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Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson partment of Civil & Environmental Engineerin Stanford University Stanford, CA 94305-4020 [email protected] March 30, 2005

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Page 1: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Presentation Slides for

Chapter 14of

Fundamentals of Atmospheric Modeling 2nd Edition

Mark Z. JacobsonDepartment of Civil & Environmental Engineering

Stanford UniversityStanford, CA [email protected]

March 30, 2005

Page 2: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Sources of New Particles

EmissionSea spraySoil dustVolcanicBiomass burningFossil-fuel combustionIndustrialMiscellaneous

Homogeneous nucleationHomomolecularBinaryTernary

Page 3: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Sea Spray EmissionForm when winds and waves force air bubbles to burst at sea

surface

Contain composition of sea water

Spume dropsDrops larger than sea spray formed when winds tear off wave crests.

Sea-spray acidificationReduction in chloride in sea spray drops as sulfuric acid or nitric acid enter the drops.

DehydrationWater loss when drop evaporates in low relative-humidity air

Page 4: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Constituents of Sea Water

Table 14.1

Constituent Mass percentWater 96.78Sodium 1.05Chlorine 1.88Magnesium 0.125Sulfur 0.0876Calcium 0.0398Potassium 0.0386Carbon 0.0027

Page 5: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Sea Spray EmissionFlux of sea spray drops per unit radius interval (Monahan)

(14.1)

(14.2)

Flux of spume drops per unit radius interval (14.1)

ΔFispray

Δri=1.373vh,10

3.411+0.057ri

1.05( )101.19e−B2

ri−3

B= 0.38−log10ri( ) 0.65

ΔFispume

Δri=

0 ri ≤10 μm

8.6×10−6e2.08vh,10ri−2 10≤ri ≤75 μm

4.83×10−2e2.08vh,10ri−4 75≤ri ≤100μm

4.83×106e2.08vh,10ri−6 100μm≤ri

⎪ ⎪ ⎪

⎪ ⎪ ⎪

Page 6: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Sea Spray EmissionFlux of sea spray drops per unit radius interval (Guelle) (14.4)

Change in number concentration of sea spray particles (14.5)

ΔFispray

Δri=0.2vh,10

3.5e−1.5ln ri 3( )

2+0.0068vh,10

3e−ln ri 30( )

2

Δni =ΔFi

spray

Δri+

ΔFispume

Δri

⎝ ⎜ ⎜

⎠ ⎟ ⎟

ΔriΔz

h

Page 7: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Sea Spray Emission

0.1

1

10

100

1000

1 10

1 10

Δ

F

i/

Δ

ri

( particles cm

-2

cm

-1

s

-1

)

10- ( / )m wind speed m s

( 86)Spray M

( 86)Spume M

ΔF/Δ

r (p

arti

cles

cm

-2 c

m-1

s-1)

Fig. 14.1

0.1

1

10

100

1000

10

4

10

5

10

6

0.1 1 10 100

Spray (M86)

Spume (M86)

SH98

0.1 1 10 100

Δ

F

i/

Δ

ri

( particles cm

-2

cm

-1

s

-1

)

(Drop radius μ )m

ΔF/Δ

r (p

arti

cles

cm

-2 c

m-1

s-1)

Page 8: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Soil Dust EmissionSoil

Natural, unconsolidated mineral and organic matter lying above bedrock on the surface of the Earth. Originates from the breakdown of rocks and decay of dead plants and animals.

RocksSedimentary: Cover 75 percent of Earth’s surface and form by deposition and cementation of carbonates, sulfates, chlorides, shell fragments. Example: chalk.

Igneous: Form by cooling of magma. Example: Granite.

Metamorphic: Form by structure transformation of existing rocks due to high temperatures and pressures. Example: Marble.

Page 9: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Breakdown of Rocks to SoilPhysical weathering

Disintegration of rocks and minerals by processes not involving chemical reactions. Examples: when stress applied to a rock. Stresses arise due to high pressure under soil or when rocks freeze/thaw or when saline solutions enter cracks and cause disintegration/fracture.

Chemical weatheringDisintegration of rocks and minerals by chemical reaction. Example: Dissolution of gypsum in water:

CaSO4-2H2O(s)

Calcium sulfatedihydrate (gypsum)

Ca2+ + SO42- + 2H2O(aq)

Calciumion

Sulfateion

Liquidwater

Page 10: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Types of Minerals in Soil DustQuartz - SiO2(s) - clear, colorless, resistant to chemical weatheringFeldspars - 50 percent of rocks on Earth’s surface

Potassium feldspar - KAlSi3O3(s)Plagioclase feldspar - NaAlSi3O3-CaAl2Si2O8(s)

Hematite - Fe2O3(s) - reddish brownCalcite - CaCO3(s) - found in limestoneDolomite - CaMg(CO3)2(s)Gypsum - CaSO4-2H2O(s)- colorless to whiteClays - soft, compact, odorous minerals resulting from weathering

Kaolinite - Al4Si4O10(OH)8(s)IlliteSmectiteVermiculiteChlorite

Organic matter - plant litter or animal tissue broken by bacteria

Page 11: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Soil Dust EmissionHorizontal flux, integrated vertically, of soil dust in saltation layer

(14.6)

Fractional cross-sectional area soil grain concentration in size bin(14.7)

(14.8)

G =2.61ρag

u*3 fsa,i 1+

u*,it

u*

⎜ ⎜

⎟ ⎟

1−u*,i

t

u*

⎜ ⎜

⎟ ⎟

2⎡

⎢ ⎢ ⎢

⎥ ⎥ ⎥ i =1

Ns

∑ Δds,i

u* >u*,it

fsa,i =AL,s,kAL,s,T

as,i,kAL,s,k

⎝ ⎜

⎠ ⎟

k=1

Nm

as,i,kAL,s,k

=Δds,i

ds,i 2π lnσg,s,kexp−

ln2 ds,i D A,s,k( )

2ln2σg,s,k

⎢ ⎢

⎥ ⎥

Page 12: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Soil Dust EmissionThreshold friction wind speed (14.9)

Threshold friction wind speed over smooth surface (14.10)

u*,it =

u*,its

feff,i

u*,its =

0.129Ki

1.928Res,i0.092−1

0.03<Res,i ≤10

0.129K, 1−0.0858e−0.0617Res,i−10( )⎡ ⎣ ⎢

⎤ ⎦ ⎥ Res,i >10

⎪ ⎪

⎪ ⎪

Page 13: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Soil Dust EmissionRatio of friction wind speed over smooth to actual surface (14.11)

Roughness length over smooth soil (14.14)

feff,i =1−

lnz0

z0,s,i

⎝ ⎜

⎠ ⎟

ln 0.3510

z0,s,i

⎝ ⎜

⎠ ⎟

0.8⎡

⎢ ⎢

⎥ ⎥

z0,s,i ≈ds,i30

Page 14: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Soil Dust EmissionFriction Reynolds number (14.12)

Threshold wind speed prefactor (14.13)

Res,i =1331ds,i1.56+0.38

Ki =ρsgds,i

ρa1+

0.006

ρsgds,i2.5

⎜ ⎜

⎟ ⎟

Page 15: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Soil Dust EmissionVertical soil dust flux (14.15)

Ratio of vertical to horizontal dust flux (14.16)

Change in soil dust concentration above saltation layer (14.17)

ΔFvertsoil=Gαs

αs ≈1013.4fclay−6

Δni =fem,iΔFvert

soil

ρsυi

hΔz

Page 16: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Volcanic EmissionOver 500 volcanos currently activeMagma contains 1-4 percent gas by mass.Water vapor makes up 50-80 percent of gas massSome other constituents:

CO2 SO2

OCS N2

CO H2

S2 HClCl2 F2

ParticlesMost abundant are silicate minerals.Range in size from <0.1 to 100 μm

Page 17: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Biomass-Burning EmissionBurning of evergreen forests, deciduous forests, woodlands,

grasslands, agricultural land either to clear land, stimulate grass growth, manage forest growth, or satisfy a ritual

Gas constituentsCO, CO2

CH4, NOx

ROGs SO2

Particle constituentsAsh, plant fibers, soil dust, organic matter, soot (black carbon plus organic matter)

Composition of soot High temperatures: Higher ratio of BC:OM in soot.

Page 18: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Fossil FuelsCoal

Combustible brown-to-black carbonaceous sedimentary rock formed by compaction of partially decomposed plant material. Stages of coal metamorphosis

Peat (unconsolidated, brown-black)Peat coal (consolidated, brown-black)Lignite coal (brown-black)Bituminous (soft) coal (dark brown to black)Anthracite (hard) coal (black)

Oil (petroleum)Natural greasy, viscous, combustible hydrocarbon liquid that forms from geological-scale decomposition of plants and animals.

Page 19: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Fossil FuelsNatural gas

Colorless, flammable gas, made primarily of methane, often found near petroleum deposits.

KeroseneCombustible, oily, water-white liquid with strong odor distilled from petroleum

DieselCombustible liquid distilled from petroleum after kerosene.

Page 20: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Fossil-Fuel Combustion EmissionGases

NOx, ROGs, CO, CO2, CH4, SO2

ParticlesSoot (BC+OM), OM alone, SO4

2-, metals, fly ash

Fly ashContains O, Si, Al, Fe, Ca, Mg.

Page 21: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Industrial Emission

Source Metals in Fly AshSmelters Fe, Cd, ZnOil-fired power plants V, Ni, FeCoal-fired power plants Fe, Zn, Pb, V, Mn, Cr, Cu, Ni, As,

Co, Cd, Sb, HgMunicipal waste incineration Zn, Fe, Hg, Pb, Sn, As, Cd, Co,

Cu, Mn, Ni, Sb

Steel-mill furnaces Fe, Zn, Cr, Cu, Mn, Ni, Pb

Table 5.5

Page 22: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Miscellaneous Particle Sources

Tire-rubber particlesPollenSpores

BacteriaViruses

Plant debrisMeteoric debris

Page 23: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Composition and Sources of Particles

Table 14.3

Nucleation Mode Accumulation Mode Coarse ModeNucleation Fossil-fuel emission Sea-spray emission

H2O(aq), SO42-, BC, OM, SO4

2-H2O(aq), Na+, Ca2+,NH4

+ Fe, Zn Mg2+, K+, Cl-, SO42-,

Br-, OM

Fossil-fuel emissionBiomass-burning Soil-dust emissionBC, OM, SO4

2-, BC, OM, SO42-, Cl- Si, Al, Fe, Ti, P,

Mn,Fe, Zn Fe, Mn, Zn, Pb, V, Co, Ni, Cr, Na+, Ca2+

Cd, Cu, Co, Sb, As, Mg2+, K+, SO42-, Cl-

Ni, Cr CO32-, OM

Page 24: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Composition and Sources of ParticlesNucleation Mode Accumulation Mode Coarse ModeBiomass burning Industrial emission Biomass-burning

ash,BC, OM, SO4

2-,Cl- BC, OM, Fe, Al, S industrial fly ash,Mn, Zn, Pb, V, P, Mn, Zn, Pb, Ba tire-particle emissionCd, Cu, Co, Sb,As, Sr, V, Cd, Cu, CoNi, Cr Hg, Sb, As, Se, Ni,

H2O(aq), NH4+, Na+,

Ca2+, K+, SO42-,

NO3-, Cl-, CO3

2-

Cond./dissolution Cond./dissolution Cond./dissolution H2O(aq), SO4

2-, H2O(aq), SO42-, H2O(aq), NO3

-

NH4+, OM NH4

+, OM

Coagulation Coagulation

Page 25: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Anthropogenic Particle Constituents Emitted in Greatest Abundance in L.A.

Table 14.4

SiliconOrganic carbonAluminumIronCalciumSulfatePotassiumBlack carbonChlorideTitaniumSulfurCarbonate ionSodium

ManganesePhosphorousNitratesZincLeadBariumAmmoniumStrontiumVanadiumCopperCobaltNickelChromium

Page 26: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

NucleationHomogeneous homomolecular

Single gas nucleates away from a surfaces

Homogeneous binaryTwo gases nucleate in tandem away from a surfaces

Homogeneous ternaryThree gases nucleate in tandem away from a surfaces

Heterogeneous homomolecularSingle gas nucleates on an existing surface

Heterogeneous binaryTwo gases nucleate in tandem on a surface

Page 27: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Classical Nucleation TheoryChange in Gibbs free energy (J) during cluster aggregation (14.18)

Saturation ratio

ΔG =4πrp2σ p−

43

πrp3ρp

R*Tmq

lnSq

Sq = pq / pq,s

Page 28: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Classical Nucleation Theory

Fig. 14.3

Change in free energy versus cluster radius

-4x10

-14

-2x10

-14

0

2x10

-14

4x10

-14

4x10

-6

8x10

-6

1.2x10

-5

1.6x10

-5

2x10

-5

Δ

( )G J

( )Particle radius cm

- Surface tension

term

- Saturation ratio

term

Sum

r

c

ΔG (

J)

Page 29: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Critical RadiusMinimize Gibbs free energy (14.20)

Solve for critical radius (14.21)

Number of molecules in a critical clusterDivide 4rc

3/3 by molecular volume [mq/(pA)] (14.22)

dΔGdrp

=8πrpσ p−4πrp2ρp

R*Tmq

lnSq =0

rc =2σpmq

ρpR*T lnSq

nc =32πσp

3mq2A

3ρp2 R*T lnSq( )

3

Page 30: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Critical Radius

Table 14.5

Critical radii and number of water molecules in a critical cluster when T = 288 K, p = 7.5 x 10-6 J cm-2, p = 1.0 g cm-3, and mq = 18 g mol-1

Saturation Critical Number of

Ratio Radius Molecules1 ∞ ∞1.01 0.11 2.03 x 108

1.02 0.055 2.58 x 107

1.10 0.011 2.32 x 105

1.5 0.0028 30102.0 0.0016 6035.0 0.0007 4810.0 0.00048 16

Page 31: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Homogen. Homomolecular NucleationRate (particles cm-3 s-1) (14.23)

Combine (14.18) and (14.20) (14.24)

Number of gas molecules striking cluster surface per second (14.25)

J hom=4πrc2βxZnNx exp

−ΔGhom*

kBT

⎝ ⎜

⎠ ⎟

ΔGhom* =

43

πrc2σp

βx =NxkBT

2πM x

Page 32: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Homogen. Homomolecular NucleationEquilibrium no. concentration of clusters of critical radius

Zeldovich non-equilibrium factor Accounts for the difference between an equilibrium and nonequilibrium cluster concentration (14.24)

Nx exp−ΔGhom* kBT( )

Zn =M x

2πrc2ρx

σpkBT

Page 33: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Homogeneous Binary Nucleation

Number of gas molecules striking cluster surface per second (14.11)

Rate (particles cm-3 s-1) (14.27)

Equilibrium no. concentration of cluster of critical radius

J hom=4πrc2βyNx exp

−ΔGhom*

kBT

⎝ ⎜

⎠ ⎟

βy =NykBT

2πM y

Nx +Ny( )exp−ΔGhom* kBT( )

Nx >>Ny Nx exp−ΔGhom* kBT( )–->

Page 34: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Heterogeneous Nucleation Rate

Fig. 14.4

Formation of critical embryo on a surface

Contact angle (c)= 0 --> surface wettable, embryo forms easily= 180o --> surface non-wettable, no embryo forms

Embryoc

Substrate

rc

Rh

Page 35: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Heterogeneous Nucleation Rate

Time a gas molecule spends on surface before bouncing off

(14.33)

Heterogeneous nucleation rate (no. embryos cm-2 s-1) (14.32)

Change in Gibbs free energy (14.30)

J het=4πrc2βyβxτexp

−ΔGhet*

kBT

⎝ ⎜

⎠ ⎟

τ=τ0expE

R*T

⎝ ⎜

⎠ ⎟

ΔGhet* =ΔGhom

* fh xh,mh( )

Page 36: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Correction Factor

Contact angle (14.29)

(14.31)

fh xh,mh( ) =1+1−mhxh

gh

⎝ ⎜

⎠ ⎟

3

+xh3 2−3

xh −mhgh

⎝ ⎜

⎠ ⎟ +

xh−mhgh

⎝ ⎜

⎠ ⎟

3⎡

⎢ ⎢

⎥ ⎥

+3mhxh2 xh−mh

gh−1

⎝ ⎜

⎠ ⎟

gh = 1+xh2 −2mhxh xh =Rh rc

mh =cosθc

θc =cos−1 σS,a −σS,wσw,a

⎝ ⎜

⎠ ⎟

Page 37: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Correction Factor

Fig. 14.5

Correction factor versus xh for different contact angles

0

0.5

1

1.5

2

2.5

0.1 1 10 100

f

h

x

h

= R

h

/ r

c

0

o

30

o

60

o

90

o

120

o

150

o

= 180

o

c

f h

Page 38: Presentation Slides for Chapter 14 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering

Parameterized NucleationParameterized homogeneous binary nucleation rate (14.33)

For sulfuric acid-water in remote marine boundary layer

Examplefr = 0.9mH2SO4 = 0.005 μg m-3

---> NH2SO4 = 3.1 x 107 molec cm-3

---> Jhom = 2.6 x 10-5 partic. cm-3 s-1

mH2SO4 = 0.05 μg m-3

---> NH2SO4 = 3.1 x 106 molec cm-3

---> Jhom = 3.1 x 105 partic. cm-3 s-1

J hom=107.0−64.24+4.7 fr( )+ 6.13+1.95fr( )log10NH2SO4