soil physics 2010 outline announcements recharge soil structure (pores)

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il Physics 2010 Outline Announcements Recharge Soil Structure (pores)

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Page 1: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

Outline

• Announcements

• Recharge

• Soil Structure (pores)

Page 2: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

Homework 5 is posted on the course website. There is a pdf, and an Excel spreadsheet.

• Homework 5 due Wednesday after Spring Break

• I can do a review session over Break if there is interest.

• Quiz!

Announcements

Page 3: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

Quiz

1) Sketch a graph of infiltration rate over time, with infiltration limited by the precipitation rate early, and by the soil later. Label the axes.

time, T

i(t)

, L/T

Rainfall-limited

Soil-limited

Page 4: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

Quiz

2) In the diagram below, water is flowing through the flexible tube.

(a) Describe the force(s) that cause the water to flow.

(b) Describe the force(s) that oppose the water flowing.

hhh

The matric potential in the soil pulls the water into the soil, so the water flows due to capillary forces.

In order for water to leave the Mariotte bottle, air must be pulled down into the watera distance h. Thisis buoyancy or gravitational force.

Page 5: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

Philip model

Recall that horizontal infiltration can be modeled as a diffusion process, with x(t) t½

But for vertical infiltration, the gradient is always at least 1, so x(t) → Ks at large t.

So for vertical infiltration, the short-time infiltration rate is i(t) t½ , but the long-term behavior is more like i(t) t.

Page 6: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

J. R. Philip on infiltration

Infinite series solution, with the first 2 terms dominating:

...22

3

24

3002 tA

tAtKA

t

sti

Kt

sti

2 KttsdttitI

Early time: 1st term dominatesLate time: 2nd term dominates

– conceptually like Green & Ampt

What’s this?

Page 7: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

Illustrating Philip’s concept

Sorptivity is like suction at the wetting front.

s: sorptivity, with units L T-0.5 (like the Boltzmann variable B)

I(t)

t

Sorptivity mostly shows up in Australian research.

Page 8: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

Illustrating Philip’s concept

Infiltration from a circular pond of zero depth:

• Capillary forces are small

• Gravity always dominates

• s is small

Coarse soil (e.g., sand)t = 0

t = 1

t = 2

t = 3

Page 9: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

Illustrating Philip’s concept

Infiltration from a circular pond of zero depth:

• Capillary forces are large

• Gravity is important only as t → ∞

• s is large

Fine soil (e.g., clay)t = 0

t = 1t = 2

t = 3

Page 10: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

Illustrating Philip’s concept

Infiltration from a circular pond of zero depth:

• Capillary forces dominate early

• Gravity more important over time

• s is intermediate

Medium soil (e.g., loam)t = 0

t = 1

t = 2

t = 3

Page 11: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Infiltration

Soil Physics 2010

Infiltration’s friends and relations

Precipitation

Percolation

Groundwater flow

Groundwater Recharge

Runoff

Page 12: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

Infiltration’s friends and relations

Evaporation

Groundwater flow

Groundwater Recharge

Then the rain stops.

Baseflow

Redistribution

Page 13: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

z

After the rain stops: Redistribution

Conservation of mass – blue area must remain constant

Surface soil changes from wettest to driest part of the profile with “new” water – even without evaporation.

For shallow wetting of the profile

Page 14: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

After saturating a deep, fine-textured soil:

z

Lines represent time doubling: ½ day, 1 day, 2 days, 4 days, etc.

ktt i expFor t in days, k can be quite small, e.g. k ≈ 0.0001

Averaged over some depth, we can expect something like

Page 15: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

After saturating a deep, coarse soil:

z

This thought-experiment is like the “long column” method for measuring K().

With several measurements in depth and time, and without evaporation, we could work out K() and h().

Page 16: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Recharge

Evaporation

Groundwater flow

Groundwater Recharge

Baseflow

Redistribution

Soil Physics 2010

courtesy of AJ

Page 17: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

Soil Structure (Pores)

Pore structure is about Transport, so it can be useful to examine other

transportation networks.

Page 18: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

Soil Structure (Pores)

Page 19: Soil Physics 2010 Outline Announcements Recharge Soil Structure (pores)

Soil Physics 2010

Soil Structure (Pores)

A soil acquires structure (pores and particles both) over time.

How?

Why one structure versus another?