Figure 3.
Predicted number of breaks for a disc with a given initial geometry, shown as a function of the surface density and temperature power-law exponents p and s. The radial extent of the disc is given as $r_{\rm disc} = \left[ r_{\rm {in}} , r_{\rm {out}} \right]$ and the initial scale height is given at a distance of $r = 5a_{\rm b}$. The central binary is an equal-mass binary with eccentricity $e_{\rm b} = 0.5$. Left: Initial inner radius and scale height. Middle: Effect of a larger inner disc radius. Right: Effect of a larger disc aspect ratio. The ‘$\times$’ in each panel marks the disc parameters used in our multiple break simulation (Section 3.3). Disc inclination is not considered as a factor in these plots, but the effect is expected to be small as long as the disc is far from the critical inclination (see Section 5.1 for details).

Predicted number of breaks for a disc with a given initial geometry, shown as a function of the surface density and temperature power-law exponents p and s. The radial extent of the disc is given as |$r_{\rm disc} = \left[ r_{\rm {in}} , r_{\rm {out}} \right]$| and the initial scale height is given at a distance of |$r = 5a_{\rm b}$|⁠. The central binary is an equal-mass binary with eccentricity |$e_{\rm b} = 0.5$|⁠. Left: Initial inner radius and scale height. Middle: Effect of a larger inner disc radius. Right: Effect of a larger disc aspect ratio. The ‘|$\times$|’ in each panel marks the disc parameters used in our multiple break simulation (Section 3.3). Disc inclination is not considered as a factor in these plots, but the effect is expected to be small as long as the disc is far from the critical inclination (see Section 5.1 for details).

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