Figures & data
![](/cms/asset/87d3f3d3-875c-4922-8157-ad143b2491c3/taos_a_1769449_uf0001_c.jpg)
Figure 1. (a) The observed (black) and simulated (red/blue for control/sensitivity experiments) tracks. (b) The observed (black) and simulated (red/blue for control/sensitivity experiments) MSLPs (solid, hPa) and MSWs (dashed, m s−1), (c) surface heat fluxes (W m−2) averaged within a 100 km radius from the TC center, and (d) 850–200-hPa wind shear magnitude (solid line) and direction (dashed line) in a 600-km box centered on the TC. The SST-1 and CTL experiments are denoted by blue and red lines in each panel, respectively. The gray shading indicates the RI period.
![Figure 1. (a) The observed (black) and simulated (red/blue for control/sensitivity experiments) tracks. (b) The observed (black) and simulated (red/blue for control/sensitivity experiments) MSLPs (solid, hPa) and MSWs (dashed, m s−1), (c) surface heat fluxes (W m−2) averaged within a 100 km radius from the TC center, and (d) 850–200-hPa wind shear magnitude (solid line) and direction (dashed line) in a 600-km box centered on the TC. The SST-1 and CTL experiments are denoted by blue and red lines in each panel, respectively. The gray shading indicates the RI period.](/cms/asset/a61bcd43-4c58-4df2-80f2-a0553b4bdea2/taos_a_1769449_f0001_c.jpg)
Table 1. Configuration of parameters in WRF model.
Figure 2. Observed 85-GHz microwave image of Typhoon Mujigae (a) at 0600 UTC and (b) at 1200 UTC 3 October 2015. (c–d) the simulated (CTL) maximum ice-phase mixing ratio (g kg−1) at heights of 8–10 km. The times are the same as in (a–b). (c–f) As in (c–d) but for the SST-1 experiment.
![Figure 2. Observed 85-GHz microwave image of Typhoon Mujigae (a) at 0600 UTC and (b) at 1200 UTC 3 October 2015. (c–d) the simulated (CTL) maximum ice-phase mixing ratio (g kg−1) at heights of 8–10 km. The times are the same as in (a–b). (c–f) As in (c–d) but for the SST-1 experiment.](/cms/asset/775155c8-e98e-486f-b55f-3b9716961f31/taos_a_1769449_f0002_c.jpg)
Figure 3. The averaged upper-tropospheric potential vorticity (PVU) at z = 10–15 km, horizontal wind vectors at z = 2 km and deep convection (black crosses) for the CTL simulation (left panel) at (a) 1800 UTC, (b) 2100 UTC 2 Ocotober, (c) 0000 UTC, (d) 0300 UTC, and (e) 0600 UTC 3 October. (f–j) As in (a–e) but for the SST-1 experiment (right panel).
![Figure 3. The averaged upper-tropospheric potential vorticity (PVU) at z = 10–15 km, horizontal wind vectors at z = 2 km and deep convection (black crosses) for the CTL simulation (left panel) at (a) 1800 UTC, (b) 2100 UTC 2 Ocotober, (c) 0000 UTC, (d) 0300 UTC, and (e) 0600 UTC 3 October. (f–j) As in (a–e) but for the SST-1 experiment (right panel).](/cms/asset/f201b0b3-ece0-4e3c-94ee-10b24b8abe73/taos_a_1769449_f0003_c.jpg)