Figure 3
Profiles from Run 1 at times tO+ 0.2 kyr (i.e. just after the primary protostar appears), tO+ 4.2 kyr, tO+ 8.1 kyr (i.e. the stage at which the disc becomes well established), tO+ 12.1 kyr, tO+ 16.0 kyr and tO+ 19.9 kyr (the end of the simulation). (a) The radial-density profile on the equatorial plane, ρ(r, z= 0). The axes are logarithmic, and a line with slope − 2.5 is shown to mimic the run of density in the disc between 10 and 200 au. The key gives the line-styles used to represent the different times. (b) The radial- temperature profile on the equatorial plane, T(r, z= 0). The axes are logarithmic, and a line with slope − 0.6 is shown to mimic the run of temperature in the disc between 10 and 200 au. (c) The radial-velocity profile on the equatorial plane, vr(r, z= 0). The velocity axis is linear, and velocity is given in units of the local sound speed. The radius axis is logarithmic. (d) The azimuthal velocity profile on the equatorial plane, vφ(r, z= 0). The axes are logarithmic, and lines with slopes of −1/2 and −1/4 are included to show that in the disc vφ∝r−1/4, corresponding to non-Keplerian differential rotation. Note that this plot has a larger radial extent than the others. (e) The radial profile of the disc aspect ratio, . Both axes are linear.

Profiles from Run 1 at times tO+ 0.2 kyr (i.e. just after the primary protostar appears), tO+ 4.2 kyr, tO+ 8.1 kyr (i.e. the stage at which the disc becomes well established), tO+ 12.1 kyr, tO+ 16.0 kyr and tO+ 19.9 kyr (the end of the simulation). (a) The radial-density profile on the equatorial plane, ρ(r, z= 0). The axes are logarithmic, and a line with slope − 2.5 is shown to mimic the run of density in the disc between 10 and 200 au. The key gives the line-styles used to represent the different times. (b) The radial- temperature profile on the equatorial plane, T(r, z= 0). The axes are logarithmic, and a line with slope − 0.6 is shown to mimic the run of temperature in the disc between 10 and 200 au. (c) The radial-velocity profile on the equatorial plane, vr(r, z= 0). The velocity axis is linear, and velocity is given in units of the local sound speed. The radius axis is logarithmic. (d) The azimuthal velocity profile on the equatorial plane, vφ(r, z= 0). The axes are logarithmic, and lines with slopes of −1/2 and −1/4 are included to show that in the disc vφr−1/4, corresponding to non-Keplerian differential rotation. Note that this plot has a larger radial extent than the others. (e) The radial profile of the disc aspect ratio, formula. Both axes are linear.

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