lecture 7 - 1 ers 482/682 (fall 2002) infiltration ers 482/682 small watershed hydrology

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ERS 482/682 (Fall 2002) Lecture 7 - 1 Infiltration ERS 482/682 Small Watershed Hydrology

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ERS 482/682 (Fall 2002) Lecture 7 - 1

Infiltration

ERS 482/682Small Watershed Hydrology

ERS 482/682 (Fall 2002) Lecture 7 - 2

Definitions

• infiltration:– process by which water enters the soil surface

• infiltration rate, f(t):– rate at which water enters the soil surface

• water-input rate, w(t):– rate at which water arrives at the soil surface

• infiltration capacity, f*(t):– maximum rate at which infiltration can occur

• depth of ponding, H(t):– depth of water standing on the surface

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ERS 482/682 (Fall 2002) Lecture 7 - 3

Definitions• percolation

– downward movement of water through the soil

• hydraulic conductivity, Kh:– rate at which water moves through a porous medium under a

unit potential-energy gradient

• sorptivity, Sp:– rate at which water will be drawn into an unsaturated soil in the

absence of gravity forces

• soil-water pressure or matric potential, :– water pressure (tension) head in a soil

• air-entry tension, ae:– pressure head when significant volumes of air begin to appear

in soil pores; occurs at the capillary fringe (i.e., height of the tension-saturated zone)

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ERS 482/682 (Fall 2002) Lecture 7 - 4

Why is infiltration important?

ERS 482/682 (Fall 2002) Lecture 7 - 5

Why is infiltration important?

• Determines availability of water for overland flow– Flood prediction

ERS 482/682 (Fall 2002) Lecture 7 - 6

Why is infiltration important?

• Determines availability of water for overland flow– Flood prediction– Irrigation plans

ERS 482/682 (Fall 2002) Lecture 7 - 7

Why is infiltration important?

• Determines availability of water for overland flow– Flood prediction– Irrigation plans– Runoff pollution

• Determines how much water goes into the soil– Groundwater estimates– Water availability for plants

ERS 482/682 (Fall 2002) Lecture 7 - 8

Infiltration conditions

• No ponding:

Soil column

0tH

tw

twtf tf *

ERS 482/682 (Fall 2002) Lecture 7 - 9

Infiltration conditions

• No ponding:

Soil column

0tH

tw

twtf tf *

• Saturation from above: 0tH

tftf * tw

ERS 482/682 (Fall 2002) Lecture 7 - 10

Infiltration conditions

• No ponding:

Soil column

0tH

tw

twtf tf *

• Saturation from above: 0tH

tftf * tw

• Saturation from below: 0tH

0tf

ERS 482/682 (Fall 2002) Lecture 7 - 11

Figure 5.2: Manning (1987)

• Capillarity:– Sorptivity– Matric potential

• Gravity:– Percolation– Hydraulic conductivity

ERS 482/682 (Fall 2002) Lecture 7 - 12

What are models?

Models are representations of the real world

A model is a conceptualizationconceptualization of a system

that retains the essential essential characteristicscharacteristics of

that system for a specific purposespecific purpose.

ERS 482/682 (Fall 2002) Lecture 7 - 13

Assumptions for most infiltration models

• Water moves vertically• Homogeneous soil• Soil volume > pore size• Moving water is liquid only• Water movement not affected by

– Airflow in soil pores– Temperature– Osmotic gradients

ERS 482/682 (Fall 2002) Lecture 7 - 14

Infiltration models

• Horton• Kostiakov• Green-Ampt• Philip• Others

ERS 482/682 (Fall 2002) Lecture 7 - 15

Time, t

Infilt

rati

on r

ate

, f(

t)What we want to quantify…

tsat

w

ERS 482/682 (Fall 2002) Lecture 7 - 16

Time, t

Infilt

rati

on r

ate

, f(

t)What we want to quantify…

K*h

tsat

w

ERS 482/682 (Fall 2002) Lecture 7 - 17

Time, t

Infilt

rati

on r

ate

, f(

t)What we want to quantify…

K*h

tsat,1 tsat,2tsat,3

Runoff

f(t)<f*(t) f(t)=f*(t)

ERS 482/682 (Fall 2002) Lecture 7 - 18

What we want to quantify…

Figure 4.2: Brooks et al. (1991)

ERS 482/682 (Fall 2002) Lecture 7 - 19

Horton model

• Infiltration rate resembles a decreasingdecreasing exponential function:

Exponential function: xexf

where e = 2.71828…

xx

edx

ed

x

f(x)=

ex

ERS 482/682 (Fall 2002) Lecture 7 - 20

Horton model

Time, t

Infilt

rati

on

rate

, f(

t)

ffcc

ff00

f(t) = fc + (f0 – fc)e-ktx

x

x

x

x

xx

x

ERS 482/682 (Fall 2002) Lecture 7 - 21

Kostiakov model

Time , t

Infilt

rati

on

rate

, f(

t) f(t) = Kkt-

ERS 482/682 (Fall 2002) Lecture 7 - 22

Water

Soil column

Dry soil = 0

Wet soil =

Green-Ampt model

• Based on– Darcy’s law (Eq. 6-8b)

dz

pzdKq w

hz

tz

tztHKtf

f

ffh

*

Capillary suctionat wetting front

wetting wetting frontfront

zf(t)

H(t)

ERS 482/682 (Fall 2002) Lecture 7 - 23

Green-Ampt model

Figure 8.10: Hornberger et al.(1998)

zf(t)

ERS 482/682 (Fall 2002) Lecture 7 - 24

• Initially (before rain) = 0, H(t) = 0, f = 0

Green-Ampt model

Soil column

Dry soil = 0

tz

tztHKtf

f

ffh

*

0hKtf

ERS 482/682 (Fall 2002) Lecture 7 - 25

Green-Ampt model

• If w < K*h:H(t) = 0

Soil column

Dry soil = 0

wtf

Kh()

w = rainfall rate

Storage

until t = tw

> 0

time when rain stopstime when rain stops

ERS 482/682 (Fall 2002) Lecture 7 - 26

Green-Ampt model

• If w > K*h:H(t) = 0

Soil column

Dry soil = 0

wtf

Kh() up to up to K*K*hh

Storage

until t=tp

=

time when ponding startstime when ponding starts

ERS 482/682 (Fall 2002) Lecture 7 - 27

Green-Ampt model

• If w > K*h:

Soil column

Dry soil = 0

for t>tp =

tz

tztHKtf

f

ffh

*

tz

tHKtf

f

fh

1*

Equation 6-40 (error in book)

ERS 482/682 (Fall 2002) Lecture 7 - 28

Green-Ampt model

• If w > K*h:

Soil column

Dry soil = 0

for t>tp =

0 tztF f

tFKtf f

h0* 1

Equation 6-42

•Volume infiltrated

zf(t)Change inChange in

water contentwater content

•H(t) ~ 0

•rate

ERS 482/682 (Fall 2002) Lecture 7 - 29

Green-Ampt model

• Difficulties with model– Need to know

• Porosity, • Initial water content, 0

• K*h

f

• See Examples 6-6 and 6-7

measuremeasureTable 6-1Table 6-1

Table 6-1Table 6-1

Equation 6-46 with Table Equation 6-46 with Table 6-16-1

ERS 482/682 (Fall 2002) Lecture 7 - 30

Philip model

• For t>tp

Soil column

Dry soil = 0

=

tKtStF pp 21

•Volume infiltrated

pp Kt

Stf

21

2

where t = time since ponding began Sp = sorptivity Kp = hydraulic conductivity

ERS 482/682 (Fall 2002) Lecture 7 - 31

Philip model

• Works after ponding only• Used for characterizing

spatial variability of infiltrometer measurements

Soil column

Dry soil = 0

=

ERS 482/682 (Fall 2002) Lecture 7 - 32

Other models

• Richard’s equation– Physically-based– Numerically intensive

• Morel-Seytoux and Khanji model– Includes viscous resistance

• Smith-Parlange model– Account for different rates of changing

hydraulic conductivity with water content

ERS 482/682 (Fall 2002) Lecture 7 - 33

Measuring infiltration

• Flooding (ring) infiltrometers– Single ring– Double ring

• Rainfall-runoff plot infiltrometers

ERS 482/682 (Fall 2002) Lecture 7 - 34

Ring infiltrometersBouwer (1986)

Cylinder infiltrationCylinder infiltration

True infiltrationTrue infiltration

Water-entry pressure head Water-entry pressure head 0.5 0.5aeae

ERS 482/682 (Fall 2002) Lecture 7 - 35

Estimating infiltration parametersBox 6-2 and Example 6-9

Time, t(hr)

f(t)(cm hr-

1)

0.4850.640.790.941.091.241.391.551.701.842.00

5.004.384.053.833.673.553.463.383.313.263.21

ponding begins; determined in Example 6-7ponding begins; determined in Example 6-7

Data from Example 6-8

ERS 482/682 (Fall 2002) Lecture 7 - 36

Estimating infiltration parametersBox 6-2 and Example 6-9

Time, t(hr)

t’(hr)

f(t)(cm hr-

1)

0.4850.640.790.941.091.241.391.551.701.842.00

0.000.1550.3050.4550.6050.7550.9051.0651.2151.3651.515

5.004.384.053.833.673.553.463.383.313.263.21

ERS 482/682 (Fall 2002) Lecture 7 - 37

Estimating infiltration parametersBox 6-2 and Example 6-9

Time, t(hr)

t’(hr)

f(t)(cm hr-

1)

0.4850.640.790.941.091.241.391.551.701.842.00

0.000.1550.3050.4550.6050.7550.9051.0651.2151.3651.515

5.004.384.053.833.673.553.463.383.313.263.21

Least squares approach:Find the parameters that

provide the ‘best fit’ of the model to the observed data

‘best fit’ occurs when sum of the squared differences

between measured and modeled values is

minimized

ERS 482/682 (Fall 2002) Lecture 7 - 38

Estimating infiltration parametersBox 6-2 and Example 6-9

Time, t(hr)

t’(hr)

f(t)(cm hr-

1)

0.4850.640.790.941.091.241.391.551.701.842.00

0.000.1550.3050.4550.6050.7550.9051.0651.2151.3651.515

5.004.384.053.833.673.553.463.383.313.263.21

2

21

2121

11

122

ii

ii

i

i

p

ttN

ttf

ttf

N

S

N

tStf

K ipi

p 2

12 21

Equations 6B2-8 and 6B2-9

note errorin book!

ERS 482/682 (Fall 2002) Lecture 7 - 39

Estimating infiltration parametersBox 6-2 and Example 6-9

Time, t(hr)

t’(hr)

f(t)(cm hr-

1)

0.4850.640.790.941.091.241.391.551.701.842.00

0.000.1550.3050.4550.6050.7550.9051.0651.2151.3651.515

5.004.384.053.833.673.553.463.383.313.263.21

21

i

i

t

tf

21

1

it it1

sumsum sumsum sumsum sumsum

ERS 482/682 (Fall 2002) Lecture 7 - 40

Variability of infiltration

• Factors that affect infiltration rate– Water-input rate or depth of ponding– Hydraulic conductivity at the surface

• Organic surface layers• Frost• Swelling-drying• Inwashing of fine sediment• Anthropogenic modification

ERS 482/682 (Fall 2002) Lecture 7 - 41

Variability of infiltration

• Factors that affect infiltration rate– Water-input rate or depth of ponding– Hydraulic conductivity at the surface

• Organic surface layers• Frost• Swelling-drying• Inwashing of fine sediment• Anthropogenic modification

ERS 482/682 (Fall 2002) Lecture 7 - 42

Variability of infiltration

• Factors that affect infiltration rate– Water content of surface pores– Surface slope and roughness– Chemical characteristics of soil

• hydrophobicity

– Physical/chemical properties of water

Figure 4.5: Brooks et al. (1991)

ERS 482/682 (Fall 2002) Lecture 7 - 43

Point watershed???

• Manley (1977) approach

0 1.0

0.5

Fraction of watershed area

Infilt

rati

on

cap

aci

ty

K*K*++hh

ww

Rain

fall

rate

InfiltrationInfiltration

*

2

2 hK

wq

ERS 482/682 (Fall 2002) Lecture 7 - 44

Point watershed???

• Areal-weighted averages

pp Kt

Stf 21

2Philip equation:

•Measure at several locations•Calculate area-weighted average of Sp and Kp

pp KEt

SEtfE 21

2

Areal-weighted average of infiltrationAreal-weighted average of infiltration

ERS 482/682 (Fall 2002) Lecture 7 - 45

Point watershed???

• Divide watershed into subareas– Soil properties– Initial conditions– Etc.

pp KEt

SEtfE 21

2

• Calculate areally-weighted infiltration

ERS 482/682 (Fall 2002) Lecture 7 - 46

Example: Incline Creek Watershed

• Objective: determine which data collection techniques are best for quantifying spatial variations in surface infiltration– Used Philip equation

Sullivan et al. 1996

ERS 482/682 (Fall 2002) Lecture 7 - 47

Watershed size:7.2 km2

ERS 482/682 (Fall 2002) Lecture 7 - 48

•Performed 50 tests with disk permeameter

ERS 482/682 (Fall 2002) Lecture 7 - 49

•Performed 50 tests with disk permeameter

•Sites were selected based on:AccessibilityMinimal surface disturbanceMacropores were absent

•Tried to pick sites that represented different soil types and vegetative cover

ERS 482/682 (Fall 2002) Lecture 7 - 50

•Created GIS coveragesSoil typesVegetative groupings

•Used field method to determine average areal % of vegetation classification per disk- permeameter test

•Calculated weighted values for Ks based on average areal % vegetation cover

ERS 482/682 (Fall 2002) Lecture 7 - 51

The infiltration rates were used to estimate time to ponding and runoff potential