We present an analytical model for describing the highly relativistic acceleration of magnetically driven jets, within the framework of ideal MHD for cold, stationary, and axisymmetric outflows. Our novel procedure is to treat the wind equation as an algebraic relation between the relativistic Alfvén Mach number and the poloidal electric-to-toroidal magnetic field amplitudes ratio ξ. This allows us to obtain easily the wind solutions for trans-fast-magnetosonic flows, together with the required range of ξ. Then, to determine the spatial variation of ξ, we solve approximately the Grad-Shafranov equation applied to a jet flow ejected with a very large total specific energy E and confined within a very small opening angle. Our trans-fast-magnetosonic model provides a closed-form expression for the transition from a magnetically dominated flow to a kinetic-energy-dominated one, which occurs in the subasymptotic region far beyond the light cylinder of radius R L . Importantly, we find that the equipartition between magnetic and kinetic energies is realized at a cylindrical radius of the order of R L E / c 2 and confirm that the further conversion of magnetic to kinetic energy proceeds logarithmically with distance in the asymptotic region. Finally, we discuss briefly the astrophysical implications of our model for jets originating from active galactic nuclei.
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Tomimatsu et al. (2003) studied this question.
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