± 3 % at
?40 mV. These results suggested that the inhibition of
IKv3.1 by AahG50 was found to be clearly voltage-and
concentration-dependent. At low concentrations, the toxic
fraction acted at potentials positive to ?10 mV, while at
50 lg/ml its effect was observed in the whole activating
voltage range. The inhibition occurred in a biphasic manner
with a faster effect at potentials less than ?10 mV to reach
then, a steady state with a maximal effect about 72.2 %. The
AahG50 observed effect did not require fully activated
channel.
AahG50 inhibitory effect on Kv1.1 and Kv1.3 currents
In order to characterize the specificity of AahG50 inhibi-
tory effect on Kv3.1, we performed experiments on Kv1.1
and Kv1.3 channels. Figure 4a, b shows the effect of
AahG50 (10 lg/ml) on Kv1.1 current–voltage relationship.
Kv1.1 current traces were elicited from a holding potential
of -80 mV, by potentials ranging from -40 to ?40 mV,
in 10 mV increments during 250 ms in control conditions
(upper panel) and after the application of 10 lg/ml of
AahG50 (lower panel). The Kv1.1 current was activated at
pulses greater than -60 mV, and the steady state I–V
Fig. 2 Concentration dependence for AahG50 block of human Kv3.1
currents expressed in Xenopus oocytes. a Superimposed currents were
obtained by applying 250 ms pulses from a holding potential of -80
to ?20 mV every 3 s under control conditions and after the blockade
by 5, 10, 25, 50 and 100 lg/ml of AahG50. The inhibition levels were
respectively 13.9 % (±8.8 %, n = 3), 27.03 % (±7.2 %, n = 10),
56.81 % (±16.26 %, n = 5), 84.31 % (±7.2 %, n = 3) and 92.1 %
(±5.5, n = 2). b Dose–response curve for the inhibition of Kv3.1 by
various concentrations of AahG50. Currents amplitude were measured
at the end of the depolarizing pulse (?40 mV), the percentage of
inhibition was plotted against respective concentrations of AahG50.
The curve was fitted by the Hill equation which yielded an IC50 value
of 40.4 ± 0.25 lg/ml and a Hill coefficient of 1.3 ± 0.05 (n = 3–8
for each concentration). c Time course of inhibition in the presence of
AahG50, 50 lg/ml. Maximal effect occurs about 3 min after the
beginning of the perfusion. A complete recovery from the inhibitory
effect was observed after the washout of the toxic fraction
b
A. Cheikh et al.
123
relationship curve showed a linear shape between -40
and ? 60 mV (Fig. 4b). The inhibition by AahG50 was
observed in the whole voltage range over which current is
activated and a steady state inhibition was reached at
?20 mV, with 83.9 % of maximum of inhibition. The
same experiments were applied on Kv1.3 currents expres-
sed on Xenopus oocytes (Fig. 4c, d). The current inhibition
by AahG50 was shown at all potentials but did not reach
the saturation as observed with Kv1.1 channels. The steady
state I–V relationship curve showed a similar linear shape
as in the control conditions and the maximum of inhibition
was about 70,4 % at ?40 mV (Fig. 4d).
Effect of KAaH1 and KAaH2 on Kv3.1 channels
Given that KAaH1 and KAaH2 are two toxins that are active
on Kv1.1 and Kv1.3 channels and present in AahG50 (Srairi-
Abid et al. 2005), we tested them on Kv3.1 channels. Currents
were induced by a step to ?20 mV from a holding potential of
-80 mV, during 250 ms. Figure 5a (left and right panels) did
not show any significant effects on the control current traces
before and after the application of 100 nM of KAaH1 and
KAaH2. Histograms in Fig. 5b summarize data deduced from
different oocytes (n = 3–8). These results suggest that
AahG50 may contain other toxic compounds active on Kv3.1
channels and different from the toxin showing already spec-
ificity to Shaker potassium channels.
Discussion
The activity of Kv channels is crucial in maintaining the
resting membrane potential, regulating action potential
duration and frequency, and determining the pacemaker
activity in a variety of excitable cells (Jan and Jan 2012).
Besides, toxins from a variety of species have been used to
characterize and pharmacologically profiling different ion
channel types. The effect of toxins on specific ion channels
Fig. 3 Voltage dependent effect of the toxic venom fraction AahG50
on Kv3.1 currents. a Typical voltage activated Kv3.1 currents
expressed in Xenopus oocytes. Current traces are shown in the
absence (left panel) and the presence (right panel) of 50 lg/ml
AahG50. Currents were elicited from a holding potential of -80 mV
by pulses applied in 10 mV increments to potentials ranging from
-40 to ?40 mV (above the figure). b Effect of AahG50 on the
steady-state activation of Kv3.1 currents. The normalized conduc-
tance-voltage relationship of Kv3.1 currents in Xenopus oocytes were
plotted under control conditions and after the perfusion of 50 lg/ml
AahG50. Data were normalized and fitted to the Boltzmann equation.
The V1/2 and the slope factor were respectively 8.3 ± 0.5 mV and
8.4 ± 0.4 (n = 16) for control conditions, and 13.6 ± 1.3 mV and
9.8 ± 1.2 (n = 9) under 50 lg/ml AahG50 application. c Activation
rate of Kv3.1 in absence and presence of AahG50 (50 mV) venom
fraction. Activation kinetics was fitted by biexponential function for
potentials positive to -10 mV. d Voltage-dependant inhibition of
Kv3.1 peak current by 10, 25 and 50 lg/ml of AahG50. Normalized
inhibition was expressed as a relative current (IAaHG50/Icontrol) for
potentials positive to -20 mV
Inhibition of human Kv3.1 current
123
has had a huge impact on the understanding of the physi-
ological as well as pathophysiological role of different ion
channels in cell functions (Grissmer and Tytgat 2004).
The present work describes the selective inhibition of
Androctonus australis hector toxic venom fraction (AahG50)
on cloned neuronal human Kv3.1 expressed in Xenopus
oocytes, using the two electrodes voltage clamp technique.
We were interested by studying whether AahG50 acts on
IKv3.1, and in which manner. AahG50 is composed of
several neurotoxins. Some ones are active on voltage gated
sodium channels such as AaHI, a scorpion a-toxin, con-
sidered as a channel gating-modifier toxin (Bosmans and
Tytgat 2007). In the literature, rarely are toxins reported
active on Kv channels and their mechanism of action is
usually not described (Srairi-Abid et al. 2005). In order to
investigate the AahG50 action mode on Kv3.1 channel, the
toxin classification suggested by Miller in 1995 seems
more suitable to discuss our results. According to this
classification, toxins are grouped into a first class of pore-
blocking toxins that interact with the external vestibule of
the ion conduction pore and a second class that interacts
with the voltage sensing domains of voltage-gated ion
channels and modifies the gating behavior of the channel,
through allosteric mechanisms (Miller 1995).
This study demonstrates that AahG50, inhibited IKv3.1
in a dose-dependent manner, within the concentration
range of 1–100 lg/ml. The inhibition rate of Kv3.1 current
amplitude is about 93 % at 100 lg/ml.
The characteristic of the AahG50-induced inhibition is
based on the following deductions: (1) AahG50 inhibited
IKv3.1, with an IC50 value of 40.4 lg/ml and a Hill coef-
ficient of 1.3. The washout allows the initial current
amplitude recovery. (2) IKv3.1 is inhibited without any
effect on the kinetics of channel activation. (3) In the con-
centration range of 5–50 lg/ml, we have noted that AahG50
effect is characterized by an acceleration of the rate decay.
Previous works, investigating the effect of scorpion
venom fractions, on in vitro expressed ion channels are
very rare. The dialyzed venom of Androctonus mauritani-
cus mauritanicus (Amm) totally blocked KCa current of
Helix U cells at 45 lg/ml (Crest et al. 1992). In a previous
work, we have reported the effect of the non toxic fraction
Fig. 4 AahG50 venom fraction inhibitory effect on Kv1.1 and Kv1.3
currents expressed in Xenopus oocytes. a Voltage-activated Kv1.1
current traces are shown in the absence (upper panel) and the
presence of 10 lg/ml AahG50 (lower panel). Currents were activated
by a voltage step protocol from a holding potential of -80 mV
followed by steps to voltages ranging from -40 to ?40 mV in 10 mV
increments during 250 ms. b The I–V relationship of Kv1.1. Control
currents are shown with empty circles and AahG50 inhibited currents
are shown with filled circles. The inhibition rate was 83.9 % at
?40 mV. c Voltage-activated Kv1.3 current traces are shown in the
absence (upper panel) and the presence of 10 lg/ml AahG50 (lower
panel). Currents were recorded using the same protocol described in
A. d The I–V relationship of Kv1.3. Control currents are shown with
empty circles and AahG50 inhibited currents are shown with filled
circles. The inhibition rate was 70.4 % at ?40 mV
A. Cheikh et al.
123
of Buthus occitanus tunetanus scorpion venom (M1 Bot)
on rat heart contraction and L-type calcium current (ICaL).
Studies with the whole cell patch clamp technique showed
that M1 decreased the ICaL in a dose-dependent manner
with an IC50 of 0.36 lg/ml. Besides, at 10 lg/ml this
fraction also induced a decrease in both heart tension and
rate (Cheikh et al. 2006).
The activation kinetics in presence of AahG50 (50 lg/ml)
demonstrates an inhibitory effect from the threshold poten-
tial (-20 mV) and the channel saturation is reached at
earlier potentials. In the same manner as gambierol and
subitramine, AahG50 doesn’t require the open channel state
to bind to Kv3.1 channels (Kim et al. 2007; Kopljar et al.
2009). AahG50 shifts slightly the V1/2 by about 5 mV
contrary to BDS toxins, which shift the V1/2 of the steady-
state activation curve by 10–20 mV to more positive
potentials (Yeung et al. 2005), and don’t induce a significant
change in the slope factor (1 mV).
The gambierol, belonging to the group of ciguatera
toxins, is active on both voltage-gated sodium and
potassium channels with different potencies (Perez et al.
2012). It inhibits Kv3.1 channels in a potent and reversible
manner, by stabilizing the closed state of the channel,
which results in a ‘‘loss of function’’ (Kopljar et al. 2009).
AahG50 increases the activation rate decay, s is 70.9 ms
instead of 43.5 ms, but the slowing down is not regular and
reaches a steady state at ?20 mV. Following the study of
the voltage-dependent inhibition of IKv3.1 by AahG50 at
different concentrations, we noted some differences. In
fact, at lower concentrations the inhibition increases
gradually with voltages. At higher concentrations, the
voltage-dependence is clearly marked in the range of -20
to ?10 mV, corresponding to the beginning of current
activation. From ?10 to ?40 mV, the inhibition produced
by AahG50 demonstrates a low degree of inhibition,
despite Kv3.1 being fully activated at this voltage range.
Sung and colleagues have explained this behavior in
presence of fluoxetine as a consequence of the effects of
the transmembrane electrical field on the interaction
between fluoxetine and Kv3.1 (Sung et al. 2008). Given
that the presence of several neurotoxins in AahG50 doesn’t
allow concluding the mode of interaction with Kv3.1, the
biochemical purification program for isolating the active
molecule is settled up.
Like fluoxetine, the psoralen inhibits Kv3.1 channel
without modifying the kinetics of current activation (Sung
et al. 2009). The psoralen-induced inhibition is voltage-
dependent with a steep increase over the voltage range of
channel opening. However, the inhibition exhibits voltage
independence over the voltage range, in which channels are
fully activated (Sung et al. 2008) reminding the AahG50
effect. Besides, AahG50 is also able to reduce Shaker
potassium current Kv1.1 and Kv1.3 subtypes with more
potency. At 10 lg/ml, AahG50 inhibits 27 % of IKv3.1 but
83.9 % of IKv1.1 and 70.4 % of IKv1.3. We have previously,
characterized two toxins; KAaH1 and KAaH2. KAaH1
inhibits Kv1.1 and Kv1.3 channels with IC50 of 5 and 50 nM
respectively, while KAaH2 (100 nM) blocks 20 % of Kv1.1
and is inactive on Kv1.3. Interestingly, 100 nM of each toxin
was applied on Kv3.1. They both neither affected the current
amplitude nor the kinetics. This observed results parallel
reported data by Cotton et al. (1997), that Shaker-related Kvl
channels are equally affected by Bunodosoma granulifera
(BgK) (Kd = 6 nM for Kvl.1, 15 nM for Kv1.2, 10 nM for
Kv1.3), while Kv3.1 is insensitive up to 0.125 lM toxin
Commonly, compounds are considered as potential
pharmacological tools when they are active at a standard
concentration level. In fact, they lack their efficiency at
high concentrations and could be toxic. We therefore
deduced that AahG50, contains an other active component
on Kv3.1 channels different from KAaH1 and KAaH2,
previously described. When isolated, this component
should be tested on Kv1.1 and Kv1.3.
Fig. 5 a Current traces following the same protocols as Fig. 2 are
shown in the absence and in the presence of 100 nM of KAaH1
(upper panel) and KAaH2 (lower panel). The protocol used for
currents recordings is represented in the figure. b Histograms
representing the effect of 100 nM of KAaH1 (n = 3) and KAaH2
(n = 8) on Kv3.1 currents at ?20 mV
Inhibition of human Kv3.1 current
123
According to our results, we could consider that this
component is able to inhibit IKv3.1, by blocking the
channel pore without affecting its conformation. As sug-
gested for psoralen, the block of Kv3.1 by AahG50 may
have significant pharmacological relevance to its possible
anticonvulsant activity (Sung et al. 2009).
Evidently, biochemical purification and characterization
of such toxin in scorpion venom would be useful not only
to carry on structure–function relationship studies, but
should enhance the development of new therapeutic tools
for the treatment of a variety of neurodegenerative diseases
including Kv3.1 channel hyperactivity.
Acknowledgments Thanks are addressed to Professor Hechmi
Louzir, General Director of Pasteur Institute for constant encour-
agements. The authors thank Dr. Zakaria Belasfer, for taking care of
animals and providing us venom; Thouraya Chagour, for venom fil-
tration. Dr. Romain Guinamard, Professor in the University of Caen,
for his valuable remarks and Salaheddine Mnasri for English cor-
rections. This work was supported by Pasteur Institute, the Ministry of
Public Health and the Ministry of Research and Development (lmvt).
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