Here is a complete, textbook-sourced explanation with diagrams:
How Action Potentials Propagate Along Axons
1. The Core Mechanism - Local Current Flow
When an action potential fires at one point on an axon, that spot becomes depolarized (inside becomes positive, ~+35 mV). The adjacent membrane is still at resting potential (-70 mV). This voltage difference drives local currents:
- Positive charges (Na⁺ ions) flow inward through the depolarized membrane
- These positive charges then travel along the inside of the axon in both directions
- On the outside, current flows back toward the depolarized zone
- This local current raises the voltage in adjacent resting membrane segments to threshold (-55 mV)
- Voltage-gated Na⁺ channels in those adjacent segments open → new action potential fires
- The cycle repeats, moving the wave of depolarization along the entire fiber
This is illustrated in the diagram below:
- A: Resting fiber (positive outside, negative inside)
- B: Depolarization at midpoint - local currents spread in both directions
- C & D: Adjacent segments reach threshold and fire; the wave expands outward
2. Why It Only Goes Forward (Unidirectional)
The area just behind the advancing wave is in the refractory period - Na⁺ channels are inactivated and cannot reopen immediately. This prevents the signal from going backwards and ensures one-way conduction from cell body toward the axon terminal.
3. Unmyelinated vs. Myelinated Fibers
Unmyelinated Fibers (Continuous Conduction)
- Local current spreads continuously along the entire membrane surface
- Every patch of membrane depolarizes in sequence
- Slow - conduction velocity ~0.5 to 2 m/s
- More energy costly (whole membrane must be re-polarized)
Myelinated Fibers - Saltatory Conduction
The myelin sheath (made by Schwann cells in PNS, oligodendrocytes in CNS) wraps the axon in multiple lipid layers - reducing ion flow across the membrane ~5000-fold. The only exposed membrane is at the nodes of Ranvier (2-3 µm gaps between Schwann cells).
As a result:
- Action potentials can only fire at nodes of Ranvier
- Electrical current jumps through the axoplasm and extracellular fluid from node to node
- The impulse "jumps" along the fiber - this is saltatory conduction (from Latin saltare = to jump)
Two major advantages of saltatory conduction:
- Speed: 5- to 50-fold faster than unmyelinated fibers (up to 120 m/s in large myelinated fibers)
- Energy efficiency: Only nodes depolarize → ~100x less ion movement → far less ATP needed to restore ion gradients via Na⁺/K⁺ pump
4. Conduction Velocity - What Determines It?
| Factor | Effect on Velocity |
|---|
| Larger axon diameter | Faster (less internal resistance) |
| Myelination | Much faster (saltatory conduction) |
| Temperature | Higher temp = faster (up to a limit) |
Examples of conduction velocities:
- Large myelinated (Aα fibers): 70-120 m/s (motor neurons, proprioception)
- Small myelinated (Aδ fibers): 5-30 m/s (fast pain, cold)
- Unmyelinated (C fibers): 0.5-2 m/s (slow/burning pain, warmth)
5. Clinical Relevance
- Demyelinating diseases (e.g., Multiple Sclerosis, Guillain-Barré): destroy myelin → saltatory conduction fails → slowed or blocked nerve signals → weakness, numbness, paralysis
- Local anesthetics (e.g., lidocaine): block voltage-gated Na⁺ channels → prevent propagation → no pain signal reaches the brain
- Nerve conduction velocity (NCV) studies: measure propagation speed to diagnose neuropathies
Source: Guyton and Hall Textbook of Medical Physiology, 14th Ed., Chapter 5 (pp. 84-88) - Propagation of the Action Potential & Saltatory Conduction