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Chapter 9 Soil Water

Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

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Page 1: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Chapter 9

Soil Water

Page 2: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Global Water BudgetVolumes in 103 km3 - Flows in 103 km3/yr

Page 3: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Soil Water is Limited

Page 4: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Residence Time

• The average length of time water spends in a reservoir: = V / Q

(tau) is the residence time, years

• V is the volume of the reservoir, km3

• Q is the flow through reservoir, km3/year

Page 5: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Think of a bathtub...

• If you start with an empty bathtub– V = how many gallons are in the tub– Q = how many gallons per minute are you

adding to the tub = V / Q = how many minutes it takes to fill

the bathtub

Page 6: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

• If you start with a full bath– There is no inflow

• And you let it drain at a constant rate

• Will it take the same time to drain?

– And you add and drain water at the same rate• Will a tracer take the same time?

Page 7: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

• Soil surfaces have negative charge! • Water is a polar molecule

– The H-side has a positive (+) charge

– The O-side has a negative (-) charge

• Water is bound to:– other water molecules by cohesive (water-water) forces

– the soil surface by adhesive (soil-water) forces

• Think of water as a bar magnet, soil is a negative box– it sticks to other water “magnets”

– the positive end sticks the “box”

Page 8: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Capillary Rise

• The wicking effect caused by small pores– h = 0.15 / r– h is the height of rise in tube, cm– r is the radius of tube, cm

• The height of rise is higher in:– clays than silts– silts than sands– sands than gravels

Page 9: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Total Energy

• The driving force for water flow

• The sum of three types of energy– E = GE + KE + PE– GE = gravitational or potential energy (like a water

balloon at the top of a building)– KE = kinetic or inertial energy (like when it's falling)– PE = pressure energy (like when it hits the ground)

Page 10: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Total Head

• Total Energy expressed as an equivalent depth of water:

– h = z + p– z is the elevation head– p is the pressure head

Page 11: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Soil Tension

• A negative pressure that accounts for moisture held in the soil by capillary forces– A small tension means water is not bound tightly– A large tension means that water is bound tightly

• We use the symbol (psi) to represent the tension: = - p– A negative pressure!!– Remember this: it’s negative...

Page 12: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr
Page 13: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Soils = Air + Water + Solids

Page 14: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr
Page 15: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr
Page 16: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Soil Tensiometer

Page 17: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Time Domain Reflectometer

Used to measure soil moisture

An electrical pulse is sent down the rod

The pulse bounces off the end and returns to the source

The wetter the soil, the longer the delay in returning

Page 18: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Some Definitions• Bulk Density:

– BD = Mass Soil / Volume Soil

• Porosity: – PS = Volume Voids / Volume Soil

– PS = 1 - BD / PD

• Water Content (theta): v = Volume Water / Volume Soil

g = Mass Water / Mass Soil

v = g · BD

Page 19: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

• Water Depth:– Dw = v Ds

– Ds is depth of soil

• Relative Saturation (capital theta): = Volume Water / Volume of pores = v / PS

Page 20: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Plant Water• Water is pumped through plants partly by the pull

or tension of the atmosphere• The tension in the atmosphere is generally

hundreds of bars• The moisture in the soil is only weakly bound.• We can measure the tension in the plant, and find

the tension is lowest in the roots, and highest in the leaf

Page 21: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr
Page 22: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Plant Stomates Control Water Loss

Page 23: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Cells collapse (or “wilt”) when their

internal fluid pressure drops

Page 24: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Classification of Soil Water

• Saturation, SAT:– The water content when the pores are

completely filled with water. – Saturation corresponds to pressure potentials of

zero, and above (positive pressure). – This is the same as saying p 0, 0

– At saturation, the volumetric water content equals the porosity.

Page 25: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Field Capacity, FC

• The water content held after rapid gravitational drainage has occurred.

• Field capacity is sometimes described as the amount of water a soil can hold against gravity.

• This is not completely true, however, as water continues to drain slowly by gravity at pressures below field capacity.

• The tensions associated with field capacity are between = 0.1 and 0.3 bars, equal to 100 to 300 cm.

Page 26: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr
Page 27: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Wilting Point, WP

• The amount of water held when plant roots can no longer extract water from the soil.

• This tension is usually assumed to be =15 bars (p = -15 bars)

• Different plants have different wilting points• Xeriphytes (dry-loving plant) can go down to =

75 bars (p = -75 bars)• Phreatophytes (water-loving plants) can only go

down to = 5 bars (p = - 5 bars)

Page 28: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Air Dry, AD

• The amount of water held by soil when it is exposed to the atmosphere.

• It is a function of the relative humidity. • Soils left in moist air are wetter than soils left in

dry air. – Soils in caves and greenhouses are moist

– Soils in the desert are dry

varies from 75 to over 1000 bars depending on the RH

Page 29: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Oven Dry, OD

• The amount of water held once the soil has been dried in a 105°C oven for 48 hours.

• Some scientists prefer to oven dry at 60°C in order to prevent clays from dehydrating.

is about 10,000 bars in the oven.

Page 30: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Plant Available Water, AW

• The water in the soil between field capacity, = 0.1 bar, and the wilting point, = 15 bars:– The water bound less tightly than the field capacity is

termed gravitational water because gravity easily drains this water before the plants can get it.

– Water bound beyond the wilting point is unavailable, because plant roots can not pull hard enough to overcome absorption of the water to the soil

– AW = FC - WP

Page 31: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Available Water

Page 32: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr
Page 33: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Moisture Characteristic Curve A plot of water content, , vs soil tension, .

Page 34: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr
Page 35: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Hysteresis: Caused by air blocking water in pores

Page 36: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Soil Water Movement

Page 37: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Soil Water Movement

• Total Head: – h = z + p = z -

• Hydraulic Gradient:– Change in energy with distance– G = h / x

• Hydraulic conductivity– a function of pores sizes and pore connectivity

Page 38: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Soil water can move from dry to wet

Page 39: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Subsurface Potentials

Page 40: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Darcy's Law

• Predict the flux (flow per unit area):– q = - K · G

• Total Flow:– Q = A q = - A (K G)

• Pore Velocity:– v = q /

Page 41: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Q = - A K G• A:

– The area of flow– The greater the area, the greater the flow.

• K: – The hydraulic conductivity or permeability– The higher the conductivity, the greater the flow.

• G: – The magnitude of the driving force– The steeper the water slope, the greater the flow

Page 42: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Fluid Flow through Soil

Page 43: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Typical Hydraulic Conductivities

• Gravel, Lava Flows, Caves – K = 10 cm/s

• Sands – K = 20 cm/hr

• Soils – K = 5 cm/day

• Clays – K = 0.9 cm/yr

Page 44: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr
Page 45: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Hydraulic Conductivity

• Solving for the hydraulic conductivity:– K = - Q / A G

• Unsaturated Conditions– q = - Ku G = - K Kr G

– Ku = K Kr = unsaturated hydraulic conductivity

– Kr = relative hydraulic conductivity

• The Unsaturated Hydraulic Conductivity is:– Less than the Saturated Conductivity!!

Page 46: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

The Hydraulic Conductivity get smaller as the water content gets lower (drier)

Page 47: Chapter 9 Soil Water. Global Water Budget Volumes in 10 3 km 3 - Flows in 10 3 km 3 /yr

Chapter 9 Quiz - Soil Water

1. What is the volumetric water content if the bulk density is 1.33 g/cm3 and the gravimetric water content is 0.25?

2. What is the depth of water in a foot of soil if the volumetric water content is 0.10?

3. Is available water primarily held in:a. Macropores (greater than 100 µm)

b. Mesopores (between 0.1 and 100 µm)

c. Micropores (smaller than 0.1 µm)

4. Identify a type of geologic material that has:a. High porosity, high permeability

b. Low porosity, low permeability

c. High porosity, low permeability

d. Low porosity, high permeability

5. [Adhesion / Cohesion] is the attraction of water to the soil surface.