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Clouds (Condensed PPT)
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Clouds take different shapes and “looks”
Shape (and “look”) of a cloud determined by its Altitude (thus temperature) Water content and distribution Maritime clouds: fewer, bigger drops Continental clouds: more, smaller droplets Vertical velocity Cumulus clouds (vertically grown, “puffy looking”) indicate instability Fast(er) upward velocities Stratus clouds: often “forced” ascent (not buoyant) Slow(er) upward velocities
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Cloud droplets form by condensation
“Spontaneous” condensation (vapor liquid, without anything to condense onto) is rare Occurs in very cold, very supersaturated conditions “Regular” condensation onto a cloud condensation nucleus (CCN) is much more common Requires only supersaturation Cool the air parcel and/or moisten it will give supersaturation Lots of processes yield cooling, several processes yield moistening Larger radii CCN are more efficient at promoting condensation (more surface area
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Warm clouds (no/little ice)
Maritime clouds: fewer CCN, thus fewer droplets that are larger in radius Continental clouds: more CCN, thus more droplets that are smaller in radius Large droplet size x-axis: number of droplets per volume. More droplets per volume means they are smaller y-axis: % of droplets a large volume of air that have those # of droplets High concentrations of CCN
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As an air parcel rises, it entrains some environmental air into itself
That dry air evaporates some of the smallest cloud droplets At the edge of a cloud, entrainment can be pretty large, enough to cool the parcel (remember, evaporation takes sensible heat from the parcel and stores it in the H2O molecule as latent heat) and stop it from rising Parcels rising in the core of the cloud don’t entrain much Undiluted parcel Diluted parcel Rising parcel near the edge of the cloud mixes in drier environmental air as it rises significant evaporation/cooling parcel stops rising Rising parcel in the center of the cloud mixes in other “cloudy” air as it rises little evaporation/cooling parcel continues to rise
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Typical sizes: CCN (very small): 0.1 μm Cloud droplet: μm Small rain drop: 100 μm Typical rain drop: 1000 μm
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Warm rain development How do rain drops form?
Condensation onto CCN Cloud droplets Cloud droplets grow by condensation Cloud droplets bump into each other (collide) They combine with each other (coalesce) Bigger droplets bump into smaller droplets Grow even bigger! Eventually cloud droplets grow so large they cannot be supported by the cloud updraft Cloud droplets start to fall, colliding and coalescing with even more smaller droplets Rain occurs! Called the “collision-coalescence process”
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Cold precipitation processes
Involve ice! Main ideas: Cloud droplets remain liquid at temperatures well below 0°C If their temperatures are below 0°C, they’re called “supercooled” droplets Super-cooled droplets will freeze when they come in contact with an ice nucleus Lots of things can serve as ice nuclei The original CCN A different particle Other ice crystals / fragments However, freezing supercooled cloud droplets is not the main process by which snow forms Instead, a particle called a deposition nucleus favors the direct deposition of water onto it I.e., the water vapor molecules go directly from vapor ice
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More on deposition One of the neat properties of liquid, and ice, phases of water is that they have different saturation vapor pressures Liquid water has a higher saturation vapor pressure than solid ice Consequence #1: supersaturation of an air parcel is higher if ice is present Consequence #2: vapor molecules “prefer” to change phase directly from vapor ice In most clouds, both ice crystals and liquid cloud droplets co-exist The above 2 consequences mean that the when liquid droplets get close to ice crystals (but not touching), they will: Evaporate into vapor Then deposit as ice
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Some cool properties of cold clouds
The shape of the ice crystal that forms via deposition depends strongly on its temperature Snowflakes are actually “aggregates of dendrites Dendrites ~ −10 to −18℃ Sector plates ~ −10 to −40℃ Rosettes ~ below −40℃ Hexagonal plates ~ 0 to −10℃ subsaturated wrt water Columns/needles ~ 0 to −10℃ saturated wrt water Aggregations of ice crystals that fall relative to the ground (at speeds generally about 1 m/s) are what you know as snowflakes
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Typical clouds The bottom part is all water
The middle part is supercooled water The top part is all ice The part that is all ice is called “glaciated” Sometimes, when an ice fragment touches a supercooled cloud droplet, the droplet freezes from the outside-in As the inner part freezes, it expands and “blows up” the cloud droplet, creating many tiny ice fragments that can then serve as ice nuclei ice Supercooled water
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Microphysical “pathways” to develop precipitation-sized particles from water vapor can be quite complex, but some common ones are as follows: Convective precipitation (e.g., in a thunderstorm): Ice growth by vapor deposition / ice multiplication Particles held aloft by updraft or recycled into updraft experience heavy riming increasing their mass Particles eventually fall out of the updraft or overcome it and begin to fall relative to the ground Particles melt above 0℃ Raindrops reach the surface Stratiform precipitation (often produced by gentle, large-scale lifting): Ice growth by vapor deposition Once formed, ice crystals descend relative to the ground (situations where fall speed of ice > vertical uplift velocities defines stratiform precipitation) Ice crystals aggregate (and perhaps lightly rime) as they approach the melting layer (if it exists) Raindrops, snowflakes, or sleet reaches the surface In extreme cases, ice particles held aloft by strong updrafts can collide with larger supercooled drops that coat their surface before freezing. As this process continues, layers of ice will build up on the particle increasing its weight until it is either lofted out of the updraft or can no longer be supported by it. These are hailstones and in very extreme situations, they can grow quite large
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What about snow, sleet, freezing rain, and rain?
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