A disc-wind model with correct crossing of all magnetohydrodynamic critical surfaces
Corresponding Author
N. Vlahakis
Department of Physics, University of Crete, PO Box 2208, GR-710 03 Heraklion, Crete, Greece
★ Present address: The University of Chicago, The Enrico Fermi Institute, 5640 S. Ellis Av., Chicago, IL 60637, USA.
† E-mail: [email protected]
Search for more papers by this authorCorresponding Author
K. Tsinganos
Department of Physics, University of Crete, PO Box 2208, GR-710 03 Heraklion, Crete, Greece
★ Present address: The University of Chicago, The Enrico Fermi Institute, 5640 S. Ellis Av., Chicago, IL 60637, USA.
† E-mail: [email protected]
Search for more papers by this authorC. Sauty
Observatoire de Paris - Université Paris 7, DAEC, F-92190 Meudon, France
Search for more papers by this authorE. Trussoni
Osservatorio Astronomico di Torino, Strada Osservatorio 20, I-10025 Pino Torinese, Italy
Search for more papers by this authorCorresponding Author
N. Vlahakis
Department of Physics, University of Crete, PO Box 2208, GR-710 03 Heraklion, Crete, Greece
★ Present address: The University of Chicago, The Enrico Fermi Institute, 5640 S. Ellis Av., Chicago, IL 60637, USA.
† E-mail: [email protected]
Search for more papers by this authorCorresponding Author
K. Tsinganos
Department of Physics, University of Crete, PO Box 2208, GR-710 03 Heraklion, Crete, Greece
★ Present address: The University of Chicago, The Enrico Fermi Institute, 5640 S. Ellis Av., Chicago, IL 60637, USA.
† E-mail: [email protected]
Search for more papers by this authorC. Sauty
Observatoire de Paris - Université Paris 7, DAEC, F-92190 Meudon, France
Search for more papers by this authorE. Trussoni
Osservatorio Astronomico di Torino, Strada Osservatorio 20, I-10025 Pino Torinese, Italy
Search for more papers by this authorAbstract
The classical Blandford & Payne model for the magneto-centrifugal acceleration and collimation of a disc-wind is revisited and refined. In the original model, the gas is cold and the solution is everywhere subfast magnetosonic. In the present model the plasma has a finite temperature and the self-consistent solution of the MHD equations starts with a subslow magnetosonic speed which subsequently crosses all critical points, at the slow magnetosonic, Alfvén and fast magnetosonic separatrix surfaces. The superfast magnetosonic solution thus satisfies MHD causality. Downstream of the fast magnetosonic critical point the poloidal streamlines overfocus towards the axis and the solution is terminated. The validity of the model to disc winds associated with young stellar objects is briefly discussed.
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