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Fig. 3

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Left column: log   ( − Be) and | h/r | for the new equilibrium torus solution described in the text. The Bernoulli parameter is shown as a function of (r,θ) and as a function of r at the midplane. The torus is energetically bound, i.e., Be < 0. Right column: log   (Be) and | h/r | for a solution of Chakrabarti (1985) which is energetically unbound, i.e., Be > 0. Note that the unbound torus is actually thinner than the bound torus in this example.

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