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Soil Physics 2010 Outline Announcements More on thermal properties More on evaporation.

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Soil Physics 2010 Measuring Thermal Properties in the Field Inverse methods using many measurements at multiple depths and times? Thermal Diffusivity  DTDT Volumetric Heat Capacity  cc Thermal Conductivity  
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il Physics 2010 Outline Announcements More on thermal properties More on evaporation
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Page 1: Soil Physics 2010 Outline Announcements More on thermal properties More on evaporation.

Soil Physics 2010

Outline

• Announcements• More on thermal properties• More on evaporation

Page 2: Soil Physics 2010 Outline Announcements More on thermal properties More on evaporation.

Soil Physics 2010

Announcements• Review session today, 11:00-1:00,

room 1581 Agronomy

• More sessions will be scheduled for next week

• 1 more homework will be assigned

• Quiz? No, not today.

Page 3: Soil Physics 2010 Outline Announcements More on thermal properties More on evaporation.

Soil Physics 2010

Measuring Thermal Properties in the Field

Inverse methods using many measurements at multiple depths and times?

ThermalDiffusivity

DT

VolumetricHeat Capacity

c

ThermalConductivity

Page 4: Soil Physics 2010 Outline Announcements More on thermal properties More on evaporation.

Soil Physics 2010

Assumptions:DT constantNo water movementNo latent heat movementSine wave

…not necessarily!

Measuring Thermal Diffusivity in the Field

Page 5: Soil Physics 2010 Outline Announcements More on thermal properties More on evaporation.

Soil Physics 2010

Measuring Thermal Diffusivity in the Field

The amplitude method:

2

2

1

221

ln2

AA

zzDT

The phase change method: 2

21

221

2

zzDT

Every sensor is a temperature sensor. But if you’re clever, you can use it to measure something else as well.

-- Gaylon Campbell

?

Page 6: Soil Physics 2010 Outline Announcements More on thermal properties More on evaporation.

Soil Physics 2010

Suppose we measure T and :We get DT from amplitude or phase shiftWe get directlyFrom DT and we calculate cFrom DT and c we calculate …?

Estimating other properties in the field

Page 7: Soil Physics 2010 Outline Announcements More on thermal properties More on evaporation.

Soil Physics 2010

Evaporation

Page 8: Soil Physics 2010 Outline Announcements More on thermal properties More on evaporation.

Soil Physics 2010

Evaporation Lawrence et al., 2007

Evaporation from the soil can be an important part of the total water budget!

Page 9: Soil Physics 2010 Outline Announcements More on thermal properties More on evaporation.

Soil Physics 2010

Evaporation

Evaporation may be limited by:• Energy• Water supply• Vapor transport

time

e, m

m/d

ay Stage I

Stage II

Stage III

Page 10: Soil Physics 2010 Outline Announcements More on thermal properties More on evaporation.

Soil Physics 2010

Evaporation

Evaporation may be limited by:• Energy in• Water in• Vapor out

time

e, m

m/d

ay Stage I

Stage II

Stage III

Water available;(mostly) energy-limited

Energy available;Transport limiting:

water upvapor out

Page 11: Soil Physics 2010 Outline Announcements More on thermal properties More on evaporation.

Soil Physics 2010

Main limitations on actual evaporation from soil• Stage I: evaporation from the surface

• Energy available at surface• Vapor pressure deficit in air near the surface• Transport of vapor away from the surface

• Stage II: evaporation from a retreating drying front• Flow of liquid water to the drying front

• Stage III: evaporation from a stationary drying front• Diffusion of water vapor from the drying front to air above

the soil surface

time

e, m

m/d

ay Stage I

Stage II

Stage III

Page 12: Soil Physics 2010 Outline Announcements More on thermal properties More on evaporation.

Soil Physics 2010

Evaporation insights and innovations 1:Maria Dragila: Enhanced evaporation from fractures

Daytime:Hot dry soil surfaceCooler, moister fracture faceEvaporation limited by diffusion

Nighttime:Cool dry soil surfaceWarmer, moister fracture faceConvection in the fracture

enhances evaporation


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