dr. michael maccracken, the climate institute, washington, dc

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Family Homecoming Special Event "Can Climate Engineering Serve as a Complementary Step to Aggressive Mitigation?" Dr. Michael MacCracken, The Climate Institute, Washington, DC Friday, Sept. 25 at 4:00 pm in Olin 1, with cookies

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Family Homecoming Special Event "Can Climate Engineering Serve as a Complementary Step to Aggressive Mitigation?". Dr. Michael MacCracken, The Climate Institute, Washington, DC Friday, Sept. 25 at 4:00 pm in Olin 1, with cookies. Clouds Precipitation Read Anthes 2 and begin 3. - PowerPoint PPT Presentation

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Page 1: Dr. Michael MacCracken, The Climate Institute, Washington, DC

Family Homecoming Special Event

"Can Climate Engineering Serve as a Complementary Step to Aggressive Mitigation?"

Dr. Michael MacCracken, The Climate Institute, Washington, DC

Friday, Sept. 25 at 4:00 pm in Olin 1, with cookies

Page 2: Dr. Michael MacCracken, The Climate Institute, Washington, DC

CloudsPrecipitation

Read Anthes 2 and begin 3

Page 3: Dr. Michael MacCracken, The Climate Institute, Washington, DC

Other special types

Orographic - clouds that form via interaction between wind and mountainous terrain features

Artificial clouds - contrails

Instability waves generated by wind shear (waves are always there, but are visible when there is moisture condensing in them

Page 4: Dr. Michael MacCracken, The Climate Institute, Washington, DC

Cloud Photos

Plymouth State UniversityMeteorology Program

Cloud Boutiquehttp://vortex.plymouth.edu/clouds.html

Page 5: Dr. Michael MacCracken, The Climate Institute, Washington, DC

Precipitation and Energy

Page 6: Dr. Michael MacCracken, The Climate Institute, Washington, DC

Mark’s Photos

Page 7: Dr. Michael MacCracken, The Climate Institute, Washington, DC

Precipitation and Energy

Page 8: Dr. Michael MacCracken, The Climate Institute, Washington, DC
Page 9: Dr. Michael MacCracken, The Climate Institute, Washington, DC

Fog is a Cloud on the Ground

How Fog is Formed

Radiation fog (local)-- Radiational cooling of a shallow moist layer with dry layer above it. Dissipates with morning sun.

Evaporation fog (local) -- Cold air in contact with a warmer water surface (e.g. lakes in autumn).

Upslope fog (mountains) -- gentle lifting of a moist layer.

Advection fog (regional) -- warm moist air moves over a cold surface. E.g. Pacific coast cold ocean surface.

Precipitation fog (regional) -- warm rain falls through a layer of cold air or over a snowfield.

Page 10: Dr. Michael MacCracken, The Climate Institute, Washington, DC

Fog, 8:00 am Sept. 14th

Page 11: Dr. Michael MacCracken, The Climate Institute, Washington, DC

No fog, 8:45 am Sept. 14th

Page 12: Dr. Michael MacCracken, The Climate Institute, Washington, DC

Fog, 6:30 am Sept. 17th

Page 13: Dr. Michael MacCracken, The Climate Institute, Washington, DC

No fog, 8:30 am Sept. 17th

Page 14: Dr. Michael MacCracken, The Climate Institute, Washington, DC

Divergence and Convergence:Bays and Headlands

Page 15: Dr. Michael MacCracken, The Climate Institute, Washington, DC

Clouds Are Formed by Lifting

Page 16: Dr. Michael MacCracken, The Climate Institute, Washington, DC

PrecipitationPrecipitation

Terminal velocity > updraft velocity Drops must be large enough to fall to ground and not evaporate.

Otherwise we call them “fall streaks.”

Page 17: Dr. Michael MacCracken, The Climate Institute, Washington, DC

Comparison of Droplet

Sizes

Page 18: Dr. Michael MacCracken, The Climate Institute, Washington, DC

How do cloud droplets grow?

Curvature effect (-)The greater the curvature of a droplet, the greater the rate of evaporation.

So small droplets tend to disappear unless the air is supersaturated.

Solute effect (+)Hygroscopic salt particles in a droplet slow the rate of evaporation,

allowing small droplets to grow larger.

Collision-Coalescence ProcessDrops of different sizes fall at different rates. Big drops sweep up little

drops.

Droplets collide and grow.

1 raindrop = 1 million cloud droplets

Page 19: Dr. Michael MacCracken, The Climate Institute, Washington, DC

Ice Crystal Process

Cold cloud process (ice and supercooled water droplets)

Water evaporates and deposits onto ice crystals

Ice crystals grow at expense of water droplets because of es

Snow forms most of our precipitation (even in summer!)

Page 20: Dr. Michael MacCracken, The Climate Institute, Washington, DC

The Ice Crystal Process

Wegener-Bergeron-FindeisenTheory

Since ice crystals have a lower saturation vapor pressure than water droplets, molecules migrate from the droplets to the ice. The ice grows at the expense of the water droplets.

Clouds can be “seeded” by chemicals like Silver Iodide which have hexagonal structure. They can be supercooled by substances like Dry Ice.

Page 21: Dr. Michael MacCracken, The Climate Institute, Washington, DC

Saturation vapor

pressure as a function of T for ice and

water surfaces

Page 22: Dr. Michael MacCracken, The Climate Institute, Washington, DC

Important terms

Divergence<-------------- O --------------->

Convergence--------------> O <--------------

SupersaturationRH > 100% due to curvature of droplets

SupercooledCloud droplets can remain liquid at T < 0

Page 23: Dr. Michael MacCracken, The Climate Institute, Washington, DC

Hydrologic Cycle

Page 24: Dr. Michael MacCracken, The Climate Institute, Washington, DC

“Clouds in a glass of beer”

Clouds = liquid droplets suspended in gas.

Beer = gas droplets suspended in liquid.

CO2 at 2 atm. in the bottle = supersaturated.

Rapid expansion: T goes from 5 C to -36 C

Water vapor condenses in neck of bottle.

Bubbles in glass do not form randomly, but at nucleation sites.

Bubbles (rain) reach an upward terminal velocity (buoyancy vs. drag)

Beer clouds can be “seeded” with explosive results.

White foam is thin -- scattering at all wavelenghts.

Yellow liquid is dense -- short, blue wavelenghts absorbed.