Water in the atmosphere. Water content of air Mass mixing ratio, Saturated vapour pressure,...
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Transcript of Water in the atmosphere. Water content of air Mass mixing ratio, Saturated vapour pressure,...
Water in the atmosphere
Water content of air
Mass mixing ratio, airdry mass
vapour watermassx
%110~ 1gkg
Saturated vapour pressure, equilibrium over flat surface
Rate of evaporation = rate of condensation
svp is a function of T only
Saturated vapour pressure
Condensation
Condensation when R.H.≥100%
R.H. can increase by
(i) increasing x,
(ii) cooling air
%100T same at svp
pressure vapourR.H. Humidity, Relative
Cooling damp air
• Radiation loss• Ascent (of air mass) • Descent, through inversion
• Advection, over cool region
• Influx of cold dry air• Convection
radiation foghill fog/cloud, frontssteam fogadvection fog, harArctic sea smokecumulus clouds
Warm Rain Process
• Saturation• Nucleation• Growth by condensation• Growth by accretion• Rainfall
Nucleation
For typical molecule, r~0.6nm, would need RH=740% (SS=640%)
In atmosphere maximum SS observed is ~1%
Condensation must be on particles with r~100nm
91 2 1.2 10exp 1
w
svp r
svp r RT r
s.v.p. over curved surface > s.v.p. over flat surface
Radius Name Conc. (cm-3) SS
< 0.1 µm Aitken nuclei 10,000 1%
0.1 - 1 µm large nuclei 100 0.1%
> 1 µm giant nuclei 1 0.01%
Nucleation
Hygroscopic nuclei
Kohler curves
9
3
1.2 101
svp r Bm
svp r r
Fewer water molecules in surface so lower evaporation rate
Sizes of droplets
Growth by Condensation
rdr
To grow by dr require this much water
24w wdm dV r dr
2
1
4w
dr dm
dt r dt
Same flux through every shell, so integrate to find Δp
Mass flux of water vapour diffusing through shell of radius n
24dm dp
F n Ddt dn
2
1
4 4
rr F dn F
p dpD n D r
24w w
dr F Dp
dt r r
1
w
dr D svp SS
dt r
Vapour pressure at droplet = svp (T)Vapour pressure in cloud = svp * RH
1
cloud drop surfacep p p
svp RH svp SS
Growth by condensation
Terminal velocity of
drops
6mg rv
22
9wgv r
343
6 6wr gmg
vr r
For laminar flow, at terminal velocitydrag force=weight
Growth by Collision/AccretionContinuous collection model
v1
v2
r1
r2
2{r1+r2}
2
1 2 1 2 l
dmr Ev
dtwr v
relative volume swept out per unit time
collection efficiency
liquid water content of cloud
22 11 1 2 1 24w s air
drr r r v v x Edt
1 2 1 2
11
if and
4s air
w
r r v v
x Edrv
dt
11
drr
dt
For large drops (>40µm) 1 1v r
Arial view of convection cells
Cloud streets