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Fig. 10

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Effect of local enhancements in the vertically integrated dust-to-gas mass ratio on the equilibrium solution by imposing fdg to be radially variable with a local Gaussian perturbation at various locations (see the dust-to-gas mass ratio profiles in Fig. F.3). The unperturbed value of fdg is the same for all the simulations, equal to 10−2. The ”5 au (10×)” case (blue) corresponds to dust enhancement at r = 5 au, where fdg varies from its unperturbed value to 10−1. The “5 au (5×)” case (dark orange) is similar to the previous case, but fdg goes up to 5 × 10−2 instead. The “DZOE (10×)” case (green) corresponds to dust enhancement at the expected dead zone outer edge (DZOE) location for the fiducial model (r = 23 au), where fdg varies from its unperturbed value to 10−1. The “DZOE (5×)” case (red) is similar to the previous case, but fdg goes up to 5 × 10−2 instead. The “60 au (10×)” case (purple) corresponds to dust enhancement at r = 60 au, where fdgvaries from its unperturbed value to 10−1. The “60 au (5×)” case (brown) is similar to the previous case, but fdg goes up to 5 × 10−2 instead. The ”No dust enhancement” case (gray) corresponds to the fiducial model. The panels show the various steady-state profiles of some key quantities, for the model parameters M = 1 M, L = 2 L, Mdisk = 0.05 M, adust = 1 μm, and αhydro = 10−4. Panels a–e show the same key quantities as in Fig. 7. Panel f: deviation from Keplerian velocity, where vϕ, gas is the azimuthal gas velocity and vK = K is the Keplerian velocity. The dotted black line corresponds to vϕ, gas = vK.

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