Deep Convection Shallow cumulus Photo: Bjorn Stevens Cumulus congestus Wikimedia The large-scale circulation Cloud Clusters Hadley/Walker Circulation Land/Sea Circulation stratocumulus tradewinds trade winds EQ warm, western tropical oceans cold, eastern subtropical ocean Clouds are not just visual expressions of the state of the atmosphere, or a collection of small droplets that produce considerable rainfall, rather, they are a crucial component of the dynamics of the atmosphere as a whole Stevens (2005) New Features • Precipitating (often intensely) • Updraft velocities can reach 50 m s-1 • Updrafts and downdrafts (evaporation of condensate) important • Development of anvils • Severe weather (pluvials, hail, tornadoes …) • Can be more organized (squall lines, mesoscale convective systems, supercells…) Cumulonimbus lifecycle “Air Air--Mass Mass”” Showers: Credit: K. Emanuel, MIT 1 Microbursts • Intense downdraft hits ground, spreads radially • Dry microburst: high cloud base, light rain evaporates into downdraft, accelerating it • Wet microburst: weight of suspended rain in wet conditions accelerates downdraft Credit:Wikipedia Denver, CO - July 1, 1993 12Z 5000 ! 25000 Revised Friday, January 30, 2009! Height (m) 4000 27 20000 3000 15000 2000 10000 Conditional Instability After sinking through the trade inversion, the air is subjected to friction. This causes its angular momentum to decrease. As it flows back equatorward, near-surface easterlies result. 1000 5000 0 300 305 310 315 320 325 330 335 340 345 350 355 0 300 360 320 340 360 380 400 420 440 460 480 500 Height (m) Denver, CO - January 2, 1993 0Z 5000 4000 5000 25000 4000 20000 Denver, CO - July 1, 1993 12Z 3000 15000 25000 2000 10000 20000 Height (m) 1000 3000 5000 15000 0 0 285 290 295 300 305 310 315 320 325 330 335 340 300 320 340 360 380 400 420 440 460 Barrow, AK - July 1, 1993 12Z 5000 2000 25000 10000 0 300 305 310 Height (m) 4000 1000 20000 5000 3000 15000 Kelvin 3152000 320 325 330 335 340 345 350 moist static energy (h) 355 0 10000 300 360 320 340 360 saturation moist static energy (h*) 420 440 460 480 500 5000 dry static energy (s) 275 280 285 290 295 4000 300 305 310 315 0 260 320 280 300 320 340 360 380 400 420 440 460 480 500 20000 Barrow, AK - January 2, 1993 0Z 5000 3000 25000 15000 Height (m) 4000 2000 1000 20000 3000 15000 10000 2000 10000 5000 1000 290 295 300 5000 0 245305 250310 255315 260320 265325 270330 275335 280340 285 0 0 240 280 260 300 280 300 320 320 Kelvin moist static energy (h) Barrow,saturation moist static energy 12Z (h*) AK - July 1, 1993 5000 400 25000 0 270 0 285 380 Denver, CO - January 2, 1993 0Z 1000 5000 Height (m) 280 340 340 360360380 400 380 420 440 400 460420 440 460 dry static energy (s) 25000 Figure 6.12: Representative observed soundings for 20000 Denver, Colorado, and Barrow, Alaska, for July and January. The curves plotted show the dry static energy, the moist static energy, and the saturation moist 3000 static energy. The panels on the right cover both the 15000 troposphere and lower stratosphere, while those on the right zoom in on the lower troposphere to show more detail. Values are divided by c p to give units in Height (m) 4000 2000 10000 1000 5000 K. Credit: D. Randall CAPE (from LFC to LNB) Gives upper bound on updraft vertical velocity CIN (from ground to LFC) Land vs. Ocean • 2-3 stronger over land (TP) than over oceans (GATE) • Often more CAPE over land (but upper bound from CAPE not reached because of entrainment) Entrainment dilution Observations @ 10N, 95W CRM (colors: vertical mass flux) Credit: C. Bretherton, UW Transition to strong convection 2370 2370 J O UJR OTS M PH I ES NCCIEESN C E S ONUARLN O A FL TOHFETA HTEMA OES R P IHCE S RCI C VOLUMEV66 OLUME 66 w/wc Neelin et al. 2009
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