Abstract
Maturation of the peripheral nervous system requires specification of axonal diameter, which, in turn, has a significant influence on nerve conduction velocity. Radial axonal growth initiates with myelination, and is dependent upon the C terminus of neurofilament medium (NF-M). Molecular phylogenetic analysis in mammals suggested that expanded NF-M C termini correlated with larger-diameter axons. We used gene targeting and computational modeling to test this new hypothesis. Increasing the length of NF-M C terminus in mice increased diameter of motor axons without altering neurofilament subunit stoichiometry. Computational modeling predicted that an expanded NF-M C terminus extended farther from the neurofilament core independent of lysine-serine-proline (KSP) phosphorylation. However, expansion of NF-M C terminus did not affect the distance between adjacent neurofilaments. Increased axonal diameter did not increase conduction velocity, possibly due to a failure to increase myelin thickness by the same proportion. Failure of myelin to compensate for larger axonal diameters suggested a lack of plasticity during the processes of myelination and radial axonal growth.
Introduction
Specification of axonal diameter is a key component of motor neuron function as it is a major axonal property that determines the velocity of signal conduction (Rushton, 1951; Waxman, 1980). Myelination of peripheral nerve fibers is necessary for rapid impulse transmission (Huxley and Stampfli, 1949) and occurs on axons that are >1 μm (Duncan, 1934). Myelination increases conduction rates by preventing charge loss and reducing membrane capacitance (Huxley and Stampfli, 1949; Koles and Rasminsky, 1972; Rasminsky and Sears, 1972). Myelination also initiates cell biological changes in axons resulting in larger axonal diameters (de Waegh et al., 1992), which further decreases axonal resistance and contributes to increasing the rate of conduction (Hursh, 1939; Boyd and Kalu, 1979).
The large increase in axonal diameter that occurs with myelination is referred to as radial growth (Cleveland, 1996), and it is dependent upon both myelination (de Waegh et al., 1992) and neurofilaments (NFs) (Ohara et al., 1993; Zhu et al., 1997). NFs are obligate heteropolymers in vivo, and can be composed of neurofilament light (NF-L), neurofilament medium (NF-M), neurofilament heavy (NF-H) (Lee et al., 1993), and α-internexin (Yuan et al., 2006). The composition of NF heteropolymers varies with developmental stage (Shaw and Weber, 1982; Shen et al., 2010).
Gene targeting studies identified NF-M as the critical subunit required for radial growth (Elder et al., 1998) and the NF-M C terminus as the critical domain (Garcia et al., 2003). NF-M was originally thought to regulate axonal diameter through myelin-dependent phosphorylation of lysine-serine-proline (KSP) repeats (de Waegh et al., 1992; Yin et al., 1998) located within the NF-M C terminus (Levy et al., 1987; Myers et al., 1987). However, preventing NF-M KSP phosphorylation in NF-MS→A mice failed to recapitulate the reduction in radial growth of motor axons observed in NF-M C-terminally truncated mice (Garcia et al., 2003, 2009). Together, these data suggest that NF-M C terminus regulates axonal diameter by a mechanism that is independent of KSP phosphorylation.
To provide insight into the role of NF-M C terminus in regulating axonal diameter, molecular phylogenetic analyses of NF-M exon 3, which codes for NF-M C terminus, were performed across several clades of mammals (Barry et al., 2010). Sequence analysis suggested that the NF-M C terminus was divided into three subdomains, two conserved regions flanking a variable region. Sequencing also revealed that independent expansion events of NF-M C terminus occurred within multiple clades of the consensus mammalian phylogenetic tree. All observed expansion events occurred by the addition of amino acids, including KSP repeats, within the variable subdomain. Moreover, NF-M KSP repeat number and, consequently, NF-M C-terminal length correlated with axonal diameter in a subset of mammals. These data suggested that lengthening the NF-M C terminus through expansion of KSP repeat number might have resulted in larger axonal diameters during mammalian evolution. To test this new hypothesis, we have applied gene replacement and computational modeling techniques to increase the length of NF-M C terminus by replacing the endogenous NF-M C terminus and its 7 KSP repeats with the longer bovine C terminus and its 22 KSP repeats.
Materials and Methods
Generation of NF-MBovineTail mice.
All procedures were in compliance with the University of Missouri Animal Care and Use Committee and with all local and federal laws governing the humane treatment of animals. The murine nefm genomic clone was a generous gift from J. P. Julien (Laval University, Quebec City, Canada) (Jacomy et al., 1999). The 7 kb NotI-BamHI fragment of nefm genomic clone was digested with AccI to produce an ∼2.2 kb fragment that included mouse nefm Exon 3 as well as ∼500 bp of 5′ and 3′ untranslated region (UTR). Nefm bovine exon 3 and its 3′UTR were PCR amplified from bovine sperm DNA (provided as a gift by Jerry Taylor, University of Missouri) and cloned into a T-Vector. The bovine exon 3 clone was then mutagenized to introduce a BsrGI restriction site that is already present in mouse nefm exon 3. An NdeI site was introduced in the mouse nefm 3′UTR by mutagenesis that was present in the bovine nefm 3′UTR. The BsrGI-NdeI bovine fragment was cloned into the AccI-AccI mouse fragment. To make the region of exon 3 5′ to the BsrGI 100% identical to bovine exon 3, amino acid codon 414 (NCBI accession number P08553) within mouse exon 3 was mutagenized from a serine codon to an alanine codon. The AccI-AccI fragment with bovine exon 3 was then cloned back into the 7 kb NotI-BamHI fragment. Nefm 5′UTR and 3′UTR regions were amplified from mouse 129SvEv Genomic DNA to increase homology arm lengths from 5 kb to a total of 8 kb. Diphtheria toxin alpha gene with poly adenylation (DT-ApA) clone was a generous gift from Y. Yanagawa and T. Yagi (Yanagawa et al., 1999). DT-ApA was introduced at the 3′ end of the construct as a negative selection marker. Finally, the nefl 3′UTR and a PGK Neo cassette were cloned at the 3′ end of bovine exon 3 (inserted at the SalI and MluI sites which were cloned into the nefm 3′UTR using a linker). The targeting construct was linearized with AatII and electroporated into mouse 129SvEv ES cells (Millipore Corporation) by the MU Transgenic Core (University of Missouri) and selected with G418 at 250 μg/ml (Joyner, 1994). Drug-resistant colonies were amplified and screened by PCR at the 3′ end and Southern blot at the 5′ end. DNA sequence analysis (MU DNA Core, University of Missouri) was used to ensure incorporation of bovine nefm exon 3. Two of 192 ES clones were identified to have undergone homologous recombination at both the 5′ and 3′ ends of the gene to produce the NF-MBovineTail targeted allele. One of the positive ES cell clones was injected into mouse C57BL/6 blastocysts and the MU Transgenic Core implanted blastocysts into the uteri of pseudo-pregnant surrogates. Four chimeric male mice were identified from the surrogates. Germ line transmission of the NF-MBovineTail allele was confirmed by PCR amplification of genomic DNA purified from tail biopsies using Ex Taq (Clontech Laboratories) with the following primers: Forward Primer, 5′-AAACTCCTAGAGGGGGAAGAGACCAGAT-3′; Mouse Reverse Primer, 5′-CAACTCCTCTGCGATGGCTGTGA-3′; Bovine Reverse Primer, 5′-CTCCTTTTCTCCTTCCTCTTCTTTA-3′. Mice of either sex were bred to homozygosity (NF-MBovineTail) and wild-type littermates of either sex were used as controls for the analyses.
Detection and quantification of neurofilament and tubulin proteins by immunoblotting.
Sciatic nerve and spinal cord tissues were dissected and homogenized on ice in a buffer containing 50 mm Tris, pH 7.5, 0.5 mm EDTA, pH 8, and protease inhibitors were added according to the manufacturer's protocol (Complete Mini, Roche). An equal volume of a solution containing 50 mm Tris, pH 7.5, 150 mm NaCl, 1% NP-40, 1% sodium deoxycholate, and 2% SDS was added, and the homogenates were sonicated for 20 s, boiled for 10 min, and clarified by centrifugation at 16,000 × g for 10 min. Protein concentration was determined using the Bio-Rad Protein Assay kit. Protein extracts were separated on 7.5% SDS-polyacrylamide gels and transferred onto nitrocellulose membrane or stained with Coomassie Blue. Mouse monoclonal antibodies to NF-L (MCA-DA2; EnCor Biotechnology) and NF-M (RMO44; Abcam) were used to identify each protein. NF-H was identified with a chicken polyclonal antibody that recognizes mammalian subunits (CPCA-NF-H; EnCor Biotechnology). NF-H was detected using a mouse monoclonal antibody that recognizes the protein in a phospho-dependent manner (SMI-31; Covance). Neuron-specific βIII-tubulin was identified with a mouse monoclonal antibody (TUJI; Covance). Mouse and chicken primary antibodies were detected with donkey anti-mouse and goat anti-chicken secondary antibodies conjugated to IRdye-700X infrared fluorophores (Rockland), respectively. Immunoreactive bands were visualized by infrared detection with an Odyssey image scanner (LI-COR Biosciences).
Absolute intensities of immunoreactive bands were obtained using Photoshop (Adobe Systems Inc.). Relative optical densities (RODs) of immunoreactive bands were calculated as follows: [(SMI-31 mean intensity − background mean intensity) * (number of pixels)]/[(CPCA-NF-H mean intensity − background mean intensity) * (number of pixels)]. Optical densities of immunoreactive bands of each NF subunit were calculated by measuring the mean intensity − background mean intensity. Wild-type average optical densities were arbitrarily set to a value of one. Average SMI-31 RODs were analyzed for statistical significance by one-way ANOVA with Holm–Sidak post hoc analysis for pairwise comparisons (SigmaPlot, Systat Software).
Tissue preparation, axon morphological analysis, EM, and NF nearest-neighbor analysis.
Mice were killed and perfused intracardially with 2.5% glutaraldehyde and 4% paraformaldehyde in 0.1 m Sorenson's phosphate buffer, pH 7.2, and postfixed overnight in the same buffer. Fifth lumbar nerve roots were dissected, treated with 2% osmium tetroxide, washed, dehydrated, and embedded in Epon-Araldite resin. Thick sections (0.75 μm) for light microscopy were stained with ρ-phenylenediamine. Images of cross sections of L5 motor axons were collected with a Zeiss Axio Imager A1 light microscope. Cross sections of L5 motor were analyzed in at least five mice per genotype and age group. Entire roots were imaged, imaging thresholds were selected individually, and the cross-sectional area of each axon was calculated and reported as a diameter of a circle of equivalent area using the AxioVision Digital Image Processing Software (Carl Zeiss MicroImaging). Axon diameters were grouped into 0.5 μm bins. Myelin thickness and g-ratios were estimated by measuring the axonal diameter and fiber diameter of individual axons for 10% of all axons per motor roots using AxioVision Digital Image Processing Software (Carl Zeiss MicroImaging). The total number of axons was analyzed for statistical significance by two-way ANOVA (SigmaPlot, Systat Software) Bimodal distributions of motor axon diameter were analyzed for overall statistical significance by the Mann–Whitney U test. Myelin thickness and g-ratios were analyzed for statistical significance by three-way ANOVA with Holm–Sidak post hoc analysis for pairwise comparisons.
Thin sections (60–90 nm) were cut from prepared resin blocks with a Leica Ultracut E ultramicrotome and stained with 1% aqueous uranyl acetate for 15 min, followed by bismuth subnitrate for 2 min. Images of selected neurons were collected at 80 kV with a JEOL 1400 Transmission Electron Microscope at magnifications of 5000, 10,000, or 20,000. Microtubules were counted within axoplasm. Neurofilaments were traced and nearest-neighbor calculations made. Raw NF spacing numbers were acquired using IMOD software (University of Colorado, Boulder, CO), and NF nearest-neighbor distance (NND) data were grouped into 4 nm bins using NCMIR Pointzilla (University of California, San Diego, CA). NF numbers were analyzed for statistical significance using Student's t test (small motor axons) or Mann–Whitney U test (large motor axons) (SigmaPlot, Systat Software).
Neurofilament clustering.
Average neurofilament spacing was determined as described previously (Garcia et al., 2003, 2009), by distributing identified neurofilaments in uniform arrays across the effective cross-sectional area of an axon. Briefly, cross-sectional area was estimated by tracing axoplasmic regions of the same digitized electron micrographs used to identify neurofilaments. Neurofilaments were organized in concentric hexagonal “rings” of equilateral triangles, with average neurofilament spacing calculated as the side length of one triangle. Neurofilament clustering was defined as the ratio of average filament spacing to nearest-neighbor filament spacing, with higher ratios implying more clustered (less uniformly distributed) neurofilaments. Analysis was performed using MATLAB 6.5 (The MathWorks). Clustering, NF density, microtubule density and microtubule/ NF ratios were analyzed for statistical significance by two-way ANOVA (SigmaPlot, Systat Software).
Nerve conduction velocity measurements.
Nerve conduction velocities were measured in the sciatic nerve, interosseus muscle system of 6-month-old mice (Calcutt et al., 1990). In brief, mice were anesthetized with isoflurane (4% in O2 for induction, 2–3% for maintenance), and both nerve and core temperatures were maintained at 37°C by a heating lamp and thermal pad connected to a temperature regulator and near-nerve rectal thermistor probes. The sciatic nerve was stimulated with single supramaximal square wave pulses (4–8 V and 0.05 ms duration) via fine needle electrodes placed at the sciatic notch and Achilles tendon. Evoked electromyograms were recorded from the interosseus muscles of the ipsilateral foot via two fine needle electrodes and displayed on a digital storage oscilloscope. The distance between the two sites of stimulation was measured using calipers, and conduction velocity was calculated as previously described (Calcutt et al., 1990). Measurements were made in triplicate from a minimum of seven animals per genotype, and the median was used as the measure of velocity. Values were compared for overall statistical significance by Student's t test (InStat, GraphPad Software).
Computational simulations of NF C termini.
The computational part of the present study uses the sequence-based, coarse-grained NF brush model of Chang et al. (2009). The model consists of long flexible side arms tethered to a central rigid cylindrical core representing the 10-nm-diameter NF backbone (Fig. 1) (Chang et al., 2009). In this model, NF C termini were modeled at amino acid resolution, with each amino acid represented by a sphere of diameter σs = 0.6 nm along with the corresponding charge. Charges consistent with a neutral pH were assigned to all ionizable residues as well as all serine residues of the KSP repeat motifs in accordance to the phosphorylation state of the filament. Counter-ions were added explicitly to achieve electroneutrality, whereas solvent was treated implicitly through the use of appropriate dielectric constant (or Bjerrum length lB = 0.7 nm for water solution at T = 300K). The interaction potential between different objects was treated as the sum of hard sphere (or rod) and electrostatic interactions. The model was based on the sequence and stoichiometry of mouse neurofilament (Stevenson et al., 2011). A model of mouse-bovine chimera (NF-MBovineTail) was generated by substituting the NF-M sequence of the mouse with that of the cow. The sequences of mouse neurofilament light, medium and heavy side arm polypeptides were retrieved from the Uniprot Consortium with accession numbers P08551, P08553, and P19246 (Jain et al., 2009). The sequence of bovine NF-M was retrieved from NCBI with accession number O77788 (Trimpin et al., 2004; Benson et al., 2009). The NF system was placed in a simulation box 400 × 400 wide and 50 nm deep. Periodic boundary condition was imposed along the longitudinal axis of the filament, allowing a representation of an infinitely long filament. Then, off-lattice canonical ensemble Monte Carlo (MC) simulations were conducted under phosphorylated, dephosphorylated, and NF-M phospho-incompetent conditions. NF-M phospho-incompetence was attained from phosphorylated NF system by replacing all the serine in the NF-M KSP repeats by alanine, thus defeating the negative charge change associated with phosphorylation. The MC simulations were performed under 150 mm ionic conditions, and was accomplished by using the screened coulomb (Debye–Hückel) potential (McQuarrie, 2000). More details on the model and simulation procedures can be found in the study by Stevenson et al. (2011). Averages of radius of gyration for each NF subunit in each condition were analyzed by Student's t test.
Mathematical modeling of nerve conduction velocity.
To estimate the effect of a change in membrane capacitance (as reflected by the change in g-ratio between wild-type and NF-MBovineTail mice) on conduction velocity, a mathematical model of the axon fashioned after linear cable theory (Cotterill, 2002) was used to determine the velocity of action potential propagation down multiple nodes in a cable as follows:
where X represents the electrotonic length x/λ and T represents t/ τm. This allowed changes in resistance and capacitance to be introduced into the model as and τm = Rm * Cm. Values of key properties measured directly from sciatic nerve axons as reported in the literature (Kriz et al., 2000) were incorporated as follows: V0 (action potential amplitude) = 87.7 mV, Vrest = −75.5 mV, Rm = 25.8 MΩ cm2. Other variables were determined based on similar measurements taken from other sources, including Ri = 200 Ω cm and Cm = 0.6 μF cm−2 (Squire, 2003) and threshold voltage of −55 mV. Time to threshold values were obtained from the nominal model (wild-type) with X representing the internodal segment electrotonic length, and then velocity was simply calculated as distance per unit time. Finally, this velocity was scaled to match that of the biological data for wild-type mice (i.e., 47.3 m/s) to estimate total distance over which the recordings were made. Factors of diameter and capacitance were altered to mimic changes observed in the experimental data. Specifically, conduction velocity of an expansion solely in axon diameter with all other factors remaining constant was estimated to predict conduction velocity for the axon diameter shift seen in the NF-MBovineTail mice. A change in Cm was estimated based on values of g-ratio proportionally as follows: Cm ∝ 1/(D − d)22 = k/(D − d)2, where D represents fiber diameter and d represents axon diameter. The k value was solved based on the nominal model and then G-ratio (fiber and axon diameter) values were substituted from the NF-MBovineTail mice to determine the change in capacitance relative to the nominal model. This was then incorporated into a final model that included the increase in axon diameter as well as the predicted change in capacitance.
Results
Generation of chimeric NF-M gene through gene replacement of murine nefm exon 3 with bovine exon 3
To replace the endogenous nefm exon 3 with bovine exon 3, a segment of murine nefm containing exon 3 (∼2.2 kb AccI/AccI fragment) was subcloned into pBluescript. Bovine exon 3 was PCR amplified from bovine sperm DNA, and subcloned into the murine ∼2.2 kb AccI/AccI nefm fragment using BsrGI and NdeI sites. The modified AccI/AccI nefm with bovine exon 3 fragment was cloned back into endogenous nefm. Replacing murine nefm exon 3 with bovine exon 3 generated a chimeric gene in which exon 1 and 2 were derived from the endogenous murine nefm while exon 3 was derived entirely from bovine nefm (Fig. 1A). Replacing endogenous exon 3 with bovine exon 3 resulted in a tail domain that was 76 aa longer and contained 15 additional KSP repeats (Fig. 1B). The final targeting construct contained 8 kb of homology, including an added 3′UTR and polyadenylation signal from the murine nefl gene and neomycin phosphotransferase gene (Fig. 1A). Following ES cell electroporation, two of 192 clones were identified to have recombined the modified nefm construct into one of the endogenous nefm alleles. The clones were injected into C57BL/6 blastocysts to produce chimeric animals that when bred to C57BL/6 mice transmitted the chimeric nefm (referred to as NF-MBovineTail) allele to their progeny. Mating pairs of mice heterozygous for the NF-MBovineTail allele produced homozygous animals (Fig. 1C) at the expected Mendelian frequency. The homozygous progeny were viable, fertile and displayed no overt phenotype through 2 years, the oldest age analyzed.
Expression of NF-MBovineTail decreased electrophoretic mobility of NF-M
Upon SDS-PAGE fractionation, mouse NF-M subunits in sciatic nerve extracts taken from 2- and 6-month-old mice migrated at a molecular weight of ∼140 kDa (Fig. 2A,D). Coomassie Blue staining revealed that NF-MBovineTail migrated at ∼160 kDa (Fig. 2A,D). Immunoblotting with an antibody specific to an epitope at the end of the NF-M rod domain (RM044, Abcam) confirmed the difference in the electrophoretic mobilities of the wild-type and NF-MBovineTail proteins and confirmed similar expression levels at 2 (Fig. 2B) and 6 (Fig. 2E) months. Moreover, similar levels of NF-L (MCA-DA2; EnCor Biotechnology), NF-H (CPCA-NF-H; EnCor Biotechnology), and the neuron-specific βIII-tubulin isoform (TUJI, Covance) were also observed in wild-type and NF-MBovineTail extracts at 2 (Fig. 2B, except βIII-tubulin) and 6 (Fig. 2E) months, demonstrating that NF-MBovineTail did not affect accumulation of the other major axonal cytoskeletal proteins in sciatic nerve. Detection of phospho-epitopes of NF-H recognized by SMI-31 (SMI-31, Covance) revealed an apparent decrease in NF-H phosphorylation in NF-MBovineTail mice at 2 (Fig. 2B) and 6 (Fig. 2D) months. ROD of immunoblots confirmed a significant reduction in NF-H phosphorylation of NF-MBovineTail heterozygous and homozygous mice relative to wild-type (Fig. 2C). This was likely due to decreased total phosphorylation of NF-H proteins, as expression of all NF subunits was not altered in NF-MBovineTail mice. Statistical analysis of ROD by one-way ANOVA followed with Holm–Sidak post hoc analysis for pairwise comparisons indicated a significant difference between wild-type, NF-MBovineTail heterozygous and homozygous mice. However, this compensatory decrease in phosphorylation of NF-H was unlikely to affect radial growth as preventing all NF-H KSP phosphorylation through the deletion of NF-H C terminus did not affect radial growth (Rao et al., 2002; Garcia et al., 2003).
Increasing the length of the NF-M C terminus increased radial growth of large motor axons
To determine whether lengthening the NF-M C terminus influences radial axonal growth and survival, the size of all axons within the fifth lumbar motor root was determined at 2 and 6 months (Fig. 3A). Axons were counted (Fig. 3B) and cross-sectional areas were measured for all axons at both time points, and corresponding diameters were calculated (Fig. 3C,D). Accumulation of wild-type and NF-MBovineTail protein yielded bimodal distributions of motor axons (Fig. 3C,D). At 2 and 6 months, the peak diameter of large motor axons from NF-MBovineTail mice was increased relative to wild-type littermates (Fig. 3C,D). Peak diameters in large NF-MBovineTail axons were 1 μm greater than large wild-type axons at 2 months and 0.75 μm greater than large wild-type axons at 6 months. Statistical analysis by Mann–Whitney U tests indicated a significant difference in the diameter distribution of motor axons at both 2 and 6 months. Interestingly, at 2 months the peak diameter of small motor axons from NF-MBovineTail mice was 0.5 μm smaller. However, there was no difference in peak diameters for small motor axons at 6 months. The total number of motor axons tended to be lower in NF-MBovineTail mice (Fig. 3B) but the difference was not statistically significant. These results demonstrate that extending the length of NF-M C terminus expanded axonal diameter of large motor axons.
Computational modeling of NF C termini predicted that NF-MBovineTail C terminus extended farther from the NF core than wild-type
Phylogenetic analysis suggested that longer NF-M C termini correlated with larger axonal diameters in a subset of mammals (Barry et al., 2010). Moreover, computational modeling of human NF-L, NF-M, and NF-H C termini under salt-free condition suggested that the NF-M C terminus extended the farthest from the NF core (Chang et al., 2009). Computational modeling was therefore used to determine whether increasing the length of NF-M C terminus increased the lateral extension of NF-M C terminus from the filament core and whether increased lateral extension was dependent upon KSP phosphorylation. The structural organization of all NF C termini was analyzed under the following conditions for wild-type murine NF-M and murine NF-M in which the C terminus was replaced by bovine C terminus (NF-MBovineTail): (1) dephosphorylated KSP repeats, (2) KSP phospho-incompetent (S→A), and (3) phosphorylated KSP repeats. Simulations were performed in 150 mm monovalent salt conditions (Fig. 4A,B). To examine the effects of charge distribution and stoichiometry on lateral extension of wild-type and NF-MBovineTail C termini, the structural organization of NF heteropolymers was visually inspected with representative snapshots taken from MC simulations (Fig. 4A,B). Qualitatively, NF-M C terminus from NF-MBovineTail axons extended farther from the NF core independent of KSP phosphorylation (Fig. 4A,B).
Radius of gyration has been previously used to quantify the lateral extension of each NF C terminus from the NF core (Chang et al., 2009; Stevenson et al., 2011). Radius of gyration for each NF C terminus under 150 mm monovalent salt conditions was determined by sampling data every 1000 iterations of the MC simulation steps (from eight independent simulations) so that a total of 8000 equilibrated configurations could be selected for averaging. The phosphorylation-mediated changes in the NF C termini were then quantified using the [Rg] values determined from this analysis. In particular, the radial (perpendicular to the core of the filament) component [Rg] that best describes the lateral extension of NF C termini was calculated. Replacing murine NF-M C terminus with bovine C terminus had no affect on NF-L and NF-H extension (Fig. 4C). Interestingly, NF-MBovineTail C terminus extended farther from the NF core than wild-type NF-M independent of NF-M KSP phosphorylation (Fig. 4C–E). Statistical analysis by Student's t test indicated significant differences in radius of gyration between NF-M C termini of wild-type and NF-MBovineTail in each condition.
Ensemble-averaged monomer density profile [ρ(r)] was also used to estimate extension of NF C termini from the NF core. Unlike radius of gyration, monomer density profiles of NF C termini estimated the maximum lateral extension of NF C termini above a cutoff value (Chang et al., 2009; Stevenson et al., 2011). This quantity measured the probability of finding monomers as a function of the radial distance r from the filament core. For each NF side arm, ρ(r) was calculated by counting the number of monomers or CG sites that were within concentric cylinders bounded by the radii r and r + δr. For any one particular configuration, the density profile ρ(r) of a particular type of C terminus was obtained by summing over all C termini belonging to the same type and then normalizing by the total number of C termini of that type. This was then averaged over 8000 configurations obtained from eight independent simulations. While [ρ(r)] served as a complementary measure for describing the C-terminal brush structure quantitatively, it also provided valuable information on the maximum lateral extension of individual C termini. By noting the cutoff radius rc at which [ρ(r)] vanished, one can estimate and compare the range of the maximum lateral extensions of NF C termini. Under 150 mm monovalent salt conditions, the maximum lateral extension of phosphorylated NF-M C termini in NF-MBovineTail was predicted to be farther than wild-type (Fig. 4F).
Expression of NF-MBovineTail did not affect neurofilament spacing or clustering in small and large motor axons
To determine whether increasing the length of the NF-M C terminus altered NF spacing, number and organization within peripheral myelinated axons, fifth lumbar small and large motor axon cross sections from wild-type and NF-MBovineTail were visualized by electron microscopy. NFs were analyzed from axons that were at or near the peak diameter for each class of axon analyzed. NF spacing and number were quantified by calculating NNDs of adjacent NFs within axoplasm of small motor axons at 2 (Fig. 5A,B) and 6 (Fig. 5C,D) months, as well as large motor axons at 2 (Fig. 5E,F) and 6 (Fig. 5G,H) months. The peak in NF spacing was unaffected in NF-MBovineTail small motor (Fig. 5A,C) and large motor (Fig. 5E,G) axons when compared with wild-type. Peak distances of NFs in wild-type and NF-MBovineTail small and large motor axoplasm were identical at 2 and 6 months. NF number in small motor axons was unaffected at 2 months (Fig. 5B). There were slightly fewer NFs in NF-MBovineTail large motor axons at 2 months (Fig. 5F) and in small and large motor axons at 6 months (Fig. 5D,H) relative to axons from age-matched wild-type mice but the differences were not statistically significant.
Neurofilament clustering was measured by identifying the positions of all NFs in small and large motor axons and calculating the ratio of average filament spacing to nearest-neighbor distance. Higher ratios implied less uniformly distributed NFs. NFs within an axon were redistributed into concentric hexagonal rings of equilateral triangles over a cross-sectional area equal to the cross-sectional area of the axon. Average NF spacing was then defined as the edge length of each triangle. A perfectly ordered array of NFs would have, therefore, yielded a value of 1.0. As expected, the NF array in wild-type mice diverged from a perfectly ordered arrangement (Fig. 6A,B) at both 2 and 6 months. In large motor axons, NF clustering indexes were slightly less in NF-MBovineTail at 2 and 6 months (Fig. 6B) relative to wild-type suggesting a more ordered array of NFs. However, statistical analysis by two-way ANOVA indicated the difference in NF clustering between wild-type and NF-MBovineTail was not significant. NF clustering indexes of small motor axons were slightly less at 2 months but greater at 6 months when compared with wild-type mice (Fig. 6A) but the differences were not statistically significant. NF densities (number of NFs/μm2 of axoplasm) small motor (Fig. 6C) and large motor (Fig. 6D) axons were not significantly different between wild-type and NF-MBovineTail at 2 and 6 months.
Motor nerve conduction velocity was unaffected in NF-MBovineTail mice
Axonal diameter was a primary determinant of conduction velocity in myelinated axons (Hursh, 1939; Boyd and Kalu, 1979; Garcia et al., 2003). Therefore, motor nerve conduction velocities (MNCVs) were measured in the sciatic nerve of 6-month-old wild-type and NF-MBovineTail mice (7 animals per genotype). MNCV was indistinguishable in NF-MBovineTail relative to wild-type littermates (Fig. 7A).
Myelin expansion was attenuated in NF-MBovineTail motor axons
To determine whether myelination was altered in NF-MBovineTail motor and axons, myelin thickness and g-ratios were calculated by measuring axon diameter and fiber (myelin and axon) diameter for 10% of randomly sampled axons from the fifth lumbar motor roots (Fig. 7B). At both 2 and 6 months myelin thickness was reduced for small motor axons of NF-MBovineTail mice relative to wild-type (Table 1). Myelin thickness of large (> 4 μm) motor axons from NF-MBovineTail mice was similar to that of wild-type mice at 2 months but by 6 months was significantly lower, reflecting a failure to increase at the same rate as myelin of wild-type mice (Table 1). Analysis of myelin thickness by three-way ANOVA followed with Holm–Sidak post hoc analysis for pairwise comparisons indicated a significant difference in myelin thickness between wild-type and NF-MBovineTail mice for small motor axons at 2 and 6 months and for large motor axons at 6 months. At both 2 and 6 months (Table 1), both g-ratios of small and large motor axons in NF-MBovineTail mice were significantly increased, indicating that the relative thickness of myelin was reduced. Analysis of the g-ratios by three-way ANOVA followed with Holm–Sidak post hoc analysis for pairwise comparisons indicated a significant difference in g-ratio of small and large motor axons between wild-type and NF-MBovineTail mice at 2 and 6 months. Inspection of compact myelin of small and large motor axons indicated no observable differences in myelin structure (Fig. 7C).
Table 1.
Axon | Genotype | Age (months) | Peak axonal diameter (μm) | Average myelin thickness (μm) | Average g-ratio |
---|---|---|---|---|---|
Small motor (<4 μm) | wild type | 2 | 1.5 | 0.730 ± 0.013 | 0.586 ± 0.004 |
6 | 1.5 | 0.826 ± 0.016 | 0.576 ± 0.004 | ||
NF-MBovineTail | 2 | 1 | 0.690 ± 0.012* | 0.604 ± 0.004* | |
6 | 1.5 | 0.768 ± 0.015* | 0.604 ± 0.004** | ||
Large motor (>4 μm) | wild type | 2 | 5 | 1.442 ± 0.015 | 0.707 ± 0.003 |
6 | 7.5 | 1.754 ± 0.014 | 0.724 ± 0.003 | ||
NF-MBovineTail | 2 | 6 | 1.423 ± 0.015 | 0.719 ± 0.003** | |
6 | 8 | 1.690 ± 0.013** | 0.741 ± 0.003** |
g-ratio, Axon diameter/fiber diameter (myelin and axon diameter). ± values are SEM.
*p < 0.05;
**p < 0.001.
Mathematical modeling was performed to predict the effect of altering axonal diameter and g-ratios on conduction velocity in NF-MBovineTail mice (Table 2), bearing in mind that our experimental MNCV measurements record the velocity of large myelinated fibers. Consistent with experimental MNCV results, the modeling predicted a MNCV of 46.8 m/s, which was similar to the MNCV measured in NF-MBovineTail mice. Interestingly, if g-ratios were the same in NF-MBovineTail mice as wild-type, the model predicted an increase in MNCV to 50.5 m/s in NF-MBovineTail mice (Table 2).
Table 2.
Group | Diameter (μm) | G-ratio | Rm (MΩ cm2) | Ri (Ω cm) | Cm (μF cm−2) | τm (ms) | MNCV (m/s) |
---|---|---|---|---|---|---|---|
Wild-type mouse | 7.5 | 0.72 | – | – | – | – | 47.3 ± 2.6 |
NF-MBovineTail mouse | 8 | 0.74 | – | – | – | – | 46.2 ± 1.7 |
wild type model | 7.5 | 0.72 | 25.8 | 200 | 0.6 | 1.55 | 47.2 |
NF-MBovineTail model (Δ diameter + Δ g-ratio) | 8 | 0.74 | 25.8 | 200 | 0.646 | 1.67 | 46.8 |
NF-MBovineTail model (Δ diameter) | 8 | 0.72 | 25.8 | 200 | 0.6 | 1.55 | 50.5 |
Experimental values for peak axonal diameter, G-ratio, and MNCV were obtained from large myelinated fibers. Rm, membrane resistance; Ri, axonal resistance; Cm, membrane capacitance; τm, membrane time constant. Dashes are values that were not determined.
Discussion
NF-M C terminus mediated radial growth by a mechanism that was independent of KSP phosphorylation. Using a combination of gene targeting and computational modeling, we demonstrated that increasing the overall length of NF-M C terminus, by replacing mouse exon 3 with cow exon 3, resulted in larger axonal diameters in motor neurons. Increasing the length of NF-M C terminus resulted in an increase in peak axonal volume of ∼44% at 2 months and ∼ 22% at 6 months relative to wild-type. The enhancement at 2 months was exactly the same magnitude observed in mice overexpressing NF-L and NF-M subunits by 300 and 360%, respectively, relative to wild-type levels (Xu et al., 1996). However, enhanced radial growth in NF-MBovineTail mice was accomplished by expanding the NF-M C terminus by 76 amino acids including 15 additional KSP repeats. This alteration did not affect subunit stoichiometry, nor did it affect NF-M interaction with other NF subunits.
Increasing the length of NF-M C terminus might have enhanced radial growth by increasing the distance the C terminus extended from the filament core. Utilizing parameters originally developed for wild-type mouse and human NF-M (Chang et al., 2009; Stevenson et al., 2011), computational analysis of NF-MBovineTail suggested that the longer C terminus projected farther from the filament core than wild-type mouse NF-M in conditions that simulate the ionic strength of axoplasm. Moreover, increased extension was independent of phosphorylation status of NF-M C-terminal KSP repeats supporting the observation that expressing KSP phoshpo-incompetent NF-M did not prevent radial growth in vivo (Garcia et al., 2009). Despite potentially extending farther from the filament core, axoplasmic organization and NF-NF spacing were unaltered in NF-MBovineTail motor axons. These results supported earlier observation that NF-NF spacing did not directly correlate with larger axonal diameters (Garcia et al., 2003, 2009). Moreover, NF-NF spacing was not increased in transgenic mice overexpressing NF-L and NF-M in which radial growth was increased (Xu et al., 1996). Therefore, it remains to be determined precisely how NF-M C terminus determines axonal diameter. One possible explanation is that NF-M C terminus serves as a scaffold for cytoskeletal linking proteins such as plectin. Plectin is a member of the plakin family of cytoskeletal linking proteins (Jefferson et al., 2004), which has been detected in motor neurons (Errante et al., 1994). Moreover, deletion of the neuron-specific isoform of plectin resulted in a phenotype that was similar to the phenotypes observed in NF-M deleted mice (Elder et al., 1998; Kriz et al., 2000) and mice expressing C-terminally truncated NF-M (Garcia et al., 2003). Specifically, deletion of plectin 1c reduced axonal diameter and motor neuron conduction velocity (Fuchs et al., 2009). Thus, increasing the length that NF-M C terminus extended from the filament core may have resulted in a longer-range interaction between NF-M C terminus and plectin 1c resulting in larger axonal diameters.
Despite increased axonal diameter, MNCV of the largest fibers in the sciatic nerve was unaffected in NF-MBovineTail mice (Fig. 7A). Failure to increase conduction velocity in motor axons may have resulted from relatively thinner myelin in NF-MBovineTail mice, without observable differences in the structure of myelin lamellae. Comparing myelin thickness at 2 and 6 months indicated that NF-MBovineTail mice did not increase their myelin thickness in response to larger axonal diameters. Mathematical modeling of conduction velocity suggested that the observed failure to adequately increase myelin thickness was sufficient to account for slower than expected conduction velocities in NF-MBovineTail mice. Moreover, mathematical modeling indicated that, had myelin thickness increased in proportion with increasing axonal diameter in NF-MBovineTail mice, the observed increase in fiber diameter would have resulted in faster MNCV. Despite not increasing small motor axon diameter, expansion of NF-M C terminus resulted in a significant reduction in relative myelin thickness and a significant increase in g-ratio of small motor axons. In fact, the increased g-ratio of small motor axons was greater than the observed increase in large motor axons. A more pronounced effect on myelin thickness was also observed in small axons of mice with altered neuregulin (NRG) expression (Michailov et al., 2004). It is unclear why small axons were more susceptible to genetic manipulations that altered myelin thickness.
Increased expression of NRG1 type III resulted in significantly thicker myelin sheaths (Michailov et al., 2004), but axonal diameter appeared largely unaffected. Moreover, increasing radial growth, by expanding the length of NF-M C terminus, resulted in significantly larger motor axons with myelin sheaths that failed to expand proportionally. Active signaling has been observed between Schwann cells and axons. NRG1 type III was an axonal ligand for the Schwann cell receptor, ErbB2 (Nave and Salzer, 2006), that regulated myelin thickness (Michailov et al., 2004). Formation of compact myelin increased NF phosphorylation (de Waegh et al., 1992) possibly through the interaction of myelin associated glycoprotein (Yin et al., 1998) with an as yet to be identified axonal receptor. However, when taken together with the NRG1 type III results, our data suggested that once the processes of myelination and radial growth initiated there was no active feedback between myelinating Schwann cell and axons. Therefore, during myelination and radial growth, there was no plasticity allowing for compensatory alterations to myelin thickness or axonal diameter due to enhanced radial growth or myelination, respectively.
Footnotes
This work was supported by grants from the National Science Foundation (NSF) (MCB-0544602) and University of Missouri Research Board to M.L.G., National Institutes of Health (DK 057629) to N.A.C., and National Science Foundation (CMMI1130997) to S.S. Salary support for M.L.G. was provided by University of Missouri and C.S. Bond Life Sciences Center. D.M.B. was supported by both the C.S. Bond Life Sciences Fellowship Program and the Graduate Assistance in Areas of National Need Fellowship Program. P.J.W. was supported by a NSF REU grant to Dr. Satish Nair and Dr. David Schulz (DBI 2062667). We thank Lucie Guernsey and Katie Frizzi for technical support; Dr. Natalia Karasseva and the University of Missouri Transgenic Animal Core for the generation of gene-replacement chimeric mice; Cheryl Jensen and the University of Missouri EM Core for assistance with EM preparation and imaging; Brian Reigle for writing the scripts used in automated determination of numbers of axons in assigned groups for axonal diameter profiles; and Steve Lamont for writing Pointzilla.
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