| Literature DB >> 26909041 |
Chimeglkham Banzrai1, Hiroyuki Nodera1, Toshitaka Kawarai1, Saki Higashi1, Ryo Okada1, Atsuko Mori1, Yoshimitsu Shimatani1, Yusuke Osaki1, Ryuji Kaji1.
Abstract
This study aimed to characterize the excitability changes in peripheral motor axons caused by hindlimb unloading (HLU), which is a model of disuse neuromuscular atrophy. HLU was performed in normal 8-week-old male mice by fixing the proximal tail by a clip connected to the top of the animal's cage for 3 weeks. Axonal excitability studies were performed by stimulating the sciatic nerve at the ankle and recording the compound muscle action potential (CMAP) from the foot. The amplitudes of the motor responses of the unloading group were 51% of the control amplitudes [2.2 ± 1.3 mV (HLU) vs. 4.3 ± 1.2 mV (Control), P = 0.03]. Multiple axonal excitability analysis showed that the unloading group had a smaller strength-duration time constant (SDTC) and late subexcitability (recovery cycle) than the controls [0.075 ± 0.01 (HLU) vs. 0.12 ± 0.01 (Control), P < 0.01; 5.4 ± 1.0 (HLU) vs. 10.0 ± 1.3 % (Control), P = 0.01, respectively]. Three weeks after releasing from HLU, the SDTC became comparable to the control range. Using a modeling study, the observed differences in the waveforms could be explained by reduced persistent Na(+) currents along with parameters related to current leakage. Quantification of RNA of a SCA1A gene coding a voltage-gated Na(+) channel tended to be decreased in the sciatic nerve in HLU. The present study suggested that axonal ion currents are altered in vivo by HLU. It is still undetermined whether the dysfunctional axonal ion currents have any pathogenicity on neuromuscular atrophy or are the results of neural plasticity by atrophy.Entities:
Keywords: axonal excitability; disuse atrophy; ion channels; persistent sodium current; threshold tracking
Year: 2016 PMID: 26909041 PMCID: PMC4754663 DOI: 10.3389/fphys.2016.00036
Source DB: PubMed Journal: Front Physiol ISSN: 1664-042X Impact factor: 4.566
Figure 1The waveforms of axonal excitability studies. The data are shown as mean ± standard error of the mean [filled circles = hindlimb unloading (HLU) (N = 14): open circles = control (N = 10)]. The mean amplitude of the compound muscle action potential (CMAP) in the HLU group was approximately half of the control group (P = 0.03) and tended to require stronger currents (A). The relative slopes of the current-response curves were similar (B). The waveforms of threshold electrotonus and current/threshold relationship (I/V) were similar (C,E). Strength-duration time constant (SDTC) was smaller in the HLU group than in the control (P < 0.01) (D, the intercept with the x-axis, arrow). Recovery cycle showed smaller late subexcitability in the HLU group (F, arrow).
The parameters of the motor conduction and the excitability study.
| CMAP amplitude (mV) | 2.2 ± 1.3 | 4.3 ± 1.2 | |
| Peak latency (ms) | 1.9 ± 0.1 | 2.1 ± 0.1 | 0.12 |
| Stimulus for 50% maximum amplitude | 0.55 ± 1.2 | 0.52 ± 1.1 | 0.8 |
| TEd (10–20 ms) | 44.0 ± 1.8 | 44.5 ± 0.8 | 1.0 |
| TEd (40–60 ms) | 39.0 ± 1.2 | 38.8 ± 0.5 | 0.7 |
| TEd (90–100 ms) | 37.8 ± 1.4 | 37.4 ± 0.7 | 0.4 |
| TEh (10-20 ms) | −60.3 ± 2.0 | −58.7 ± 1.0 | 0.5 |
| TEh (20–40 ms) | −66.1 ± 2.6 | −63.9 ± 1.4 | 0.4 |
| TEh (90–100 ms) | −65.9 ± 3.0 | −59.5 ± 1.7 | 0.1 |
| S2 accommodation | 6.5 ± 1.2 | 7.2 ± 0.8 | 0.4 |
| TEh (peak: −70%) | −153.9 ± 8.0 | −154.8 ± 5.0 | 0.9 |
| S3 accommodation (−70%) | 29.9 ± 4.5 | 32.5 ± 2.4 | 1.0 |
| Relative refractory period | 3.3 ± 1.1 | 2.7 ± 1.0 | 0.4 |
| Refractoriness at 2 ms | 21.3 ± 5.1 | 31.1 ± 5.3 | 0.2 |
| Superexcitability (%) | −1.9 ± 0.7 | −0.7 ± 0.3 | 0.2 |
| Late subexcitability (%) | 5.4 ± 1.0 | 10.0 ± 1.3 | |
| Resting I/V slope | 0.85 ± 0.02 | 0.91 ± 0.02 | 0.15 |
| Minimum I/V slope | 0.46 ± 0.04 | 0.44 ± 0.01 | 0.6 |
| Hyperpolarizing I/V slope | 0.53 ± 0.04 | 0.54 ± 0.02 | 0.9 |
| Strength-duration time constant | 0.075 ± 0.01 | 0.12 ± 0.01 | |
CMAP, compound muscle action potential. Significant values are underlined.
Figure 2Modeled effects on multiple excitability tests by changing one of the relevant excitability parameters listed in Table 2 (original control waveforms in dashed line). Waveforms in solid line were based on the optimized excitability parameters for the HLU animals as shown in Table 2.
Figure 3Modeled gating property and currents of persistent Na. Voltage-dependent open fractions of m23 gates are comparable between the control (the left panel) and the HLU group (the right panel), whereas the nodal currents are significantly smaller in the HLU group than the controls. Vertical lines indicate modeled resting potentials.
Figure 4Quantification of RNA of the SCA1A and SCN2A showed a tendency of lower expression of SCA1A in the HLU group than in the control subjects, whereas the expression of SCA2A were similar between the groups.
| PNaP (%) | 0.014 (0.30) | GBB | 52.5 (46.5) | 33.4% |
| PNaP (%) | 0.005 (0.30) | IPumpNI | −0.019 (−0.049) | 30.9% |
| GKsI | 1000 (272) | GBB | 80.4 (46.5) | 18.6% |
| PNaP (%) | 0.04 (0.30) | GLkN | 13.9 (1.8) | GBB | 64.5 (46.5) | 80.3% |
| PNaN | 3.8 (6.85) | GLk | 30.5 (7.3) | GBB | 76.9 (46.5) | 53.8% |
| PNaP(%) | 0.04 (0.3) | GH | 55.5 (33) | GBB | 58.6 (46.5) | 31.8% |
GBB, Barrett-Barrett conductance; GH, Internodal H conductance; GKsI, Max. internodal conductance of slow K.