Curriculum/Pillar 1 · Electrophysiology of Motor Systems

Conduction Physiology

Module 3 of 36·28 min readLIVE MODEL
Learning objectives
  • 1Derive conduction velocity from internodal geometry and nodal currents
  • 2Quantify the effects of temperature and axon diameter on velocity
  • 3Predict how demyelination degrades the safety factor and slows or blocks conduction

Conduction velocity is the single most informative number in nerve conduction studies because it is mechanistically transparent: it is determined almost entirely by axon diameter and myelin integrity, and it shifts in lawful, quantifiable ways with temperature. A clinician who understands why myelinated fibres conduct at metres per millisecond — and precisely how that speed collapses when myelin fails — can read a velocity not as a number but as a statement about the structure of the nerve.

Saltatory conduction: leaping the insulated cable

In an unmyelinated axon the action potential propagates continuously, each patch of membrane sequentially depolarizing its neighbour — a slow, metabolically expensive process limited to ~0.5–2 m/s. Myelination replaces this with saltatory conduction (Latin saltare, to leap): the high-resistance, low-capacitance sheath confines transmembrane current to the bare nodes of Ranvier, so the regenerative spike is excited only at successive nodes while the depolarizing current flows passively and almost instantaneously down the insulated internode between them. The action potential therefore appears to jump from node to node. The speed gain is enormous — large myelinated fibres reach 50–70 m/s — and it is purchased by the cable optimization described below.

The biophysical requirements are twofold. The internodal myelin must raise the membrane space constant λ enough that the passive voltage reaching the next node still exceeds threshold, and it must lower membrane capacitance so little charge is wasted swinging the internodal voltage. When both hold, current that would otherwise leak radially across the membrane is instead delivered longitudinally to the next node — conduction is fast because the current is not wasted.

Nodes of Ranvier: high channel density, high current

The node is a roughly 1 µm gap in the myelin where the regenerative machinery is concentrated. Its defining feature is an extraordinary density of voltage-gated Na⁺ channels (Nav1.6) — on the order of 1,000–2,000 channels/µm², orders of magnitude above the internodal axolemma. This concentration produces a large nodal inward current in a brief interval, generating enough charge to depolarize the next node to threshold across the intervening cable losses. The molecular architecture is precisely engineered: Na⁺ channels are anchored at the node by ankyrin-G and βIV-spectrin and fenced in by the paranodal junctions, while delayed-rectifier Kv1 channels sit in the juxtaparanode, shielded by myelin. In health the Kv channels are barely engaged; the nodal spike is dominated by fast Na⁺ entry, and conduction is efficient.

LIVE MODELThe nodal spike — modelling current density and channel availability
Vₘ now
-65mV
Last peak
-65mV
Fired?
Firing rate
0Hz
The action potential modelled here is the regenerative event that must fire at each node. Press Stimulate and observe the large, brief sodium current (blue) that supplies the charge for propagation. Now reduce Na⁺ channel availability: as nodal sodium current falls, the spike narrows, slows, and ultimately fails — the direct analogue of what demyelination does to the downstream node when increased capacitative load and current leak starve it of the charge it needs to reach threshold. This is the biophysics of conduction slowing and block made visible.

Determinants of conduction velocity and the 6 × diameter rule

For a myelinated fibre, conduction velocity scales linearly with total fibre diameter, and the relationship is captured by a remarkably durable empirical rule:

CV (m/s) ≈ 6 × fibre diameter (µm)

Thus a 12 µm fibre conducts at roughly 72 m/s and a 10 µm fibre at ~60 m/s — values that bracket the fastest motor and sensory axons sampled in routine studies. The linear scaling arises because larger diameter simultaneously lowers internal axoplasmic resistance (raising λ and speeding longitudinal current flow) and is accompanied by proportionally longer internodes and thicker myelin, so the leap distance per node grows in step with the cable improvement. (In unmyelinated fibres, by contrast, velocity scales only with the square root of diameter, which is why unmyelinated conduction is so much slower for a given size and why evolution favoured myelin for speed.) Two practical consequences follow. First, a clinically measured velocity reflects only the fastest-conducting fibres in the population, because the onset latency times the earliest arrivals; loss of the largest fibres slows the measured velocity even when most axons survive. Second, because velocity is set by diameter and myelin, it is the parameter that dissociates demyelinating from axonal pathology.

Velocity reads the fastest fibres, amplitude counts all of them

Onset latency — and therefore calculated conduction velocity — is determined by the earliest-arriving, largest-diameter axons. Amplitude, by contrast, integrates the whole responding population. This is why dropout of the largest fibres can slow velocity into the "demyelinating" range while amplitude is only mildly reduced, and why interpreting velocity in isolation from amplitude is a recurring source of error. Always read the pair together.

Temperature: the most common confounder in the laboratory

Cooling slows the gating kinetics of voltage-gated channels, prolonging the time course of the action potential at every node and therefore slowing propagation. The effect is large and quantifiable: conduction velocity falls by roughly 1.5–2.4 m/s for every 1 °C drop in limb temperature, and distal latencies lengthen by ~0.2 ms/°C. Cooling also increases amplitude and duration (slowed Na⁺ inactivation prolongs the spike and reduces phase cancellation), so a cold limb can mimic both demyelinating slowing and, paradoxically, healthier-looking amplitudes. Because the consequences are so systematic, temperature control is non-negotiable:

  • Warm the limb to ≥ 32–34 °C at the recording site (some laboratories target ≥ 33 °C upper limb / ≥ 30 °C lower limb) and document the temperature.
  • A cold limb is the most frequent benign cause of prolonged latencies, slowed velocities, and a falsely positive demyelinating picture — correct it before interpreting anything.
  • Conversely, an unrecognized cold limb can mask a true conduction block by inflating distal amplitude; warming and repeating is the disambiguating maneuver.
≈ 6 m/s
CV per µm fibre diameter
1.5–2.4 m/s
Velocity change per °C
~0.2 ms
Distal latency per °C
≥ 32–34 °C
Target limb temperature

Axon diameter, myelin integrity, and the collapse of the safety factor

The same physics that makes saltatory conduction fast makes it fragile. The margin by which nodal current exceeds the threshold demand of the next node is the safety factor, normally about 5–7×. Demyelination attacks this margin from two directions at once: stripping the internodal sheath raises capacitance (more charge is needed to swing the bared membrane) and lowers resistance (current leaks radially instead of reaching the next node). As the safety factor erodes, a graded spectrum of failure unfolds:

  • Conduction slowing — the wavefront still reaches each node but later; internodal and nodal current is delivered more slowly, and velocity falls. This is the hallmark of demyelinating neuropathy and may include disproportionate prolongation of late responses and distal latencies.
  • Temporal dispersion — different fibres slow by different amounts, so their potentials arrive desynchronized; the CMAP broadens, drops in amplitude, and becomes polyphasic through phase cancellation, even before any fibre blocks outright.
  • Conduction block — once the depolarizing current can no longer bring the next node to threshold, the impulse fails to propagate across that segment. Demonstrating a focal drop in CMAP amplitude/area across a nerve segment, with preserved distal response, is the electrophysiological signature of focal demyelination and the basis for localizing entrapments and inflammatory lesions.

The critical lesion is the internode: failure of even a single internodal segment can drop conduction below the safety factor, which is why focal demyelination produces such disproportionate functional deficit relative to the small length of nerve involved. Newly demyelinated segments are also unusually temperature- and activity-sensitive — a marginally conducting fibre may block with mild warming, after exertion, or during high-frequency firing, explaining the fatigability and heat sensitivity (Uhthoff-type phenomena) characteristic of demyelinating disease.

Clinical Pearl
Before you ever call a study "demyelinating," confirm the limb was warm. A 4 °C drop in temperature can slow conduction velocity by ~8–10 m/s and prolong distal latency by nearly a millisecond — enough to manufacture a demyelinating pattern out of a normal nerve. Temperature is the cheapest variable to control and the most common reason a borderline velocity is over-interpreted; warm to ≥ 32–34 °C, document it, and only then trust the numbers.
Common Pitfall
Do not infer the health of the whole axon population from conduction velocity. Velocity is set by the surviving fastest, largest fibres, so a nerve that has lost most of its large axons but retains a few can still post a near-normal velocity, masking severe axon loss that only the reduced amplitude reveals. Equally, attributing every slowed velocity to demyelination ignores that selective large-fibre loss slows velocity too — the amplitude, temporal dispersion, and conduction-block pattern, not the velocity alone, separate the two mechanisms.
Key points
  • Saltatory conduction confines current to nodes of Ranvier via high-resistance/low-capacitance myelin, raising velocity to 50–70 m/s in large fibres.
  • Nodal Nav1.6 density (~1,000–2,000/µm²) supplies the large brief current that depolarizes the next node; juxtaparanodal Kv1 channels are myelin-shielded in health.
  • For myelinated fibres CV (m/s) ≈ 6 × diameter (µm); velocity reads only the fastest fibres, while amplitude counts the whole population.
  • Temperature is the dominant benign confounder: velocity falls ~1.5–2.4 m/s and distal latency rises ~0.2 ms per °C — warm to ≥ 32–34 °C and document it.
  • Demyelination raises capacitance and lowers resistance, eroding the safety factor (~5–7×) and producing slowing, temporal dispersion, then conduction block.
  • Internodal failure causes disproportionate deficit and temperature/activity-dependent block — the substrate of fatigable, heat-sensitive demyelinating symptoms.
Further reading
  1. 1.Kimura J. Electrodiagnosis in Diseases of Nerve and Muscle. 4th ed. Oxford University Press; 2013: Ch. 4–6 (principles of nerve conduction).
  2. 2.Preston DC, Shapiro BE. Electromyography and Neuromuscular Disorders. 4th ed. Elsevier; 2021: Ch. 2, 8.
  3. 3.Hursh JB. Conduction velocity and diameter of nerve fibers. Am J Physiol. 1939;127:131–139.
  4. 4.Rutkove SB. Effects of temperature on neuromuscular electrophysiology. Muscle Nerve. 2001;24:867–882.
  5. 5.Dumitru D, Amato AA, Zwarts M. Electrodiagnostic Medicine. 2nd ed. Hanley & Belfus; 2002: nerve conduction physiology.
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