4. Results: dusty case up previous next
4.a. Feature of dust mixing (2)

Figure 10b: Dust mixing of the second day after the switch-on of dust injection. Results of every 1 hour from LT = 07:00 to 18:00 are shown. (Upper panel) Mixing ratio of dust (kg/kg). Areas of the value of dust mixing ratio larger than 1.0×10-8 are colored. (Lower panel) Turbulent diffusion coefficient. Areas of the value larger than 1.0×10-5 are colored.


Dust, which has been mixed and spread up to about 10 km height, is further transported upward into the stratosphere. Figure 10b (upper panel) shows the distribution of dust mixing ratio of the second day after the switch-on of dust injection. In the afternoon at the altitudes of around 10 km height, dust moves upward taking the form of plumes. The distribution of turbulent diffusion coefficient (Figure 10b (lower panel)) suggests that these plumes are accompanied with a vertical mixing process which is different from the km-size thermal convection near the surface.

The vertical mixing of those altitudes is caused by the vertical difference of radiative heating associated with the vertical contrast of dust density. As a result of dust injection and mixing of the first day, a region with a large vertical gradient of dust mixing ratio forms at the altitudes from 11 to 13 km height (Figure 11a). Associated with this, there appears large difference of solar radiative heating between the regions below and above the height of around 11 to 13 km (Figure 11g, Figure 11h). Consequently, inversion of potential temperature occurs between the levels of about 10km height and above, and the layer becomes convectively unstable. The vertical distribution of the horizontal mean potential temperature (Figure 11d (right panel)) shows that the unstable layer is rapidly stabilized and potential temperature of the altitudes from 10 to 15 km becomes vertically uniform. The upward transport of dust into the stratosphere is a direct result of the heating of dust solar absorption; dust is no longer a passive tracer in this region.

The vertical profile of horizontal mean dust mixing ratio does not change greatly at the 4th day and after (Figure 11b). In the convection layer, dust mixing ratio slightly increases as the depth of the convection layer decreases. In the region above the convection layer, dust mixing ratio slightly decreases because of the gravitational sedimentation of dust.


Horizontal mean fields during dust injection occurs


A numerical simulation of thermal convection in the Martian lower atmosphere.
Odaka, Nakajima, Ishiwatari, Hayashi,   Nagare Multimedia 2001
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