Audited 31 Jul 2026·Last updated 28 Oct 2026·3 citations·Tier 3·0 uses

Alfvén Velocity Calculator

Alfvén speed v_A = B/√(μρ) from magnetic field in tesla, plasma mass density and permeability, in m/s and km/s, for solar wind, corona or lab plasmas.

Alfvén Velocity Calculator

T
kg/m³
Default: 2022 CODATA vacuum permeability; edit for another medium.
H/m
Alfvén velocity
892,062.0581
The ideal-MHD Alfvén speed in metres per second: the magnetic field divided by the square root of permeability times mass density.
Alfvén velocity
892.0621 km/s
Model scope
Ideal-MHD characteristic speed from coherent SI inputs; plasma composition and relativistic corrections are outside this model.

Background.

Pluck a magnetic field line in a plasma and the kink travels along it like a wave on a guitar string. The field supplies the tension and the plasma threaded on it supplies the mass, so the wave speed comes out the same way a string's does: the square root of tension over density. That speed is the Alfvén velocity, named after Hannes Alfvén, who predicted these waves in 1942 and later shared the 1970 Nobel Prize in Physics for his work on magnetohydrodynamics.

It is one of the first numbers a space physicist works out for any plasma, because comparing it with the flow speed tells you what kind of medium you are dealing with. Near Earth the solar wind blows at several times its local Alfvén speed, which is why a shock wave stands in front of the planet's magnetic field. Close to the Sun the order reverses; in 2021 Parker Solar Probe became the first spacecraft to fly through the boundary where the two speeds are equal.

The calculation takes three SI inputs: field B in tesla, total mass density ρ in kilograms per cubic metre, and permeability μ, which defaults to the vacuum value. Mass density, not particle count, is asked for deliberately, since converting one to the other means choosing what the plasma is made of. The result belongs to ideal magnetohydrodynamics: no resistivity, no kinetic effects, no relativistic correction.

What is alfvén velocity calculator?

The Alfvén velocity, v_A = B ÷ √(μρ), is the speed at which a transverse disturbance of the magnetic field, an Alfvén wave, travels along the field in a perfectly conducting fluid. It depends only on the field strength and the inertia of the material carried with the field. It is a wave speed, not the speed of the plasma itself, and the ratio of flow speed to Alfvén speed, the Alfvén Mach number, separates sub-Alfvénic from super-Alfvénic flow.

How to use this calculator.

  1. Enter the magnetic flux density in tesla. Space data usually comes in nanotesla (1 nT = 10⁻⁹ T) and older solar papers in gauss (1 G = 10⁻⁴ T).
  2. Enter the total mass density in kg/m³. For a hydrogen plasma, multiply the number of protons per cubic metre by 1.6726 × 10⁻²⁷ kg; add the mass of any helium or heavier ions.
  3. Leave the permeability at the vacuum value for any plasma or liquid metal. Change it only if you are modelling a magnetisable medium.
  4. Read the speed in m/s or km/s. The calculator refuses inputs whose speed would reach the speed of light; if the result is above a few per cent of that, see the relativistic note in the questions below.

The formula.

v_A = B / sqrt(μρ)

In magnetohydrodynamics a bent field line pulls itself straight with a tension of B²/μ per unit area, while the plasma frozen onto the field has density ρ. As with a stretched string, wave speed is √(tension ÷ density), so v_A = √(B²/(μρ)) = B ÷ √(μρ). With B in tesla, μ in henries per metre and ρ in kg/m³ the units reduce to metres per second. The speed rises in direct proportion to the field and falls with the square root of the density, so a field twice as strong doubles it, while four times the density halves it. The default μ is the 2022 CODATA value of the vacuum permeability, 1.25663706127 × 10⁻⁶ H/m; since the 2019 SI revision it is a measured constant rather than exactly 4π × 10⁻⁷, though the two differ by about one part in ten billion. The formula leaves out the displacement current, so it overstates speeds that approach that of light.

A worked example.

Example

Take a field of 0.001 T, which is 10 gauss, in a plasma of mass density 1 × 10⁻¹² kg/m³, with the vacuum permeability 1.25663706127 × 10⁻⁶ H/m. For pure hydrogen that density is about 5.979 × 10⁸ protons per cubic centimetre, conditions of the kind found in the Sun's lower corona. Multiply permeability by density: 1.25663706127 × 10⁻⁶ × 1 × 10⁻¹² = 1.2566 × 10⁻¹⁸. The square root is 1.121 × 10⁻⁹. Dividing the field by it, 0.001 ÷ 1.121 × 10⁻⁹, gives v_A = 892,062.0581 m/s, or 892.0621 km/s, just under 0.3% of the speed of light.

magnetic Field Tesla0.001
magnetic Permeability Hm0
mass Density Kg M30

Frequently asked questions.

What is the Alfvén speed in the solar wind near Earth?
With a typical field of 5 nT and 5 protons per cubic centimetre, the density is 8.363 × 10⁻²¹ kg/m³ and v_A comes to about 48.77 km/s. The wind itself blows at around 400 km/s, roughly eight times faster, so it is strongly super-Alfvénic, and Earth's magnetosphere sits behind a bow shock.
How do I convert a number density into mass density?
Multiply the ion count per cubic metre by the ion mass. For hydrogen, ρ = n × 1.6726 × 10⁻²⁷ kg, and electrons add only about one part in 1,836. A shortcut for hydrogen: v_A in km/s ≈ 21.81 × B in nT ÷ √(n in cm⁻³).
Can the result exceed the speed of light?
The bare formula can, and then it is wrong, so the calculator refuses any input that gives the speed of light or more. Once displacement current is included the wave speed becomes v_A ÷ √(1 + v_A²/c²), which never reaches c. A 1 T field in the example's 1 × 10⁻¹² kg/m³ plasma would give 8.921 × 10⁸ m/s from the bare formula, which is why the page refuses it; with the correction the speed would be about 2.842 × 10⁸ m/s.
Should I change the permeability for a plasma?
No. Plasmas and liquid metals are not magnetisable in the way iron is, so μ stays at the vacuum value; the plasma's own currents act through B instead. Editing μ only makes sense for a model of a genuinely magnetic medium.
Why are Alfvén waves hard to see in the laboratory?
Dense conductors make them slow. In liquid sodium at about 927 kg/m³ a strong 1 T field gives only 29.3 m/s, and in mercury at about 13,500 kg/m³ just 7.68 m/s, so the wave crosses a small apparatus slowly while electrical resistance damps it away.

How this page was produced

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Method
v_A = B / sqrt(μρ)
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