Ion channel dysfunction causes a range of neurological disorders by altering transmembrane ion fluxes, neuronal or muscle excitability, and neurotransmitter release. Genetic neuronal channelopathies affecting peripheral axons provide a unique opportunity to examine the impact of dysfunction of a single channel subtype in detail in vivo. Episodic ataxia type 2 is caused by mutations in CACNA1A, which encodes the pore-forming subunit of the neuronal voltage-gated calcium channel Cav2.1. In peripheral motor axons, this channel is highly expressed at the presynaptic neuromuscular junction where it contributes to action potential-evoked neurotransmitter release, but it is not expressed mid-axon or thought to contribute to action potential generation. Eight patients from five families with genetically confirmed episodic ataxia type 2 underwent neurophysiological assessment to determine whether axonal excitability was normal and, if not, whether changes could be explained by Cav2.1 dysfunction. New mutations in the CACNA1A gene were identified in two families. Nerve conduction studies were normal, but increased jitter in single-fibre EMG studies indicated unstable neuromuscular transmission in two patients. Excitability properties of median motor axons were compared with those in 30 age-matched healthy control subjects. All patients had similar excitability abnormalities, including a high electrical threshold and increased responses to hyperpolarizing (P < 0.00007) and depolarizing currents (P < 0.001) in threshold electrotonus. In the recovery cycle, refractoriness (P < 0.0002) and superexcitability (P < 0.006) were increased. Cav2.1 dysfunction in episodic ataxia type 2 thus has unexpected effects on axon excitability, which may reflect an indirect effect of abnormal calcium current fluxes during development.
Episodic ataxia type 2 (EA2) is an autosomal dominant disorder caused by mutations in the CACNA1A gene, which encodes the α1A subunit of the presynaptic P/Q-type calcium channel Cav2.1 (Gancher and Nutt, 1986; Ophoff et al., 1996). The channel is widely expressed in the CNS, particularly in the cerebellum and hippocampus (Vacher et al., 2008), and in spinal motor neurons (Westenbroek et al., 1988). Large myelinated motor axons in peripheral nerve express Cav2.1 calcium channels at the presynaptic membrane at the neuromuscular junction, where, together with N-type Cav2.2 channels, they trigger action potential-evoked neurotransmitter release (Day et al., 1997), but in rodents, Cav2.1 channels are not normally expressed in peripheral axons between the cell body and the neuromuscular junction (Ousley and Froehner, 1994; Vogel and Schwarz, 1995; Plant et al., 1998). This also seems to be true for human axons (Schwarz et al., 1995; Protti et al., 1996). However, Cav2.1 channels have been reported during development in neonatal rodent optic nerve axons (‘developing central axons’), where they contribute to normal action potential propagation (Alix et al., 2008). As indicated by Alix et al. (2008), the α1A subunits that form P/Q channels are transiently clustered in the axolemma of immature axons and are expressed where the underlying vesiculotubular complex is fusing with the axolemma, including regions where development of node of Ranvier is occurring. Mutations of either the α1A subunit or the α2δ2 subunit resulted in malformed nodes of Ranvier in mice, manifesting morphologically as loss of nodal protein localization, disruption of the nodal membrane and build-up of vesicles under the nodal axolemma (Alix et al., 2008). It was hypothesized that disrupting calcium channel localization has either a ‘direct’ effect on node of Ranvier development due to a disruption in vesicle docking at the nodal axolemma, or an ‘indirect’ effect, stemming from a reduction in axonal excitability (Alix et al., 2008).
Patients with EA2 manifest an intermittent cerebellar disturbance, which can last hours to days (Jen et al., 2007). Some patients develop fixed or progressive cerebellar features, and there is an increased incidence of epilepsy in patients with EA2 (Rajakulendran et al., 2010). The condition is allelic with spinocerebellar ataxia type 6 (SCA6), and familial hemiplegic migraine type 1 (FHM1), and there may be clinical overlap between these disorders (Battistini et al., 1999; Jen et al., 1999; Kors et al., 2004). Intermittent myasthaenia-like weakness has been reported in some patients with EA2 (Jen et al., 1999). During nerve conduction studies in these patients, repetitive stimulation and voluntary contractions can produce features suggestive of variable presynaptic endplate function (Jen et al., 2001; Melzer et al., 2010), and there may be neurophysiological evidence of a disturbance of transmission across the neuromuscular junction (Maselli et al., 2003).
We have previously reported highly stereotypic changes in the excitability of motor axons in the median nerve of patients with episodic ataxia type 1 (EA1), which is caused by loss-of-function mutations of the potassium channel gene KCNA1 (Tomlinson et al., 2010). These changes in excitability are not unexpected, because the Kv1.1 subunit encoded by KCNA1 is expressed in the juxtaparanodal membrane of motor axons, and EA1 patients commonly exhibit neuromyotonia. We have also observed abnormal axonal excitability in subjects with mutations in KCNQ2 channel gene responsible for slower K+ currents. These subjects had a history of benign familial neonatal epilepsy, but were asymptomatic when studied and did not have neuromyotonia (Tomlinson et al., 2012).
The purpose of the present study was to evaluate whether EA2 patients would have changes in axonal excitability, even though calcium channels are not normally expressed in mid-axon (at the site of stimulation), and axonal function is normal in routine nerve conduction studies.
Materials and methods
Eight patients with a clinical phenotype of EA2 were studied in the UK, USA and Australia between 2007 and 2009 by the same clinician (S.T.), who performed the nerve excitability studies on patients and control subjects contemporaneously. All subjects were over the age of 18 and provided written informed consent. Ethical approval was obtained from the Joint National Hospital for Neurology and Neurosurgery/University College London Ethics Committee, The University of Rochester Ethics Committee, and the University of Sydney Human Research Ethics Committee. They were assessed clinically and, where possible, using nerve conduction studies (including repetitive stimulation), EMG, single fibre EMG, and stimulated single fibre EMG, according to a previously described protocol (Mills, 2005; Tomlinson et al., 2009). Medications were not changed for assessment. Two subjects (Subjects 3 and 5) were not taking acetazolamide at the time of clinical or neurophysiological assessment. Genomic DNA was extracted from peripheral blood leucocytes using standard procedures. Probands were screened for CACNA1A mutations [NCBI transcript NM_001127221.1 (on LRG_7)] by standard bidirectional Sanger sequencing of all coding exons and exon–intron boundaries (primer sequences available on request). Dosage analysis for CACNA1A exonic deletions and duplications was performed by multiplex ligation-dependent probe amplification (MRC).
Subsequent measurements in the protocol were based on ‘threshold tracking’, in which the current required to produce the target CMAP is referred to as a ‘threshold’ for that CMAP. Conditioning stimuli were applied to the nerve, and the change in stimulus required to produce the target CMAP response was ‘tracked’. There were three manipulations designed to measure: (i) strength-duration properties; (ii) the responses to subthreshold conditioning stimuli; and (iii) the responses to supramaximal conditioning stimuli. Each provides information about different influences on membrane potential and ion channel function.
Strength–duration measurements of nerve membrane reflect properties of the nodes of Ranvier, and can provide insight into persistent Na+ conductances active at the resting potential (Bostock and Rothwell, 1997). The measurement was made using unconditioned test stimuli of different duration (0.2, 0.4, 0.6, 0.8 and 1.0 ms). As stimulus duration increased, a smaller current was required to produce the target CMAP. Using these measurements, rheobase and the strength–duration time constant (τsd) were calculated from a plot of stimulus charge against stimulus duration.
During threshold electrotonus (TE), subthreshold polarizing currents were applied for 100 ms, and the change in threshold was tested at different times, before and during the 100 ms polarizing currents and for 100 ms afterwards. The conditioning stimuli were hyperpolarizing (TEh) or depolarizing (TEd), and were set at strengths of 20% (TEd20 or TEh20) and 40% (TEd40 or TEh40) of the unconditioned threshold current (which was monitored throughout the recording). Threshold electrotonus can provide insight into the state of membrane polarization and the activity of some voltage-dependent ion channels: nodal Na+ channels and slow K+ channels, and internodal K+ and hyperpolarization-activated, cyclic nucleotide-gated (HCN) channels (Bostock et al., 1998; Howells et al., 2012).
The current/threshold (I/V) relationship measured the change in threshold at the end of a 200 ms conditioning current, which was varied in 10% steps from 50% (depolarizing) to −100% (hyperpolarizing). The resting I/V slope is the slope of the current–threshold relationship at resting membrane potential. The minimum I/V slope is the minimum slope of the current–threshold curve. The hyperpolarizing I/V slope: slope of the current–threshold relationship for hyperpolarizing currents of −80% to −100% of threshold. These data allowed rectifying currents to be assessed; K+ currents with depolarization and inwardly rectifying HCN currents (Ih) with hyperpolarization. The slope of the I/V curve is analogous to conductance.
The recovery cycle consists of the relative refractory period (RRP, largely reflecting recovery of nodal Na+ channels from inactivation), the superexcitable period (due to the depolarizing after potential, which can be affected by the activity of fast K+ channels), and the late subexcitable period (reflecting the slowly decaying hyperpolarization following slow K+ channel activation) (Bostock et al., 1998; Burke et al., 2009; Howells et al., 2012). In the TROND protocol, the recovery cycle was measured using a supramaximal conditioning stimulus. The change in threshold was tracked at intervals up to 200 ms after the conditioning stimulus. The conditioning potential was subtracted on-line from the response to the conditioning and test stimulus pair so that accurate measurements could be made at short conditioning-test intervals.
Control data for nerve excitability studies were obtained from age-matched subjects from a database of healthy volunteers (Table 2). Statistical analysis was performed by the QTRACP software (version 23/10/2012). Differences in mean nerve excitability measures between patients and controls were assessed by Welch’s unequal variance t-test. Because we were interested in which measurements were different, rather than in whether any measurements were different, Bonferroni correction was not applied, and P < 0.05 was considered significant.
A mathematical model of axonal excitability was applied to the data generated from the studies (Bostock et al., 1995; Kiernan et al., 2005a; Jankelowitz et al., 2007; Howells et al., 2012). The means and standard deviations (SDs) of each recorded data point were evaluated for the 30 normal subjects and the eight patients. The conductances of the model were first adjusted to minimize the discrepancy between the model and the mean control recordings, where discrepancy was defined as the weighted sum of the error terms: ([xm − xn] / sn)2, where xm is the threshold of the model, xn is the mean, and sn is the standard deviation of the thresholds for the real nerves. The weights were the same for all thresholds of the same type (e.g. recovery cycle) and were chosen to give total weights to the four different types of threshold measurement: threshold electrotonus, current–threshold relation, recovery cycle, and strength–duration time constant in the ratio 4:2:2:1. As in previous modelling studies, these ratios reflect, albeit crudely, that the four threshold electrotonus traces provide more information about membrane properties than the current/threshold relationship or the recovery cycle, which in turn provide more information than the strength–duration relationship. The ‘control’ model was achieved when the discrepancy could not be further reduced by changing any of 29 parameters in the model, alone or in combination. Then, for each of the 17 parameters in the model (comprising 10 conductances, three capacitances, 15 channel gating parameters and the resting membrane potential), either alone or in combination. To explore possible explanations for the abnormal excitability properties of axons in EA2 a different strategy was used: selected model parameters were tested one at a time to see how well changes in a single parameter could account for the abnormalities. The modelling and the fitting of the model to the control and patient recordings were carried out by the MEMFIT function within the QTRACP program (version 23/10/2012).
Eight patients with genetically confirmed EA2 from five families were studied. Clinical features are summarized in Table 1. Subjects 1 and 2 were dizygotic twins. A family history of EA2 was defined in seven patients. All subjects gave a history of intermittent cerebellar dysfunction lasting hours to days, triggered by stress/emotion, intercurrent illness and vigorous exertion or sudden movement. All patients demonstrated a clinical response to acetazolamide but this was discontinued in two because of side effects (Subject 3 due to renal calculi; Subject 5 due to thrombocytopaenia). Subjects 3 and 5 were both from Family 2 and reported feeling muscle weakness in association with their ataxic episodes.
Clinical and genetic features of patients with EA2
A c.3992+1G>A p.?
Onset age 6. Up to 4 episodes/week. Subtle interictal cerebellar findings.
Onset age 6. Up to 4 episodes a month. Normal interictal exam.
B c.5137–10_–2delAATTCCACA p.?
Onset age 7. Up to 4 episodes/week. Minor interictal cerebellar findings. Acetazolamide ceased due to renal calculi.
Onset age 4. Up to 4 episodes/week. Normal exam.
Onset age 8. Up to 2 episodes/week. Normal exam. Acetazolamide ceased due to thrombocytopaenia.
C c.3695+1G>A p.?
Onset age 6. Up to 4 episodes/month. Minor interictal cerebellar findings.
D c.5455C>T p.Arg1819*
Onset age 5 when started sports. Up to 2 episodes/week. Requires 4-AP in addition to acetazolamide.
E c.835C>T p.(Arg279Cys)
Onset age 5. Normal interictal exam. Requires dichlorphenamide and topirimate in addition to acetazolamide.
Nerve conduction studies and EMG were performed in six of eight subjects. No significant abnormalities were detected on concentric needle EMG, nerve conduction or on repetitive stimulation of motor nerves at various rates. However, increased jitter was demonstrated on single fibre EMG (Fig. 1A) in Subjects 3 and 5 from Family 2, both of whom reported weakness during attacks. In addition, Subject 5 (in Family 2) had increased jitter with blocking on stimulated single fibre EMG, which was maximal at low stimulation rates (2–5 Hz; Fig. 1B). These findings demonstrate instability of neuromuscular transmission in these subjects.
Single-fibre EMG studies in EA2. (A–C) Increased jitter with blocking in Subject 5 (Family 2). (A) Superimposed traces of single fibre EMG during recordings during voluntary contraction demonstrating increased jitter, reflecting instability of the neuromuscular junction. (B and C) Same recording displayed in raster mode showing increased jitter and blocking. (D) Stimulation single-fibre EMG in EA2. Stimulation rates are 1, 2, 5, 10, 15 and 20 Hz. Maximal jitter is seen at 2–5 Hz stimulation, decreasing at higher rates, similar to the findings in Lambert-Eaton syndrome.
New mutations were found in Families A and B (Table 1). In Family A, the mutation in exon 24: c.3992+1G>A p.? affects a consensus splice donor site. The consequence of this change is not predictable but is likely to cause a skip of exon 24, which would introduce a premature stop after the inclusion of three aberrant amino acids, which in turn predicts subsequent nonsense mediated decay of the aberrant message and may prevent translation of the mRNA.
The mutation identified in Family 2 is c.5137-10_2delAATTCCACA p.?. The consequence of this change is not predictable but is likely to cause a skip of exon 34, which would introduce a premature stop after the inclusion of 20 aberrant amino acids.
Subject 6 was known to carry G to A substitution at donor splice site of exon 21 (c.3695+1G>A p.?) (Eunson et al., 2005). The consequence of this change again is not predictable, but is likely to cause a skip of exon 21, which would introduce a premature stop after the inclusion of nine aberrant amino acids.
Subject 7 carries a mutation that introduces a premature stop codon at the beginning of the C-terminus, c.5455C>T p.Arg1819*, which was not identified in his parents. This mutation has been previously reported in two unrelated patients in association with EA2, absence seizures and cognitive impairment (Jouvenceau et al., 2001; Strupp et al., 2004) albeit as Arg1820* due to a different reference sequence being used. Subject 8 carries the previously reported c.835C>T p.(Arg279Cys) mutation.
Nerve excitability studies
The mean data for subjects with EA2 and normal controls are compared in Table 2. Prominent differences were found in absolute electrical thresholds, threshold electrotonus and the recovery cycle.
For definition of excitability measurements see Glossary.
Values are mean ± SEM, except for four measurementsc.
↵at and degrees of freedom for Welch’s unequal variance t-test.
↵bP indicates probability for two-tailed test *P < 0.05, **P < 0.01, ***P < 0.001, ****P < 0.0001.
↵cValues were normalized by log conversion and given as geometric mean ×/÷ standard error expressed as a factor.
Stimulus–response and strength–duration relationship
Subjects with EA2 exhibited an increased threshold. The stimulus required to produce a CMAP 50% of the maximal response was ∼85% greater in patients than controls [listed in Table 2 as ‘Stimulus (mA) for 50% maximal CMAP’; P = 0.009].
The strength–duration data are plotted in Fig. 2A as a charge–duration plot (i.e. mA.ms versus ms). The strength–duration time constant (τsd) is given by the negative intercept of the regression line on the x-axis, and the rheobase is given by the slope of the regression line. The τsd was not significantly different (Figs 2A and 3A), but mean rheobase (i.e. threshold current for very long stimulus pulses) was nearly twice as high in the affected individuals (Table 2), and in four of eight cases was outside the 95% confidence limits for the normal controls (Fig. 3B). This is consistent with the increased threshold for activation, noted in the previous paragraph.
Axonal excitability measurements in Subjects with EA2 compared to controls. (A) Strength–duration time constant is given by the negative intercept of the regression line on the x-axis (open arrow). Rheobase is given by the slope of the regression line (filled arrow). (B) Threshold electrotonus in patients with EA2 and control subjects. Each point is mean ± SEM. Filled circles = EA2 (n = 8). Open arrow indicates increase in TEd in patients with EA2. Black arrow indicates increase in TEh in patients with EA2. (C) The recovery cycle in EA2. The patients’ recordings are characterized by a 12% shorter relative refractory period (open arrow) and a 24% increase in superexcitability (closed arrow).
Dot plots illustrating individual data points in EA2 subjects compared to controls. (A) Strength duration time constant. (B) Rheobase. (C) Peak threshold decrease with 20% depolarizing current. (D) Threshold electrotonus with 40% hyperpolarizing current. (E) Relative refractory period (RRP). (F) Peak superexcitability in recovery cycle. NC = normal controls; NS = not significant. Asterisks indicate level of significance by Welch unequal variance t-test, as in Table 2. Note logarithmic axes in B and E to help normalize distributions. Horizontal lines indicate means (solid) and means ± standard error (dotted).
Averaged threshold electrotonus curves for the eight patients are compared to the mean for the 30 controls (Fig. 2B). These graphs depict the change in threshold during and after 100 ms subthreshold conditioning currents of ± 40% and ±20% of the unconditioned threshold current. There was a greater increase in excitability in response to depolarizing currents in the patients and a greater decrease in excitability during hyperpolarization, producing a ‘fanning out’ appearance (Nodera and Kaji, 2006). These differences are statistically significant, especially for the hyperpolarizing threshold electrotonus (Fig. 3B and D). This is illustrated for TEd20(peak) (i.e. the greatest reduction in threshold during the 20% depolarizing current) in Fig. 3C and for TEh40(90–100 ms) (i.e. the increase in threshold at the end of the hyperpolarizing current, which is 40% of threshold) in Fig. 3D.
The current–threshold relationship (Supplementary Fig. 1A) measures the changes in threshold at the end of 200 ms currents, varied in strength from 50% of threshold to −100% of threshold. Because threshold is closely related to membrane potential, this plot is a threshold analogue of a current–voltage curve (Kiernan et al., 2000). Similarly, the slope of this curve is a threshold analogue of input conductance, designated ‘IV slope’ in Fig. 1B. There were only modest differences between the subjects with EA2 and controls (Table 2).
The excitability changes following supramaximal stimulation are compared for the patients with EA2 and control subjects in Fig. 2C. The patient recordings were characterized by a 13% shorter relative refractory period (white arrow) and a 30% greater superexcitability (black arrow). These differences are statistically significant (Fig 3E, F and Table 2), but there was no significant difference in late subexcitability.
After optimizing its parameters (see ‘Materials and methods’ section), the model fitted the control data with a residual discrepancy of 0.063. The discrepancy between this control model and the mean EA2 axonal excitability data was 1.15. To explore whether, for example, a change in fast potassium channels could account for this discrepancy, we determined the best reduction in discrepancy that could be achieved by changing the fast potassium conductance at nodes, internodes, or by making the same relative change in both. The discrepancy reductions for these changes are listed in Table 3 and were only 23.0, 22.3 and 23.9%, respectively, so they could not provide a convincing explanation for the altered excitability. Table 3 also lists the best discrepancy reductions achieved by changing the 13 other conductances, and also by changing the three capacitances in the model, the resting membrane potential, and also the half-activation voltage of the HCN channels. This membrane property is sensitive to intracellular cyclic nucleotides and other metabolic factors and most likely accounts for much of the variability in nerve excitability properties between normal subjects, and the changes in inward rectification reported in some pathologies (Jankelowitz et al., 2007; Lin et al., 2008;Howells et al., 2012). Interestingly, the most appropriate changes in the model, resulting in a 73% reduction in discrepancy were made not by changes in any ion channel, but by increasing the Barrett-Barrett conductance (the conductance of the multiple pathways between the internodal axolemma and the exterior of the nerve fibre; see Barrett and Barrett, 1982). Figure 4 illustrates the excitability curves generated by the control model and by the model for patient data. The control results are in grey and the patient results in black, with the recorded data shown in circles and the output of the model by continuous lines. For the patient data the modelled change was a 13.7% increase in the Barrett-Barrett conductance. The differences in excitability waveforms resemble those seen in the recordings from controls and patients in Fig. 2. For completeness, we also computed the best discrepancy reductions achievable by altering the remaining 14 channel gating parameters in the model (which are not listed in Table 3, as there was no reason to suspect they might be involved in EA2), but none of them reduced the discrepancy by more than 31%.
Modelling possible explanations of altered nerve excitability properties in EA2.
Best fit value
Discrepancy reduction (%)
Resting potential (altered by applied current)
Internodal leak conductance
Nodal and internodal leak conductances (rel)
Nodal leak conductance
HCN channel half-activation voltage
Slow potassium conductances (rel)
Nodal slow potassium conductance
Fast potassium conductances (rel)
Nodal fast potassium conductance
Internodal fast potassium conductance
Persistent sodium permeability (% transient)
HCN channel conductance
Transient sodium permeability
Internodal slow potassium conductance
Capacitance internodal axon
List of best fits to the EA2 patient nerve excitability data made by changing a single parameter in the model first fitted to the normal control data. For example, increasing the Barrett-Barrett conductance from 36.5 to 41.5 nS reduces the discrepancy between the model and the EA2 data from 1.15 to 0.311, a reduction of 73%. The parameters designated ‘(rel)’ are factors applied to both nodal and internodal conductances of the same type.
Difference between control and EA2 nerve excitability modelled as an increase in Barrett-Barrett conductance. The control results are in grey and the patient results in black, with the recorded data shown in circles and the output of the model by continuous lines. For the patient data the modelled change was a 13.7% increase in the Barrett-Barrett conductance. (A) Threshold electrotonus. (B) Recovery cycle. (C) Current/threshold reduction curve. (D) I/V slope.
The present study has revealed disturbed excitability of motor axons in eight subjects with genetically confirmed EA2, with changes that can be modelled by an increase in shunt conductance between the internodal axolemma and exterior.
All subjects reported the onset of characteristic attacks of cerebellar dysfunction lasting hours to days from childhood. Two subjects from one kindred described myasthenic-type weakness during attacks. All subjects experienced a clinical response to acetazolamide though this was incomplete in two. It could be anticipated that acetazolamide would have affected measures of axonal excitability, but this is unlikely to be significant at clinical dosages. It is therefore important that the studies in the two patients not taking acetazolamide did not differ significantly from those taking the medication at the time of the study. Three of eight subjects had subtle fixed cerebellar signs between attacks. Cerebellar ataxia is consistent with dysfunction of central synapses; however, Cav2.1 is also expressed in peripheral motor axons, albeit confined to the neuromuscular junction (Vogel and Schwarz, 1995). Nevertheless, the measurements of axonal excitability at the wrist detected significant differences between the EA2 cohort and normal control subjects. The possible reasons for these altered excitability properties are discussed below.
Abnormal neuromuscular transmission in episodic ataxia type 2
Cav2.1 is highly expressed at the neuromuscular junction where it is closely associated with neurotransmitter exocytic machinery (Protti et al., 1996; Plant et al., 1998). As a result of an action potential, Cav2.1 activation facilitates calcium-dependant acetylcholine release. In the autoimmune disease Lambert-Eaton myasthenic syndrome (LEMS), antibodies directed against Cav2.1 impair presynaptic acetylcholine release producing muscle weakness. In these patients, the jitter and blocking is maximal at stimulation rates of ≤5 Hz and reduces at higher rates (Trontelj and Stålberg, 1991; Mills, 2005). The stimulated single fibre EMG findings in Subject 5 (in Family 2) closely parallel the findings in LEMS and is consistent with impaired Cav2.1 function. Repetitive activation at high frequency (e.g. 20–50 Hz) restores neurotransmission (Mills, 2005). It is not surprising therefore that similar clinical and neurophysiological findings have been reported in patients with EA2. In the recovery cycle, it is conceivable that the conditioning discharge would affect transmission at the neuromuscular junction. In patients with LEMS, this could change the test CMAP at the intervals used in the recovery cycle (>5 Hz), producing equivalent changes in threshold. However, the two patients who had abnormal stimulated single fibre EMG had no abnormalities on repetitive stimulation and their recovery cycle data were not significantly different from those of the other six patients.
Axonal excitability in episodic ataxia type 2
This paper reports alterations in the excitability properties of motor axons in the nerve trunk in patients with EA2. Acetazolamide was not discontinued prior to the study, but as noted above, the same excitability changes were seen in the two patients in whom the medication had been discontinued for medical reasons. The features seen in patients with EA2 include an increase in threshold, a shortened relative refractory period and greater threshold changes to the changes in membrane potential seen in threshold electrotonus. These abnormalities are qualitatively similar to those in EA1 (Tomlinson et al., 2010). However, some measures behaved differently, and this was not just qualitative. For example, late subexcitability was normal in EA2 (Table 2) whereas it was increased in the 20 patients with EA1, so that the difference between the two types of episodic ataxia was highly significant (EA2: 14.4 ± 0.65%; EA1: 24.1 ± 1.7%; mean ± SE, P < 0.0001, Welch test). There was greater accommodation to 40% depolarizing currents in EA1 (EA2: 15.07 ± 0.7%; EA1: 23.41 ± 1.59% P < 0.00001). Also, although superexcitability was increased in both groups, it was increased much more in EA1 (EA2: −30.39 ± 1.9%; EA1: −44.3 ± 1.8%, P < 0.0001). Low serum potassium can produce some of the features seen in EA2 (Boërio et al., 2014). These include increased threshold change to hyperpolarization in threshold electrotonus and increased superexcitability. However, low serum potassium would have also increased the threshold change to depolarization and increased late subexcitability. These changes were not seen in the EA2 cohort.
Whereas the nerve excitability changes in the EA1 subjects can be attributed directly to the loss of Kv1.1 fast potassium channels (Tomlinson et al., 2010), the same mechanism cannot be responsible for the superficially similar but less severe changes in EA2. A quantitative model of motor nerve excitability, previously used to account for the excitability changes induced by puffer fish poisoning (Kiernan et al., 2005a), showed that the single parameter change that best explained the differences between patients and controls was a 14% increase in the conductance path across and around the myelin sheath, also known as the Barrett-Barrett conductance (Barrett and Barrett, 1982) (Table 3 and Fig. 4). The modelling suggests that the altered axonal excitability arises from quite different mechanisms in EA1 and EA2, and in EA2 is more likely due to changes in Schwann cell ensheathment than in axonal ion channels. According to this interpretation, the superficial similarity in excitability changes in threshold electrotonus and in the recovery cycle arises because in each case, both applied currents and the current generated during the nerve impulse cause a greater change in the membrane potential of the internodal axon: in EA1 this is because the internodal axolemma has fewer Kv1.1 channels to resist potential change, whereas in EA2 the access resistance restricting current flow to the internodes is lower. Comparison between Fig. 4 and Fig. 2 show that there is a good correspondence between the other excitability abnormalities recorded in EA2 and the predicted effects of increasing the Barrett-Barrett conductance, supporting the high discrepancy reduction for this parameter [which at 73% was almost as great as the 75% discrepancy reduction reported by Kiernan et al. (2005a) when recordings from patients with puffer fish poisoning were modelled by a reduction in sodium channel permeability]. While this level of ‘goodness of fit’ obtained by changing the Barrett-Barrett conductance provides a strong pointer to the nature of the abnormality, it cannot prove that this pathway is involved, and to find a plausible mechanism relating this interpretation to the calcium channel defect we must look elsewhere. Such a mechanism is suggested by the report of Alix et al. (2008), who observed transient expression of α1A subunit of P/Q calcium channels along the axolemma of optic nerve axons during early neonatal development in mice. Mutation in the CACNA1A gene caused malformation of the nodes of Ranvier, with disordered localization of nodal proteins including voltage-gated sodium channels, β IV spectrin and contactin-associated protein-1 (CASPR1, encoded by CNTNAP1). If the P/Q calcium channels present in peripheral nerve axons during development have a similar role, it is likely that the changes in excitability in peripheral nerve axons described here reflect the sustained impact of nodal malformation in the early neonatal period. The mathematical modelling is consistent with this hypothesis. Interestingly, studies from infancy to adulthood by Farrar et al. (2013) have demonstrated changes in excitability that are generally consistent with those described in EA2, and were attributed to maturational changes at the axo–glial junction.
Accommodation half-time: Half-time of accommodative response to a 100 ms subthreshold depolarizing conditioning stimulus
TEd: Change in threshold in response to a subthreshold depolarising conditioning stimulus
TEh: Change in threshold in response to a subthreshold hyperpolarising conditioning stimulus
I/V: Current/voltage; the current/threshold relationship is analogous to the traditional current/voltage relationship
I/V slope: Slope of the currentthreshold relationship
Ih: Hyperpolarization-activated current (mediated by HCN channels)
In conclusion, the excitability properties of peripheral motor axons in EA2 differ significantly from those in normal controls, and also from those in EA1. The pattern of excitability changes in EA2 may result from nodal malformation in the neonatal period. As was the case with our previous study of patients recovered from benign familial neonatal epilepsy (Tomlinson et al., 2012), this study demonstrates the power of excitability studies to detect membrane abnormalities that are too subtle to produce symptoms or to be detected by routine neurophysiological studies. In addition, this study raises a further mechanism through which peripheral nerve axons can be altered in disorders that are primarily central (Kiernan et al., 2005b; Jankelowitz et al., 2007; Ng et al., 2008;Boland et al., 2009; Tomlinson et al., 2010, 2012) even when the relevant channel is not normally expressed at the site of stimulation. Indirect consequences of inherited channelopathies should be taken into account when considering the circuit consequences of the ion channel defect. However, in their recent study, Zhang and David (2016) used Ca2+ imaging to provide evidence for T-type (Cav3.x) Ca2+ channels at the node of Ranvier and L-type (Cav1.x) channels on the paranodal or juxtaparanodal membrane of myelinated motor axons of the mouse. When axons were stimulated at 50 Hz for 10 s, there was a small increase in axoplasmic [Ca2+] at the node, and this was greater when there was paranodal demyelination. They found no evidence for the involvement of Cav2.1 channels, so our conclusions are not directly affected, but it can no longer be maintained with confidence that Ca2+ channels are not present at the node of Ranvier of human motor axons.
S.T. is supported by British Medical Association Vera Down Fellowship, Charities Aid Foundation Patrick Berthould Fellowship, University of Sydney Postgraduate Award, Brain Foundation (Australia) and the National Health and Medical Research Council (Australia). RCG and CINCH studies are supported by NIH grant: 5 U54 NS 059065 and the Rochester Clinical Research Center. D.K. is supported by the Wellcome Trust. M.G.H. is supported by a MRC Centre grant and by the UCLH Biomedical Research Centre.
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