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Department of Physiology and Biophysics, University of Colorado Health Sciences Center at Fitzsimons, Aurora, Colorado
Submitted 12 October 2004; accepted in final form 25 January 2005
| ABSTRACT |
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| INTRODUCTION |
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A classic system for multilevel analysis of neuronal excitability at early stages is the developing spinal cord of the Xenopus embryo. For this system, several lines of evidence implicate transcriptional mechanisms in developmentally regulated changes in excitability. For example, the duration of the action potential shortens as neurons mature (Baccaglini and Spitzer 1977
; Spitzer and Lamborghini 1976
). This developmentally regulated change in excitability requires upregulation of voltage-gated potassium current (IKv) that in turn requires new transcription (Ribera and Spitzer 1989
). Even in this system, however, there is evidence for posttranslational control of IKv (Blaine et al. 2004
).
Several different types of neurons increase sodium current density during early developmental stages (Alessandri-Haber et al. 1999
; Baines and Bate 1998
; Dourado and Dryer 1992
; Gao and Ziskind-Conhaim 1998
; Gottmann et al. 1991
; Huguenard et al. 1988
; MacDermott and Westbrook 1986
; McCobb et al. 1990
; Nerbonne and Gurney 1989
; O'Dowd et al. 1988
; Ribera and Nüsslein-Volhard 1998
; Schmid and Guenther 1998
; Skaliora et al. 1993
). Despite the critical role that sodium current (INa) plays in generation of rapid signaling in the nervous system, little is known about mechanisms that regulate expression and function of this current during early stages of neuronal development. Some studies support the notion that increases in the numbers of early expressed sodium channels underlie the dramatic upregulation that is frequently observed in embryonic neurons (Dourado and Dryer 1992
; Gao and Ziskind-Conhaim 1998
; MacDermott and Westbrook 1986
; Nerbonne and Gurney 1989
). However, other studies indicate that changes in either time- or voltage-dependent properties of sodium channels occur (Huguenard et al. 1988
; Schmid and Guenther 1998
; Skaliora et al. 1993
). At a molecular level, the latter findings raise the possibility that different channel classes appear and/or that channels undergo posttranslational modifications at later developmental stages.
Electrophysiological analysis of the zebrafish macho (mao) mutant indicates that several different classes of sensory neurons fail to undergo developmental upregulation of sodium current. Retinal ganglion cells have much reduced sodium current densities and consequently fail to show an activity-dependent pruning of connections in the tectum (Gneugge et al. 2001
). RohonBeard (RB) mechanosensory spinal neurons fail to upregulate sodium current density and consequently do not fire overshooting action potentials that are required for generation of the behavioral response to touch (Ribera and Nüsslein-Volhard 1998
). Recently, the identities of sodium channel
-subunit (Nav1) genes expressed in zebrafish RB cells have been elucidated (Novak and Ribera 2004
). This molecular information combined with the mao mutant provide powerful tools for dissection of mechanisms regulating sodium current maturation in RB cells.
Our studies reveal that 2 different sodium
-subunit genes contribute to RB INa. One of these, Nav1.6, underlies current in all RB cells. In contrast, the other, Nav1.1, contributes to current in only a subset of cells. Further, the consequences of elimination of each subunit vary during development. Elimination of Nav1.1 has greater effects at earlier stages, whereas knockdown of Nav1.6 eliminates more current in neurons of older embryos. Elimination of each subunit also selectively allows in vivo examination of developmental regulation of specific INa components. These latter studies indicate that both changes in the number of channels as well as their properties occur during differentiation of zebrafish RB cells.
| METHODS |
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Three different wild-type strains were used: Tü, WIK, and PS (the latter strain was from a local pet store). Similar results were obtained with all strains. Adult fish were housed at 28°C in the fish facility of the UCHSC Center for Animal Laboratory Care. Embryos were obtained by pairwise crossing of adults. The mao line was kindly provided by Dr. Hans-Georg Frohnhöfer of the Tübingen Stockcenter. The ethynitrosourea-induced mutation was created in the Tü strain (Granato et al. 1996
; Haffter et al. 1996
). Macho (mao) mutant zebrafish embryos were obtained from matings of identified heterozygous carriers. Typically, a subset of embryos in a clutch was sorted at the earliest time the phenotype appeared [about 30 h postfertilization (hpf)]. The identification of an embryo as mutant or sibling was reconfirmed just before dissection and recording. Staging was done according to the criteria of external morphology as described by Kimmel et al. (1995)
.
Morpholino design and microinjection
Antisense oligonucleotide morpholinos (MOs) for sodium channels Nav1.6 (MO1.6) and Nav1.1 (MO1.1) were designed and synthesized by GeneTools (Corvalis, OR). The MO1.6 and MO1.1 sequences were 5'-gggTgCAgCCATgTTTTCATCCTgC-3' and 5'-CgCCATT-TTCTCATCCTgAAgCT-3', respectively. Similar results were obtained with MOs that targeted sequences that were upstream or downstream of those above (MO1.6: 5'-gCAAgAAggggTgCAgCCATgTTTT-3'; MO1.1: 5'-TCAgAgTgATCCgCTACAC-3'). For each Nav1 MO, control MOs were synthesized by introducing mismatches at 5 positions. Stock MO solutions were prepared by resuspending the oligonucleotide in sterile filtered water (5 mM), and aliquots were stored at 80°C. Working MO solutions (1.003.30 mg/ml) were prepared by dilution with 1 x Danieau solution [58 mM NaCl, 0.7 mM KCl, 0.4 mM MgSO4, 0.6 mM Ca(NO3)2, 5.0 mM HEPES, pH 7.6] containing 1% Fast Green or 300 mM rhodamine-conjugated dextran (10,000 MW; Molecular Probes, Eugene OR). MOs were microinjected using a gas-driven PLI-100 injection apparatus (Medical Systems, Greenvale, NY) into the yolk sac of one-cellstage wild-type zebrafish embryos (Nasevicius and Ekker 2000
). At 15 min after injection, the embryos were examined and those that had Fast Green or rhodaminedextran within animal cells were transferred to a petri dish containing embryo medium (130 mM NaCl, 0.5 mM KCl, 0.02 mM Na2HPO4, 0.04 mM KH2PO4, 1.3 mM CaCl2, 1.0 mM MgSO4, 0.4 mM NaH2CO3) and then raised at 28°C until the desired developmental stage. For all experiments, embryos were manually dechorionated at 1624 hpf. Embryos that were injected with MO1.6 or MO1.1 are referred to as 1.6 or 1.1 morphants, respectively.
Semi-intact preparations of spinal cord from zebrafish embryos
Semi-intact preparations of zebrafish embryos were prepared as described previously (Ribera and Nüsslein-Volhard 1998
). Briefly, in the presence of Ringer solution (145 mM NaCl, 3 mM KCl, 1.8 mM CaCl2, 10 mM HEPES, pH 7.2) containing 0.02% tricaine, embryos were mounted on glass coverslips using Vetbond tissue adhesive (3M Animal Care Products, St Paul, MN). Once mounted, embryos were killed by transection at the level of the hindbrain. The skin was removed using dissection needles. Tricaine was then removed by washing the preparation with
40 ml of recording solution over the course of 15 min. Preparations were viewed with differential interference contrast optics on an Axioskop FS microscope (Zeiss) at a magnification of 640x.
Conventional whole cell and nucleated-patch recordings
Current- and voltage-clamp recordings were obtained using conventional whole cell and nucleated-patch configurations. Experiments were performed using an Axopatch 200B patch-clamp amplifier (Axon Instruments, Foster City, CA) in conjunction with a Digidata 1322A (Axon Instruments) analog-to-digital (A/D) interface. The pCLAMP8 software package (Axon Instruments) was used for data acquisition and analysis. Recordings were conducted at room temperature (2022°C). Unpolished electrodes with tip resistances ranging between 2.5 and 3.5 M
were fabricated from borosilicate glass using a P-97 FlamingBrown micropipette puller (Sutter Instruments, Novato, CA). Cell capacitance and series resistance were routinely compensated by 7580% with a lag of 10 µs using the electronic features of the amplifier. Currents were filtered at 5 kHz and digitized at 25 kHz. Passive leak and capacitative transients were subtracted on-line using a P/8 protocol (Armstrong and Bezanilla 1977
).
After establishment of the whole cell configuration, nucleated patches were formed (Sather et al. 1992
). Briefly, mild suction was applied to the recording pipette. Then, the pipette was slowly raised, thereby pulling the RohonBeard soma out of the neural tube. Seal resistance was closely monitored as the pipette was raised. Electronic compensation of series resistance and cell capacitance were adjusted as necessary. Typically, after achieving the nucleated-patch configuration, seal resistances and cell capacitances decreased by approximately 520% versus the whole cell configuration. Nucleated-patch recordings were continued when the following criteria were met on-line: 1) input resistances >1 G
and 2) monoexponential decay of the whole cell capacitance transient.
For recording of voltage-gated sodium currents (INa), the bath solution consisted of 127 mM NaCl, 20 mM TEA-Cl, 3 mM KCl, 10 mM CoCl2, and 10 mM HEPES, pH 7.2. [To determine the extent to which series resistance errors might be affecting currents recorded from RBs with large sodium current (e.g., those from 48 hpf wild-type embryos as in Fig. 2), some recordings were done with reduced extracellular sodium concentration of 30 and 80 mM using N-methyl-glucamine to maintain osmolarity.] The pipette solution contained: 125 mM CsCl, 12 mM NaCl, 10 mM EGTA, and 10 mM HEPES, pH 7.2. Inward sodium currents were evoked from a holding potential of 80 mV by 160-ms depolarizing voltage steps to potentials ranging between 60 and +60 mV in 5- to 10-mV increments.
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For recording of voltage-gated potassium current IKv, the bath solution contained 80 mM NaCl, 3 mM KCl, 5 mM MgCl2, 10 mM CoCl2, 5 mM HEPES, 1 µM tetrodotoxin (TTX; Calbiochem, La Jolla, CA), pH 7.4. The pipette solution consisted of (in mM): 135 mM KCl, 10 mM EGTA, 10 mM HEPES, pH 7.4. Neurons were held at 80 mV and stepped to potentials ranging between 60 and +40 mV in 10-mV increments for 60 ms. IKv amplitudes were measured by averaging values during a 10-ms interval at the end of the depolarizing pulse.
Analysis of data
Statistical analysis was performed using JMP v5.0 software (SAS Institute). Results are presented as means ± SE. Statistical comparisons were done using either the Student's t-test or, for comparisons of multiple groups, ANOVA. Statistical significance was identified by values of P
0.05.
| RESULTS |
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Previously, recordings were obtained from RB cells in situ in preparations of the developing spinal cord (Ribera and Nüsslein-Volhard 1998
). However, the long axonal processes of RB cells led frequently to space-clamp problems that precluded detailed biophysical examination of the voltage-dependent properties of INa. In this study, we avoided this difficulty by creating nucleated patches from RB cells in intact preparations. To form a nucleated patch, we first established the conventional whole cell configuration (Hamill et al. 1981
). Next, we isolated the soma from the processes by lifting the cell body out of the spinal cord (Fig. 1; Sather et al. 1992
). The formation of the nucleated patch resulted in a more compact spherical cell body geometry that avoided space-clamp problems and improved control of membrane voltage. In addition, the use of nucleated patches focused our study on currents present in or near the vicinity of the soma.
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We recorded INa from RB nucleated patches excised from embryos at 3 developmental stages: 1618 (16), 2426 (24), and 4850 (48) hpf (Fig. 2). At all stages, the reversal potential (Erev) was about 46 mV, close to the calculated value of ENa.
Peak INa amplitude increased almost 6-fold between 16 and 48 hpf (16 = 519 ± 64, n = 9; 24 = 1,080 ± 123, n = 14; 48 = 2,930 ± 235, n = 14; 24 or 48 vs. 16 hpf: P < 0.001; Fig. 2B). In RB cells of older embryos, INa peak amplitude was elicited at more negative voltages (Fig. 2C). Between 16 and 24 hpf, there was a 10-mV shift in the observed voltage that elicited peak amplitude (16 = 0.01 ± 0.001 mV; 24 = 10.0 ± 0.01 mV). Because current amplitudes also increased during this period, the shift may have reflected voltage errors arising from series resistance. To examine this possibility, we carried out some recordings in the presence of lower concentrations of external sodium to reduce current amplitudes and resultant series resistance voltage errors. Even under these conditions, developmental shifts in voltage activation were observed (Table 1; Fig. 4B).
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In anamniote vertebrates, RB cells constitute a transient population of mechanosensory neurons whose function is later assumed by dorsal root ganglion neurons (Clarke et al. 1984
). Mammalian dorsal root ganglion neurons display a substantial INa component that is resistant to the blocker TTX (Kostyuk et al. 1981
; for review, see McCleskey and Gold 1999
). However, RB INa was completely abolished at 300 nM TTX, a concentration that spares TTX-resistant current (Blair and Bean 2002
; Fig. 3).
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To examine voltage-dependent properties of activation more directly, we calculated conductancevoltage relationships (Fig. 4). Statistically significant 5- to 6-mV negative shifts in the midpoint of activation were observed between each developmental stage (16 = 16.2 ± 0.9 mV; 24 = 21.9 ± 1.0 mV; 48 = 27.4 ± 1.1 mV; P < 0.001; Fig. 4, A and B). To minimize voltage errors arising from series resistance that would be most significant for RB cells from 48 hpf embryos, we also performed some recordings under conditions of reduced extracellular sodium (30 and 80 mM; see METHODS). In the presence of 30 mM external sodium, INa recorded from RB neurons of 48 hpf embryos had peak amplitudes (433 ± 71 pA, n = 4) similar to those recorded at 16 hpf (519 ± 64 pA, n = 9). Further, we found that, even under conditions of reduced external sodium, the V1/2 of activation was shifted to more positive values (80 mM Na+: 26.5 ± 3.0 mV, n = 4; 30 mM Na+: 27.6 ± 0.3 mV, n = 4) and thus not different from that obtained under control conditions (Table 1).
In addition, the slope factor k also decreased significantly at each developmental stage, reflecting the steeper dependency on voltage for INa activation in nucleated patches formed from RB cells in older embryos (16 = 6.0 ± 0.2 mV; 24 = 4.8 ± 0.3 mV; 48 = 3.8 ± 0.4 mV; Fig. 4, A and B; P < 0.01).
Between 16 and 24 hpf, the time to peak current decreased. However, the time to peak did not show further changes at 48 hpf (in milliseconds at 30 mV: 16 = 0.96 ± 0.01; 24 = 0.42 ± 0.01; 48 = 0.44 ± 0.02; P < 0.001; Fig, 4C). The changes in time to peak that occurred between 16 and 24 hpf could have resulted from changes in either activation or inactivation, as discussed in the following text.
Developmental regulation of voltage-dependent properties of inactivation of RB INa
We used a standard protocol to examine steady-state inactivation (Fig. 5). In contrast to V1/2 of activation, the half-inactivation potential for INa remained relatively constant during the developmental period examined (16 = 49.7 ± 0.9 mV; 24 = 51.9 ± 1.0 mV; 48 = 52.8 ± 0.8 mV; Fig. 5, A and B). However, the absolute value of the slope factor k increased between 16 and 24 hpf (2.3 ± 0.4 vs. 7.2 ± 0.2 ms, P < 0.0001). No further changes were noted at 48 hpf (7.1 ± 0.2 ms). This change in k reflected the less-steep dependency on voltage of steady-state inactivation of INa recorded from RB cells of older embryos (Fig. 5, A and B).
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These data suggested that changes in fast inactivation could have contributed to decreases in the time to peak observed between 16 and 24 hpf at voltages
10 mV, potentials at which the largest changes were observed. However, at voltages positive to 0 mV, the increase in
between 16 and 24 hpf opposes the observed decrease in time to peak (Fig. 4C). Thus the data support changes in both activation and inactivation rates of INa between 16 and 24 hpf.
The time course of recovery from inactivation was examined at each developmental stage using a standard double-pulse protocol (Fig. 5D). At the 3 stages examined, recovery from inactivation occurred with similar time courses. The current recovered 50% of its initial amplitude within about 2 ms (n = 6, for each stage).
Molecular dissection of RB INa
The large changes observed in INa amplitude suggested that the density of functional sodium channels increased during this developmental period. If the upregulated channel type had properties different from those of preexisting ones, changes in voltage-dependent properties of activation and inactivation would also result. Alternatively, the observed changes in channel properties could result from posttranslational modification of channels. We used an antisense approach to explore these possibilities.
RB cells express 2 different sodium channel
-subunit genes: Nav1.1 and Nav1.6 (Novak and Ribera 2004
; Tsai et al. 2001
). We injected MO1.6, MO1.1, and control MOs and then assayed sodium currents as described above for RB cells in wild-type (WT) uninjected embryos. Control MOs had no effect on sodium current amplitude, regardless of the dose (Fig. 6A). In contrast, injection of MO1.6 or MO1.1 led to dose-dependent decreases in the amplitude of RB INa. Further, only a subset of neurons responded to injection of MO1.1 (Fig. 6B, columns in black). In contrast, all RB neurons of MO1.6-injected embryos displayed reduced sodium-current amplitudes (Fig. 6B, gray column) when compared with data obtained from control embryos (white columns).
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To get an idea of the current components that were sensitive or not to MO1.1, we compared exemplar sodium current recordings from 48 hpf control embryos to those obtained from 48 hpf MO1.1-injected embryos. Further, for this comparison, the y-axis (amplitude) was scaled so that the exemplars reflected the mean amplitudes obtained either for controls (Fig. 8A, black trace) or MO1.1-injected (Fig. 8A, green trace) embryos. For example, at 48 hpf, RB neurons of 1.1 morphant embryos displayed an average 25% reduction in sodium current amplitudes when compared with stage-matched WT embryos (1. 8 ± 0.2 vs. 2.9 ± 0.2 nA; P < 0.001; Fig. 8A). Thus the MO1.1-resistant current trace (Fig. 8A, green trace) was scaled to have an amplitude that was about 60% of that obtained from control (Fig. 8A, black trace). Then, we subtracted these 2 exemplar traces from each other to obtain a difference current that reflects the properties of MO1.1-sensitive current (Fig. 8A, red trace).
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The activation V1/2 of the MO1.1-resistant current shifted to more negative values between 24 and 48 hpf (18.1 ± 0.1 mV vs. 29.1 ± 1.6; P < 0.001; Fig. 8B). The slope value k did not show any statistically significant change (5.8 ± 0.1 vs. 5.4 ± 0.8, respectively).
The V1/2 and k for steady-state inactivation also displayed developmental differences (Fig. 8C). For example, V1/2 shifted to more negative values (24 = 50.2 ± 0.8 mV; 48 = 59.4 ± 0.6 mV; P < 0.001). The absolute value of k revealed a slight change diminishing the voltage sensitivity (6.4 ± 0.3 at 24 hpf vs. 8.2 ± 0.8 at 48 hpf; P < 0.05). In comparison to these properties, the time constant of fast inactivation of the MO1.1-resistant current displayed smaller differences between 24 and 48 hpf (Fig. 8D).
Injection of MO1.6 removed a large-amplitude, rapidly activating INa component
In contrast to the effects of MO1.1, RB neurons of 1.6 morphant embryos displayed dramatically reduced sodium-current amplitudes (Fig. 9A). The exemplar MO-resistant and MO-sensitive traces were obtained as described for Fig. 8. The MO1.6-resistant current seems to activate more slowly than did currents recorded from wild-type uninjected or control-injected embryos (Fig. 9A). For comparison, we subtracted the MO1.6-resistant sodium current from stage-matching WT INa at 10 mV. The difference current, reflecting the INa component that was sensitive to MO1.6, seemed to reach time to peak more rapidly than did control currents (e.g., Fig. 2). Further, although the majority of the resistant current inactivated rapidly, a small persistent current was observed similar to what was present in control cells (e.g., Fig. 3). In these respects, the MO1.6-difference current was similar to the MO1.1-resistant current.
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The voltage midpoint for steady-state inactivation of the MO1.6-resistant current displayed a shift toward less-negative values as development proceeded (52.1 ± 0.8 vs. 38.9 ± 1.1 mV; P < 0.05; Fig. 9C). Further, the absolute value of k changed, reflecting the observed developmental reduction in voltage sensitivity (6.8 ± 0.4 vs. 9.2 ± 0.5 mV; P < 0.05, 24 vs. 48 hpf, respectively). Additionally, a decrease in the time constant for fast inactivation was observed (Fig. 9D).
Developmentally regulated effects of MO1.1 and MO1.6
Injection of MO1.6 had substantial effects on current amplitude at all stages examined, suggesting that Nav1.6 channels underlie a large component of RB INa between 16 and 48 hpf. In contrast to MO1.6, the MO1.1 affected only a subset of RB neurons at each developmental stage examined (Fig. 10A), indicating that, at all stages examined, Nav1.1 channels were present in only a subset of RB cells.
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The time to peak of sodium current was a key developmentally regulated property of RB INa in WT embryos (Fig. 4C). Injection of MO1.6 prevented the normal developmental decrease in time to peak and the MO1.6-resistant current had times to peak that were significantly greater than those of INa in either WT or control-injected neurons (Fig. 10B). Further, the time to peak of MO1.6-resistant current resembled that of INa recorded from 16 hpf WT embryos (at 30 mV: 1.4 ± 0.1 vs. 1.0 ± 0.01 ms). In contrast, injection of MO1.1 significantly reduced the time to peak (Fig. 10B). Control MOs had no effect on the time to peak when compared with wild-type (WT = 0.44 ± 0.02; MO1.1-mis = 0.48 ± 0.08 and MO1.6-mis = 0.42 ± 0.08 ms at 10 mV). Overall, the results supported the possibility that Nav1.6 channels underlie the developmentally regulated increase in INa amplitude observed for RB neurons between 16 and 48 hpf (Fig. 2).
INa of mao mutants resembled that of 1.6 morphants and 16 hpf embryos
During development, wild-type zebrafish embryos acquire the ability to respond to tactile stimuli by 2427 hpf, displaying a stereotypical escape response (Kimmel et al. 1995
; Saint-Amant and Drapeau 2000
). However, mao homozygous mutant embryos (Granato et al. 1996
) do not acquire a touch response at 27 hpf and remain touch-insensitive thereafter. The gene harboring the mao mutation has not yet been identified. Ribera and Nüsslein-Volhard (1998)
demonstrated that RB INa of mao mutants does not undergo the developmentally regulated increase in sodium current, suggesting that a larger sodium current density was critical for acquisition of the touch response. On the basis of results we obtained using MO1.1 and MO1.6, one possibility is that mao mutants lack Nav1.6 channels. To test this possibility, we characterized the biophysical properties of RB INa in mao mutants and compared them to those of MO1.1- and MO1.6-resistant currents.
We recorded RB INa from mao mutants (/) and behaviorally unaffected siblings (+/?). RB cells of mao mutants displayed sodium currents of much smaller amplitude (0.5 ± 0.1 nA; n = 12) versus those recorded from siblings (2.0 ± 0.2 nA, n = 20; P < 0.001; Fig. 11, A and C). Further, the amplitude of INa in RB cells of mao mutants was similar to that recorded from RB cells of 16 hpf WT embryos (0.5 ± 0.1 nA; Fig. 2) and of 48 hpf MO1.6-injected embryos (0.9 ± 0.2 nA; Fig. 8). Interestingly, the average peak current amplitude recorded from RB cells of mao siblings was smaller than that recorded from WT embryos at the same developmental stage (1.8 ± 0.1 vs. 2.9 ± 0.2 nA; n = 14; P < 0.001; Fig. 11C; cf. Figs. 2 and 10). This result suggested a heterozygous phenotype that was not detected at the behavioral level. If so, because siblings represent a mixture of wild-type and heterozygous embryos, some of the current amplitudes recorded from sibling embryos (about 1/3) would be in the range of wild-type values, whereas the remainder (about 2/3) would be reduced. In fact, analysis of the INa amplitudes in mao unaffected siblings supported the existence of a heterozygous phenotype (Fig. 11D).
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Thus on the basis of current amplitude and time to peak, the possibility that mao mutants lack developmental upregulation of Nav1.6 channels is supported. Further, voltage-dependent properties of activation were similar for INa recorded from mao mutants and 1.6 morphants. However, steady-state properties of inactivation differed between mao mutants and 1.6 morphants, raising the possibility that the mao mutation has effects that cannot be accounted for by a lack of Nav1.6 channels in RB cells (Table 1).
| DISCUSSION |
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Our results reveal significant changes in the density and properties of voltage-gated sodium current in RB cells between 16 and 48 hpf (Fig. 2). Peak INa amplitude increased almost 6-fold during this period. Fast inactivation also accelerated (Fig. 5), probably contributing to the decrease in time to peak (Fig. 4). Moreover, the voltage of half-activation became more negative (Fig. 4). These changes would contribute to a developmentally regulated increase in excitability of RB cells.
To examine the molecular basis of developmental changes in INa, we used antisense morpholinos to knock down expression of protein coded for by Nav1 genes expressed in RB cells, i.e., Nav1.1 and Nav1.6 (Novak et al. 2004
). Morpholinos have proven to be highly effective and specific tools for gene inactivation (Nasevicius and Ekker 2000
). MOs have been used successfully to knock down the function of specific ion channels (Brent and Drapeau 2002
; Sidi et al. 2003
). Nonetheless, nonspecific effects can occur with their use (Nasevicius and Ekker 2000
). Our tests of specificity, however, indicated that, as used here, the Nav1.1 and Nav1.6 MOs targeted their intended sodium channel isotypes selectively and without nonspecific effects. First, we found that effects were dependent on dose (Fig. 6). For each targeted gene, we obtained similar results with 2 different MOs. Further, effects on INa but not IKv were observed. Control MOs consisting of 5 base mismatches did not affect INa. Moreover, we obtained different results both at the cellular (i.e., INa) and behavioral (Fig. 7) levels with MO1.6 versus MO1.1.
Our studies revealed that knockdown of Nav1.6 prevented the developmentally regulated increase in sodium current density, the decrease in time to peak, and negative shift in the activation V1/2 (cf. Fig. 4 and Figs. 9 and 10). These data suggest that increased expression of Nav1.6 channels constitutes a molecular basis for the developmental changes in RB INa. However, the MO1.1-resistant current, to which Nav1.6 channels presumably make the major contribution, displayed substantial changes in voltage-dependent properties between 24 and 48 hpf. These latter results suggest that in addition to increasing the number of Nav1.6 channels, developmental regulation also entails posttranslational modifications of specific channel properties, including activation and inactivation V1/2 values and the inactivation
(Fig. 9). Posttranslational modifications, such as coassembly with Nav
subunits, glycosylation, or phosphorylation of Nav1
-subunits, can modify these properties for mammalian sodium channels (Tyrrell et al. 2001
; for review, see Cantrell and Catterall 2001
; Chen et al. 2002
, 2004
). Whether these modifications occur in a developmentally regulated manner has yet to be addressed.
Our data also indicated that the relative contributions of Nav1.1 and Nav1.6 channels to RB INa change during development (Fig. 11). The effects of knockdown of Nav1.1 channels were greater in neurons of 16 hpf embryos. In contrast, MO1.6 had greater effects as development progressed. A straightforward explanation for these findings is that Nav1.1 channels are gradually replaced by Nav1.6 channels. However, because our studies were restricted to the vicinity of the soma, it is also possible that both channels are expressed to the same extent in RB neurons at all stages examined, but their subcellular distribution changes.
Between 16 and 48 hpf, RohonBeard cells provide sensory function to the embryo because dorsal root ganglion cells do not yet function. Mammalian dorsal root ganglion cells subserve different functional modalities and express multiple sodium channel genes (Benn et al. 2001
; Felts et al. 1997
). Expression of some Nav1 isotypes is indicative of a functional class of dorsal root ganglion cells (e.g., Friedel et al. 1997
). In contrast to dorsal root ganglion cells, RB cells are often considered to be a homogeneous neuronal population. Consistent with this notion, many molecular markers are expressed in all RB cells (e.g., Hu, HNK-1, P2X, acetylated tubulin; Boue-Grabot et al. 2000
; Metcalfe et al. 1990
; Svoboda et al. 2001
). However, a few molecular markers are expressed in only a subset of RB cells (TrkC, Nav1.1; Martin et al. 1998
; Novak and Ribera 2004
; Williams et al. 2000
). Between 16 and 48 hpf, we found that 2 different sodium channel types, Nav1.1 and Nav1.6, underlie sodium current in RohonBeard cells. However, knockdown of Nav1.6 affected all RB cells, whereas only a subset of RB cells were sensitive to the Nav1.1 MO. These results revealed a functional heterogeneity within the zebrafish RB cell population. These data raise the possibility that, like dorsal root ganglia, the functional diversity of RB cells allows them to subserve additional sensory modalities.
| GRANTS |
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| ACKNOWLEDGMENTS |
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| FOOTNOTES |
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Address for reprint requests and other correspondence: A. B. Ribera, Department of Physiology and Biophysics, Mail Stop 8307, University of Colorado Health Sciences Center at Fitzsimons, P.O. Box 6511, Aurora, CO 80045 (E-mail: angie.ribera{at}uchsc.edu)
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