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The Stability of Self-Gravitating Polytropic Tori
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J. W. Woodward, J. E. Tohline, & I. Hachisu (1994; hereafter WTH94) used nonlinear numerical hydrodynamic techniques to examine the relative stability of self-gravitating, polytropic tori toward the development of nonaxisymmetric structure. The following pair of tables list key properties of the set of model tori that were examined: Table 5 gives characteristics of the initial models and Table 6 presents results ascertained from the numerical stability analyses.
Table extracted from J. W. Woodward, J. E. Tohline & I. Hachisu (1994)
"The Stability of Thick, Self-gravitating Disks in Protostellar Systems"
ApJ, vol. 420, pp. 247-267 © American Astronomical Society | |
Online Movies
Figure 1: Animation Sequences to Supplement Figure 10 of WTH94 (click on security-lock icon or caption model name to go to YouTube) | ||
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Table 5, Model O15 | Table 5, Model O14 | |
Table 5, Model E17 | Table 5, Model E29 | |
Caption to Fig. 10 from WTH94: "<math>~\phi_m - r</math>" diagrams illustrating the azimuthal structure of the four specific eigenmodes that were found to be dynamically unstable in our modeled disks. (a) The m = 1 P-mode, shown here as it developed in model O15 <math>~[M_d/M_c = 1; ~T/|W| = 0.316];</math> (b) The m = 1 A-mode, shown here as it developed in model O14 <math>~[M_d/M_c = 1; ~T/|W| = 0.251];</math> (c) The m = 2 I-mode, shown here as it developed in model E17 <math>~[M_d/M_c = 5; ~T/|W| = 0.256];</math> (d) The m = 2 L-mode, shown here as it developed in model E29 <math>~[M_d/M_c = 0.2; ~T/|W| = 0.447]\, .</math> |
Figure 2: Five Additional Animation Sequences to Supplement Table 5 of WTH94 (click on security-lock icon or caption model name to go to YouTube) | ||||
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Table 5, Model O13 | Table 5, Model O16 | Table 5, Model O17 | Table 5, Model O18 | Table 5, Model O22 |
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