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Climate Modeling Theory - 1
Module 3 Climate Modeling Theory - 1 William J. Gutowski, Jr. Iowa State University
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Climate Modeling Theory - 1
Module 3 Climate Modeling Theory - 1 GOAL: Understand basis for modeling climate from (almost) first principles
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Climate Modeling Theory - 1
Module 3 Climate Modeling Theory - 1 OUTLINE (Part 1): Symbolism Conservation Laws mass thermodynamic energy momentum Equation of State Water in the Atmosphere
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Climate Modeling Theory - 1
Module 3 Climate Modeling Theory - 1 OUTLINE (Part 1): Symbolism
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Some Symbolism t time x west-east coordinate y south-north coordinate z vertical coordinate f latitude l longitude horizontal wind u west-east component of v south-north component of w vertical wind
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Climate Modeling Theory - 1
Module 3 Climate Modeling Theory - 1 OUTLINE (Part 1): Symbolism Conservation Laws mass thermodynamic energy momentum
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Conservation of “M”
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Conservation of “M”
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Conservation of “M”
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Conservation of “M”
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Conservation of “M”
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(Continuity Equation)
Conservation of Mass (Continuity Equation) = density [kg/m3] Source/sink = 0
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Conservation of Mass
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Conservation of Water Mass
q = specific humidity [kg-(H2O)v/kg-air] s(q) = cond. - evap.
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Conservation of Water Mass
(column integral) E = sfc. evap.; P = precipitation
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Conservation of W (Precipitable Water)
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Conservation of General Constituent, i [kg-(constituent i)/kg-air]
qi = amount of i [kg-(constituent i)/kg-air] e.g., CO2, O3, etc.
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= heating/mass [J-kg-1-s-1] Conservation of Thermodynamic Energy
~ First Law of Thermodynamics ~ Heat input = D (internal energy) + (work done) = heating/mass [J-kg-1-s-1]
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Conservation of Thermodynamic Energy ~ First Law of Thermodynamics ~
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Conservation of Thermodynamic Energy
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RNET FSH RNET
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Conservation of Momentum
~ Newton’s Second Law ~
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Conservation of Momentum
~ Newton’s Second Law ~ Forces/mass: gravity pressure gradient friction
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Conservation of Momentum
~ Newton’s Second Law ~ Rotating Frame X
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Conservation of Momentum
~ Newton’s Second Law ~ Rotating Frame
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Conservation of Momentum
~ Newton’s Second Law ~ Sphere, Rotating Frame rotation of direction
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Conservation of Momentum Approximation: vertical
~ Newton’s Second Law ~ Approximation: vertical
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Conservation of Momentum Approximation: vertical
~ Newton’s Second Law ~ Approximation: vertical
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Conservation of Momentum Approximation: vertical
~ Newton’s Second Law ~ Approximation: vertical Hydrostatic Approximation Accurate to ~ 0.01% for weak vertical acceleration
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Conservation of Momentum Approximation: horizontal, extratropical
~ Newton’s Second Law ~ Approximation: horizontal, extratropical
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Conservation of Momentum Approximation: horizontal, extratropical
~ Newton’s Second Law ~ Approximation: horizontal, extratropical
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Conservation of Momentum Approximation: horizontal, extratropical
~ Newton’s Second Law ~ Approximation: horizontal, extratropical Geostrophic Approximation Accurate to ~ %
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Climate Modeling Theory - 1
Module 3 Climate Modeling Theory - 1 BREAK
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Climate Modeling Theory - 1
Module 3 Climate Modeling Theory - 1 OUTLINE (Part 1): Symbolism Conservation Laws mass thermodynamic energy momentum Equation of State
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Ideal Gas Law R = gas constant R = R(constituents) Common practice: R ≈ Rd = 287 J-kg-1-s-1 T = Tv
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Climate Modeling Theory - 1
Module 3 Climate Modeling Theory - 1 OUTLINE (Part 1): Symbolism Conservation Laws mass thermodynamic energy momentum Equation of State Water in the Atmosphere
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q versus latitude & pressure
[g-kg-1] Note: small part of atmosphere, but ...
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… water saturates changes phase
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Some Further Symbolism
q specific humidity [kg-kg-1] mass (H2O)v/mass air e vapor pressure [Pa] partial pressure by water molecules m mixing ratio [kg-kg-1] mass (H2O)v/mass dry air RH relative humidity [%] ratio: m/msat
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Water Cycle Q Q P P E E R
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Water Cycle Heat released E Heat absorbed
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Water is thus a primary form of heat transport
heat absorbed when evaporates released when water condenses largest individual source of energy for the atmosphere
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Water Cycle Radiation absorbed by water & re-emitted
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Water is thus a primary form of heat transport
heat absorbed when evaporates released when water condenses largest individual source of energy for the atmosphere and greenhouse gas ~ transparent to solar absorbs/emits infrared
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RH vs. latitude & pressure
[%] RH 70 70
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precipitation vs. latitude & longitude
[dm-yr-1] [dm-yr-1] = [100 mm-yr-1] =[0.27 mm-d-1]
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Lift Moist Parcel z 9.8 K/km T
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Lift Moist Parcel z T z RH
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Lift Moist Parcel z Lifting Condensation Level T z LCL RH 100 %
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Stable Precipitation condensation collision coalescence
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Stable Precipitation condensation collision coalescence
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Lift Further z LCL T
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Lift Further z Environment’s T(z) T
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Lift Further z Environment’s T(z) T
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Lift Further Level of free convection z T
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Convection Level of free convection z T
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Climate Modeling Theory - 1
Module 3 Climate Modeling Theory - 1 Final Question: How much heating by condensation?
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Use 1st Law of Thermodynamics
Assume: no work done = heating/mass [J-kg-1-s-1]
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Apply to precipitating column
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Apply to precipitating column
Heat released µ Mass condensed µ Mass falling out P [m/s]
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Apply to precipitating column
Heat released µ Mass condensed µ Mass falling out Prw [kgw-m-2-s-1]
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Apply to precipitating column
Heat released = LPrw [J-m-2-s-1] Prw [kgw-m-2-s-1]
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Apply to precipitating column
Heat released = LPrw [J -m-2-s-1] Mass heated = ps/g [kgair-m-2]
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Apply to precipitating column
Heat released = LPrw [J -m-3-s-1] Mass heated = ps/g [kgair-m-2] = Heating/mass = LPrwg/ps [J -(kgair)-1-s-1]
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How much heating by condensation?
P = 1000 mm-yr-1 = m-s-1 Ps = 1000 hPa =10+5 Pa dT/dt = deg-s-1 = 0.67 deg-day-1 (Radiation ~ -1 deg-day-1)
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Climate Modeling Theory - 2
Coming: Module 5 Climate Modeling Theory - 2 OUTLINE (Part 2): Radiation Surface Processes Earth System
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