We present direct numerical simulations of inhomogeneous reduced magnetohydrodynamic (RMHD) turbulence between the Sun and the Alfvén critical point. These are the first such simulations that take into account the solar-wind outflow velocity and the radial inhomogeneity of the background solar wind without approximating the nonlinear terms in the governing equations. RMHD turbulence is driven by outward-propagating Alfvén waves (z+ fluctuations) launched from the Sun, which undergo partial non-WKB reflection to produce sunward-propagating Alfvén waves (z− fluctuations). We present 10 simulations with different values of the correlation time and perpendicular correlation length L⊥☉ of outward-propagating Alfvén waves at the coronal base. We find that between 15% and 33% of the z+ energy launched into the corona dissipates between the coronal base and Alfvén critical point. Between 33% and 40% of this input energy goes into work on the solar-wind outflow, and between 22% and 36% escapes as z+ fluctuations through the simulation boundary at r = rA. The z± power spectra scale like , where k⊥ is the wavenumber in the plane perpendicular to B0. In our simulation with the smallest value of (∼2 minutes) and largest value of L⊥☉ (2 × 104 km), we find that α+ decreases approximately linearly with increasing ln (r), reaching a value of 1.3 at r = 11.1 R☉. Our simulations with larger values of exhibit alignment between the contours of constant ϕ+, ϕ−, , and , where ϕ± are the Elsässer potentials and are the outer-scale parallel Elsässer vorticities.
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Perez et al. (2013) studied this question.
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