In this question, the coefficient multiplying is the magnetic diffusivity. Denote it ; it is the paper's , with dimensions of length squared per time. If denotes electrical resistivity, then . The two conventions must not be interchanged.
For an imposed real positive , retain the momentum equation and use
Elimination gives the exact Resistive damping of an Alfvén wave relation
Here is complex because the driving frequency is real. Introduce the dimensionless diffusion parameter . For propagation and attenuation along , choose the square-root branch with . The spatial damping of a driven Alfvén wave is
With the convention , the amplitude decays as . Define its e-folding length and the wavelength . Then
If damping length instead refers to wave energy, the squared amplitude decays twice as fast: and . Stating the convention avoids a factor-of-two ambiguity. The temporal damping rate at fixed real is a different specification from this imposed-frequency problem.
Figure 1.
Weak spatial attenuation of a driven Alfvén wave and its amplitude envelope
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Spatial damping of a driven Alfvén wave Created 2026-10-25 Updated 2026-11-05
For fixed real positive angular frequency , a transverse Alfvén wave proportional to in a uniform fluid has when magnetic diffusivity is retained and viscosity is neglected. Choose the branch with positive real and imaginary parts for propagation and attenuation along . For , . The amplitude attenuation length is , whereas the energy attenuation length is . With wavelength , and . Fixed-real-wavenumber temporal Resistive damping of an Alfvén wave is a different boundary-value prescription.