prof. fred remer university of north dakota water in the atmosphere

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Prof. Fred RemerUniversity of North Dakota

Water in the AtmosphereWater in the Atmosphere

Prof. Fred RemerUniversity of North Dakota

ReadingReading

Hess– pp 43 - 44– pp 58 – 60

Tsonis– pp 93 – 97

Wallace & Hobbs– pp 66 – 67– pp 79 – 84

Bohren & Albrecht– pp 181-188

Prof. Fred RemerUniversity of North Dakota

ObjectivesObjectives

Be able to define water vapor pressure

Be able to define virtual temperature Be able to define specific humidity Be able to define mixing ratio

Prof. Fred RemerUniversity of North Dakota

ObjectivesObjectives

Be able to calculate the water vapor pressure

Be able to calculate virtual temperature

Be able to calculate specific humidity Be able to calculate mixing ratio

Prof. Fred RemerUniversity of North Dakota

Water In the AtmosphereWater In the Atmosphere

Unique Substance Occurs in Three Phases Under

Normal Atmospheric Pressures and Temperatures

Gaseous State– Variable 0 – 4%

HH HHOO

Prof. Fred RemerUniversity of North Dakota

Water in the AtmosphereWater in the Atmosphere

Remember Dalton’s Law?– Law of Partial Pressures

– Let’s look at the contribution of water

p = p1 + p2 + p3 + ….p = p1 + p2 + p3 + ….

Prof. Fred RemerUniversity of North Dakota

Water Vapor Pressure (e)Water Vapor Pressure (e)

Ideal Gas Law for Dry Air

Ideal Gas Law for Water Vapor

TRp dd

TRe vv

p = pressure of dry airp = pressure of dry airdd = specific volume of dry air = specific volume of dry air

RRdd = gas constant for dry air = gas constant for dry air

e = vapor pressure of water vapore = vapor pressure of water vaporvv = specific volume of water vapor = specific volume of water vapor

RRvv = gas constant for water vapor = gas constant for water vapor

Prof. Fred RemerUniversity of North Dakota

Water Vapor Pressure (e)Water Vapor Pressure (e)

Partial pressure that water vapor exerts

Total PressureTotal Pressurep = pp = pOO22

+p+pNN22+p+pHH22OOvv

Water Vapor PressureWater Vapor Pressuree = pe = pHH22OOvv

Prof. Fred RemerUniversity of North Dakota

Water Vapor Pressure (e)Water Vapor Pressure (e)

Gas Constant of Water Vapor

HH HHOO

Wv M

RR

Molecular Weight Molecular Weight (M(Mw w ))

Hydrogen = 1kg kmolHydrogen = 1kg kmol-1 -1

Oxygen = 16 kg kmolOxygen = 16 kg kmol-1-1

Water = 18 kg kmolWater = 18 kg kmol-1-1

1

11

v kmolkg18

kmolKJ8314R

11v kgKJ461R

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

The temperature dry air must have in order to have the same density as moist air at the same pressure

Fictitious temperature

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Dry Air

Total Pressure = pTotal Pressure = p

Volume = VVolume = V

Temperature = TTemperature = T

Mass of Air = mMass of Air = mdd

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Moist Air (Mixture)

Total Pressure = pTotal Pressure = p

Volume = VVolume = V

Temperature = TTemperature = T

Mass of Air = mMass of Air = md d ++ mmvv

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Density of mixture

V

mm vd

vd

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Ideal Gas Law

– For Dry Air

– For Water Vapor Alone

TRp ddd

TRe vv

ororTR

p

d

dd

TR

e

vv oror

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Substitute into density expression

vd

TR

p

d

dd

TR

e

vv

TR

e

TR

p

vd

d

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Dalton’s Law of Partial Pressure

TR

e

TR

p

vd

d

epp d oror eppd

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Substitute eppd

TR

e

TR

p

vd

d TR

e

TR

ep

vd

oror

vd R

e

R

ep

T

1

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Remove Rd

vd R

e

R

)ep(

T

1

v

d

d R

Re)ep(

TR

1

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Define 622.

M

M

R

R

d

w

v

d

eepTR

1

d

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Remove p

eepTR

1

d

p

e

p

e1

TR

p

d

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Rearrange terms

p

e

p

e1

TR

p

d

)1(

p

e1

TR

p

d

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

By definition, virtual temperature is the temperature dry air must have in order to have the same density as moist air (mixture) at the same pressure

vdTRp

TRp ddd TRe vvInstead ofInstead of oror

UseUsep = total (mixture) pressurep = total (mixture) pressure

= mixture density= mixture density

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Substitution of

)1(

p

e1

TR

p

d

vdTRp Into

)1(

p

e1

TR

pRTp

ddv

Produces

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Rearrange

)1(

p

e1

TR

pRTp

ddv

)1(pe

1TRp

R

pT

dd

v

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Start Canceling!

)1(pe

1TRp

R

pT

dd

v

)1(

pe

1

TTv

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Still looks Ugly! Simplify!

)1(

pe

1

TTv

)622.1)(p/e(1

TTv

622.

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

)p/e378(.1

TTv

p = total (atmospheric) pressurep = total (atmospheric) pressure

e = water vapor pressuree = water vapor pressure

T = temperatureT = temperature

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Moist air (mixture) is less dense than dry air

Virtual temperature is greater than actual temperature

Small difference

)p/e378(.1

TTv

Prof. Fred RemerUniversity of North Dakota

Specific Humidity (q)Specific Humidity (q)

Ratio of the density of water vapor in the air to the (total) density of the air

vq

Prof. Fred RemerUniversity of North Dakota

Mixing Ratio (w)Mixing Ratio (w)

The mass of water vapor (mv) to the mass of dry air

Mass of Dry Air = mMass of Dry Air = mdd

Mass of Water Vapor = mMass of Water Vapor = mvv

Prof. Fred RemerUniversity of North Dakota

Mixing Ratio (w)Mixing Ratio (w)

The mass of water vapor (mv) to the mass of dry air

Mass of Dry Air = mMass of Dry Air = mdd

Mass of Water Vapor = mMass of Water Vapor = mvv

d

v

m

mw

Prof. Fred RemerUniversity of North Dakota

Mixing Ratio (w)Mixing Ratio (w)

Expressed in g/kg– Dry Air

1 to 2 g/kg

– Tropical Air 20 g/kg

d

v

m

mw

Prof. Fred RemerUniversity of North Dakota

Mixing Ratio (w)Mixing Ratio (w)

Can mixing ratio be expressed in terms of water vapor pressure?

Sure as it will rain on a meteorologist’s picnic!

d

v

m

mw

Prof. Fred RemerUniversity of North Dakota

Mixing Ratio (w)Mixing Ratio (w)

By definition

Divide top and bottom by volume (V)

d

v

m

mw

V/m

V/mw

d

v

Prof. Fred RemerUniversity of North Dakota

Mixing Ratio (w)Mixing Ratio (w)

But density is so.....

V/m

V/mw

d

v

V/m

d

vw

w = mixing ratiow = mixing ratio

vv = density of water vapor in air = density of water vapor in air

dd = density of dry air = density of dry air

Prof. Fred RemerUniversity of North Dakota

Mixing Ratio (w)Mixing Ratio (w)

Ideal Gas Law

d

vw

TRp ddd

TRe vv

TR

p

d

dd

TR

e

vv

oror

oror

Prof. Fred RemerUniversity of North Dakota

Mixing Ratio (w)Mixing Ratio (w)

Substitute

d

vw

TR

p

d

dd

TR

e

vv

TR

p/

TR

ew

d

d

v

Prof. Fred RemerUniversity of North Dakota

Mixing Ratio (w)Mixing Ratio (w)

Simplify

Remember

TR

p/

TR

ew

d

d

v

dv

d

p

e

R

Rw

622.M

M

R

R

d

w

v

d

Prof. Fred RemerUniversity of North Dakota

Mixing Ratio (w)Mixing Ratio (w)

Substitute into

But

v

d

R

R

dv

d

p

e

R

Rw

dp

ew

eppd p = total pressure of air (mixture)p = total pressure of air (mixture)

Prof. Fred RemerUniversity of North Dakota

Mixing Ratio (w)Mixing Ratio (w)

Substitute into

Ta-Da!

dp

ew eppd

ep

ew

Prof. Fred RemerUniversity of North Dakota

Mixing Ratio (w)Mixing Ratio (w)

Expression for Mixing Ratio (w)– Water Vapor Pressure (e) in any units– Atmospheric Pressure (p) in any units

ep

e622.w

Prof. Fred RemerUniversity of North Dakota

Mixing Ratio (w)Mixing Ratio (w)

Can be used to determine other water variables

Let’s look at– Specific Humidity – Water Vapor Pressure (e)

– Virtual Temperature (Tv)

Prof. Fred RemerUniversity of North Dakota

Specific Humidity (q)Specific Humidity (q)

By definition

But

vqq = specific humidityq = specific humidity

vv = density of water vapor in air = density of water vapor in air

= density of air = density of air

dv dd = density of dry air = density of dry air

Prof. Fred RemerUniversity of North Dakota

Specific Humidity (q)Specific Humidity (q)

Substitute into

Results in

But

vqdv

dv

vq

V

m

Prof. Fred RemerUniversity of North Dakota

Specific Humidity (q)Specific Humidity (q)

Substitute into

Results in

dv

vq

V

m

V/mV/m

V/mq

dv

v

Prof. Fred RemerUniversity of North Dakota

Specific Humidity (q)Specific Humidity (q)

Eliminate V

dv

v

mm

mq

V/mV/m

V/mq

dv

v

Prof. Fred RemerUniversity of North Dakota

Specific Humidity (q)Specific Humidity (q)

Divide top and bottom by md

dv

v

mm

mq

dddv

dv

m/mm/m

m/mq

Prof. Fred RemerUniversity of North Dakota

Specific Humidity (q)Specific Humidity (q)

But so

dddv

dv

m/mm/m

m/mq

d

v

m

mw

1w

wq

Prof. Fred RemerUniversity of North Dakota

Specific Humidity (q)Specific Humidity (q)

Expression for specific humidity (q)– Mixing Ratio (w) in kg kg-1

1w

wq

Prof. Fred RemerUniversity of North Dakota

Water Vapor Pressure (e)Water Vapor Pressure (e)

Pressure exerted by water vapor is a fraction of total pressure of air

Fraction is proportional to # of moles in mixture

pfe e = water vapor pressuree = water vapor pressure

f = fractional amount of water vapor f = fractional amount of water vapor

p = total pressure of airp = total pressure of air

Prof. Fred RemerUniversity of North Dakota

Water Vapor Pressure (e)Water Vapor Pressure (e)

How many moles of water are in a sample of air?

Number of moles of water

w

vv M

mn

nnvv = # of moles = # of moles

mmvv = mass of water molecules = mass of water molecules

MMww = molecular weight of water = molecular weight of water

Prof. Fred RemerUniversity of North Dakota

Water Vapor Pressure (e)Water Vapor Pressure (e)

How many moles of dry air are in a sample of air?

Number of moles of dry air

d

dd M

mn

nndd = # of moles = # of moles

mmdd = mass of dry air = mass of dry air

MMdd = mean molecular weight of dry air = mean molecular weight of dry air

Prof. Fred RemerUniversity of North Dakota

Water Vapor Pressure (e)Water Vapor Pressure (e)

How many moles of air are in a sample of air?

Number of moles of air

d

d

w

v

M

m

M

mn

Prof. Fred RemerUniversity of North Dakota

Water Vapor Pressure (e)Water Vapor Pressure (e)

What is the molar fraction of water vapor in the air?

Substitute into

ddwv

wv

M/mM/m

M/mf

pfe

Prof. Fred RemerUniversity of North Dakota

Water Vapor Pressure (e)Water Vapor Pressure (e)

Yikes! Let’s make this more manageable!

ddwv

wv

M/mM/m

M/mf

pfe

pM/mM/m

M/me

ddwv

wv

Prof. Fred RemerUniversity of North Dakota

pM/mM/m

M/me

ddwv

wv

Water Vapor Pressure (e)Water Vapor Pressure (e)

Multiply top and bottowm by Mw/md

pm/M

m/M

M/mM/m

M/me

dw

dw

ddwv

wv

Prof. Fred RemerUniversity of North Dakota

Water Vapor Pressure (e)Water Vapor Pressure (e)

Canceling out

pm/M

m/M

M/mM/m

M/me

dw

dw

ddwv

wv

pM/Mm/m

m/me

dwdv

dv

Prof. Fred RemerUniversity of North Dakota

Water Vapor Pressure (e)Water Vapor Pressure (e)

But

pM/Mm/m

m/me

dwdv

dv

d

v

m

mw

Mixing RatioMixing Ratio

andand 622.M

M

R

R

d

w

v

d

Prof. Fred RemerUniversity of North Dakota

Water Vapor Pressure (e)Water Vapor Pressure (e)

pM/Mm/m

m/me

dwdv

dv

d

v

m

mw

d

w

M

M

pw

we

Prof. Fred RemerUniversity of North Dakota

pw

we

Water Vapor Pressure (e)Water Vapor Pressure (e)

Expression for water vapor pressure (e)– Mixing Ratio (w) in kg kg-1

– Atmospheric Pressure (p)

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Derive an expression for virtual temperature (Tv) using mixing ratio (w)

)1(

pe

1

TTv

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Expression for water vapor pressure

pw

we

)1(

pe

1

TTv

oror

w

w

p

e

Prof. Fred RemerUniversity of North Dakota

)1(

pe

1

TTv

w

w

p

e

Virtual Temperature (TVirtual Temperature (Tvv))

Substituting

)1(

ww

1

TTv

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Expand

)1(

ww

1

TTv

ww

ww

1

TTv

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Common denominator w+

ww

ww

1

TTv

ww

ww

ww

TTv

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Group

ww

ww

ww

TTv

wwww

TTv

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Simplify

wwww

TTv

ww

TTv

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Divide numerator by denominator (polynomial division) and eliminate w2 terms

)w1(

wTTv

w1

1TTv

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (TVirtual Temperature (Tvv))

Substitute = .622

w1

1TTv

w61.1TTv

Prof. Fred RemerUniversity of North Dakota

Virtual Temperature (Tv)Virtual Temperature (Tv)

Expression for virtual temperature– Mixing Ratio (w) in kg kg-1

w61.1TTv

Prof. Fred RemerUniversity of North Dakota

Review of Water VariablesReview of Water Variables

Water Vapor Pressure

TRe vv

pw

we

Prof. Fred RemerUniversity of North Dakota

Review of Water VariablesReview of Water Variables

Virtual Temperature

w61.1TTv

)p/e378(.1

TTv

Prof. Fred RemerUniversity of North Dakota

Review of Water VariablesReview of Water Variables

Mixing Ratio

d

v

m

mw

ep

e622.w

d

vw

Prof. Fred RemerUniversity of North Dakota

Review of Water VariablesReview of Water Variables

Specific Humidity

vq1w

wq

Prof. Fred RemerUniversity of North Dakota

Water in the AtmosphereWater in the Atmosphere

Moisture Variables– Water Vapor Pressure– Virtual Temperature– Mixing Ratio– Specific Humidity

Amount of Moisture in the Atmosphere

Prof. Fred RemerUniversity of North Dakota

Water in the AtmosphereWater in the Atmosphere

Unanswered Questions– How much water vapor can the air hold?– When will condensation form?– Is the air saturated?

The Beer Analogy

Prof. Fred RemerUniversity of North Dakota

The Beer AnalogyThe Beer Analogy

You are thirsty! You would like a

beer. Obey your thirst!

Prof. Fred RemerUniversity of North Dakota

The Beer AnalogyThe Beer Analogy

Pour a glass but watch the foam

Prof. Fred RemerUniversity of North Dakota

The Beer AnalogyThe Beer Analogy

Wait! Some joker put

a hole in the bottom of your Styrofoam cup!

It is leaking!

Prof. Fred RemerUniversity of North Dakota

The Beer AnalogyThe Beer Analogy

Having had many beers already, you are intrigued by the phenomena!

Prof. Fred RemerUniversity of North Dakota

The Beer AnalogyThe Beer Analogy

Rate at beer flows from keg is constant

Prof. Fred RemerUniversity of North Dakota

The Beer AnalogyThe Beer Analogy

Rate at beer flows from keg is constant

Rate at beer flows from cup depends on height

Prof. Fred RemerUniversity of North Dakota

The Beer AnalogyThe Beer Analogy

The higher the level of beer in the cup, the faster it leaks!

Prof. Fred RemerUniversity of North Dakota

The Beer AnalogyThe Beer Analogy

The cup fills up Height

becomes constant

Equilibrium Reached

Inflow(Constant)

Leakage(Varies with

Height)

Prof. Fred RemerUniversity of North Dakota

The Beer AnalogyThe Beer Analogy

What do you do?

Inflow(Constant)

Leakage(Varies with

Height)

Prof. Fred RemerUniversity of North Dakota

The Beer AnalogyThe Beer Analogy

Get a new cup!

Prof. Fred RemerUniversity of North Dakota

OverviewOverview

Similar to what happens to water in the atmosphere

Prof. Fred RemerUniversity of North Dakota

OverviewOverview

Molecules in liquid water attract each other

In motion

Prof. Fred RemerUniversity of North Dakota

OverviewOverview

Collisions Molecules near

surface gain velocity by collisions

Prof. Fred RemerUniversity of North Dakota

OverviewOverview

Fast moving molecules leave the surface

Evaporation

Prof. Fred RemerUniversity of North Dakota

OverviewOverview

Soon, there are many water molecules in the air

Prof. Fred RemerUniversity of North Dakota

OverviewOverview

Slower molecules return to water surface

Condensation

Prof. Fred RemerUniversity of North Dakota

OverviewOverview

Net Evaporation– Number leaving

water surface is greater than the number returning

– Evaporation greater than condensation

Prof. Fred RemerUniversity of North Dakota

OverviewOverview

Molecules leave the water surface at a constant rate

Depends on temperature of liquid

Prof. Fred RemerUniversity of North Dakota

OverviewOverview

Molecules return to the surface at a variable rate

Depends on mass of water molecules in air

Prof. Fred RemerUniversity of North Dakota

OverviewOverview

Rate at which molecule return increases with time– Evaporation

continues to pump moisture into air

– Water vapor increases with time

Prof. Fred RemerUniversity of North Dakota

OverviewOverview

Eventually, equal rates of condensation and evaporation

“Air is saturated” Equilibrium

Prof. Fred RemerUniversity of North Dakota

OverviewOverview

Derive a relationship that describes this equilibrium

Prof. Fred RemerUniversity of North Dakota

Clausius-Clapeyron Clausius-Clapeyron EquationEquation

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