Figure 19.
Volume filling factor (top panels) and the associated mass fraction (bottom panels) in each temperature range above the disc on both sides (|z| > 200pc) for the models with: SB wind only (C.MHD.100SF, left) and with SB + AGN wind (C.MHD.100SF.360°.L2, right) shown in five different times: t = 0.0, 0.525, 1.05, 1.575, and 2.1 Myr. The model with AGN wind removes a bigger fraction of cold and warm gas (right panels), specially after 2.1 Myr of evolution, when the AGN-wind remnant is no longer visible. This suggests that, at least at the scales studied here (< 1 kpc), the past AGN-wind activity is a determining factor in the production of cold outflows, that are the most massive component of the gas being ejected.

Volume filling factor (top panels) and the associated mass fraction (bottom panels) in each temperature range above the disc on both sides (|z| > 200pc) for the models with: SB wind only (C.MHD.100SF, left) and with SB + AGN wind (C.MHD.100SF.360°.L2, right) shown in five different times: t = 0.0, 0.525, 1.05, 1.575, and 2.1 Myr. The model with AGN wind removes a bigger fraction of cold and warm gas (right panels), specially after 2.1 Myr of evolution, when the AGN-wind remnant is no longer visible. This suggests that, at least at the scales studied here (< 1 kpc), the past AGN-wind activity is a determining factor in the production of cold outflows, that are the most massive component of the gas being ejected.

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