Soil Water. Soil Water. Soils and Water, Spring Lecture 3, Soil Water 1

Similar documents
Water in Soils. Too Much Water in the Soil. Not Enough Water in the Soil. Soils and Water, Spring Lecture 4, Soil Water 1

Soil Water Relationship. Dr. M. R. Kabir

HOW WATER MOVES IN SOIL Beth Guertal Auburn University

Agry 560 Exam November 7, 2002 (135 points) (10 pages)

Water Budget IV: Soil Water Processes P = Q + ET + G + ΔS

Lecture 5. Soil Water Characteristic Curves (SWCC)

Ex: If porosity of a soil sample is 50% by volume, the moisture in each meter of a saturated soil is equivalent to 50 cm on the field surface.

Lecture 6: Soil Water

Lecture 11: Water Flow; Soils and the Hydrologic Cycle

My Notes. Ka Hana Imi Na auao A Science Careers Curriculum Resource Go to: 1

Soils & Hydrology ( Part II)

Sedimentation and Remote Sensing

THE PORTION OF THE SOIL WATER THAT IS USABLE BY PLANTS. DIFFERENCE BETWEEN FIELD CAPACITY AND WILTING POINT.

Agronomy 406 World Climates

WHAT IS SOIL? soil is a complex system of organic and inorganic (mineral) compounds Soil properties depend on formation process particle size climate

Agry 465 Exam November 17, 2004 (100 points) (8 pages)

General Groundwater Concepts

Texture Definition: relative proportions of various sizes of individual soil particles USDA classifications Sand: mm Silt:

An Introduction into Applied Soil Hydrology

What is the Vadose Zone? Why Do We Care? Tiffany Messer Assistant Professor Biological Systems Engineering School of Natural Resources University of

ENGINEERING HYDROLOGY

Water Related Soil Properties

POROSITY, SPECIFIC YIELD & SPECIFIC RETENTION. Physical properties of

Introduction to Land Surface Modeling Hydrology. Mark Decker

Lecture 20: Groundwater Introduction

Lecture Notes on Groundwater Hydrology. Part 1

Outline 12/9/2010. Two Variables are Needed to Describe the State of Water. Definition: Volumetric Water Content Definition: Gravimetric water content

The Hydrological Cycle. Hydrological Cycle. Definition of Terms. Soils and Water, Spring Lecture 7, The Hydrological Cycle 1

Page 1. Name:

SEES 503 SUSTAINABLE WATER RESOURCES GROUNDWATER. Instructor. Assist. Prof. Dr. Bertuğ Akıntuğ

Simplified Procedure for Unsaturated Flow Parameters

The soil is a very. The soil can. The manure. Soil Characteristics. effective manure treatment system if manures are applied at the proper rate.

APPENDICES SYMBOLS AND NOTATION GLOSSARY. Copyright 2003 David G Tarboton, Utah State University

Geol 220: GROUNDWATER HYDROLOGY

SOIL AND THE HYDROLOGIC CYCLE

Rainwater harvesting and greywater recovery - Part 1 -

CE 240 Soil Mechanics & Foundations Lecture 4.3. Permeability I (Das, Ch. 6)

Topic 2: Occurrence & Movement of Groundwater

This document downloaded from vulcanhammer.net vulcanhammer.info Chet Aero Marine

3/7/ Basic Types of Rocks. A Brief Review of Physics

Chapter 3 THEORY OF INFILTRATION. 3.1 General

Groundwater 3/16/2010. GG22A: GEOSPHERE & HYDROSPHERE Hydrology

Understanding Hydrologic Process for Better Stormwater Management

PE Exam Review - Geotechnical

Infiltration. Infiltration is the term applied to the process of water entry into the soil. The rate of infiltration determines

Water balance at the field and watershed scale.

THE INFLUENCE OF VARYING COMPOSITION OF SOIL SAMPLES ON WATER FLOW RATE (2MM SHARP SAND 1MM MEDIUM SAND)

FACT FLASH. 5: Groundwater. What is groundwater? How does the ground store water? Fact Flash 5: Groundwater

Precipitation Surface Cover Topography Soil Properties

FELIX JARIA Soil Moisture measurement

Remediation of Brine Spills- What Goes Wrong Kerry Sublette

Introduction. Welcome to the Belgium Study Abroad Program. Courses:

EFFECTIVENESS OF UNSATURATED DRAINAGE LAYER IN WATER DIVERSION UNDER DIFFERENT RAINFALL CONDITIONS

TOOLS AND TIPS FOR MEASURING THE FULL SOIL MOISTURE RELEASE CURVE

9/9/ Basic Types of Rocks. Porosity of Earth Materials

Groundwater Flow Demonstration Model Activities for grades 4-12

Evapotranspiration Calculations for Stormwater Quality Models

Evapotranspiration Calculations for Stormwater Quality Models

Other Septic Tank Effluent Dispersal Options

Water Resources Management Plan

Hydrologic Cycle. Rain Shadow:

Soil Mechanics FLUID FLW IN SOIL ONE DIMENSIONAL FLOW. Tikrit University. College of Engineering Civil engineering Department

2. WATER IN SOIL 2.1 ADSORBED WATER

Published by: PIONEER RESEARCH & DEVELOPMENT GROUP ( 1

CHAPTER 13 OUTLINE The Hydrologic Cycle and Groundwater. Hydrologic cycle. Hydrologic cycle cont.

2012 Soil Mechanics I and Exercises Final Examination

Looking at movement of energy through natural systems

Development of Water Demand Forecasting Service for Cropping Land

Source of Pollution or Groundwater Solution?

Operating, Calibrating, and Maintaining Irrigation Systems

Placement and Interpretation of Soil Moisture Sensors for Irrigated Cotton Production in Humid Regions SITE SELECTION IN A FIELD OBJECTIVE

Computation of excess stormflow at the basin scale. Prof. Pierluigi Claps. Dept. DIATI, Politecnico di Torino

Lecture 2: Soil Properties and Groundwater Flow

A Normalized Function for Predicting the Coefficient Permeability of Unsaturated Soils

Maria Claudia Zingariello Centro euro-mediterraneo per i cambiamenti climatici S.C.a.r.l., CMCC. ISC - Impacts on ground and coast.

Available online at ScienceDirect. Energy Procedia 85 (2016) 93 98

Vadose/unsaturated. (Basic concepts) Lucila Candela ERASMUS

A soil moisture accounting-procedure with a Richards equation-based soil texturedependent

The Soil Water Characteristic - Introduction and Measurement

Loss Control TIPS Technical Information Paper Series

Scientific registration n : 1368 Symposium n : 3 Presentation : poster. HASEGAWA Shuichi

Simplified Forms of Surface Runoff Estimation Method for Silt- Loam Soils Suat Irmak, Soil and Water Resources and Irrigation Engineer, Professor

A Short Course on Soil McDaniel s Nut Grove Wednesday, October 12 th, Soil Characteristics

9. SOIL PERMEABILITY. 9.0 Why is it important to determine soil permeability?

Desiccation of Porous Media: Intermediate-Scale Flow Cell Experiments and Numerical Simulations

Methods of Irrigation Scheduling and Determination of Irrigation threshold triggers

Overview. Learning Objectives: This module provides step-by-step instructions in how to do the Bulk Density Protocol.

A Preliminary Experimental Analysis of Infiltration Capacity through Disturbed River Bank Soil Samples

Chapter 4 Soil Properties

The Decline of Soil Infiltration Capacity Due To High Elevation Groundwater

GEOTECHNICAL & SOILS LABORATORY PERMEABILITY TEST : CONSTANT HEAD & FALLING HEAD

Sensor Strategies in Cotton. Stacia L. Davis, Ph.D. Assistant Professor Irrigation Engineering LSU AgCenter

Stormwater Retention Pond Recovery Analysis

VADOSE/W 2D Tutorial

CHARACTERISTIC LENGTHS AFFECTING EVAPORATION FROM HETEROGENEOUS POROUS MEDIA WITH SHARP TEXTURAL BOUNDARIES. D. Or, P. Lehmann, N.

TENSIOMETER Hydrostatic pressure potential Piezometer

Applying Polyacrylamide (PAM) to Reduce Seepage Loss of Water Through Unlined Canals

Distance from inlet end (ft)

Water Resources Engineering. Prof. R. Srivastava. Department of Water Resources Engineering. Indian Institute of Technology, Kanpur.

Soil Physical Properties and Wastewater Treatment

Transcription:

Soil Water Importance. Global distribution. Properties of water. Amount and energy of water in soil. Hydraulic properties (hydraulic conductivity and water retention). Soil Water Objectives Gain an appreciation of the importance of soils as mediators of matter (gas and liquid) and energy (temperature) exchanges at the surface of the earth. Distinguish between water quantity and water energy. Learn the principles of water movement. http://www.wcc.nrcs.usda.gov/scan/ SCAN plotter at http://hydrolab.arsusda.gov/cgi-bin/plotscandata.pl Lecture 3, Soil Water 1

Soil Climate Limitations to Agriculture Climate driven Soil driven Soil driven Source: Linking Land Quality, Agricultural Productivity, and Food Security. 003. K. Wiebe. Resource Economics Division, Economic Research Service, U.S. Department of Agriculture. Agricultural Economic Report No. 83. Irrigation Irrigated land account for only 0% of cropland but it produces 40% of the global harvest. However, between 0% to 30% of the irrigated land is affected by salinization caused by improper management. The other problem is water availability. Population and food consumption continues to grow, while water availability for agriculture is expected to decrease from 70% to 6% by 00. Water in Soils Natural Resource Conservation Service, U.S.D.A. Lecture 3, Soil Water

Distribution of Wetlands Too Much Water in the Soil Use of Histosol for fuel (Scotland) Subsidence in a drained Histosol (Everglades, Florida) http://soils.ag.uidaho.edu/soilorders/histosols.htm Not Enough Water in the Soil Lecture 3, Soil Water 3

The Dust Belt Global distributions of dust and smoke: monthly frequency of occurrence of TOMS absorbing aerosol product over the period 1980 199. (a) January and (b) July. Scale is number of days per month when the absorbing aerosol index (AAI) equals or exceeds 0.7. In July the large dark area in southern Africa is due to biomass burning. In January, there is biomass burning in the region just north of the equator in Africa; part of the plume over the equatorial ocean is due to smoke. Essentially, all other distributions in Figure 1 are due to dust. Source: J. M. Prospero, J.M., P. Ginoux, O. Torres, S. E. Nicholson, and T. E. Gill. 00. Environmental characterization of global sources of atmospheric soil dust identified with the nimbus 7 total ozone mapping spectrometer (TOMS) absorbing aerosol product, Rev. Geophys., 40(1), 100, doi:10.109/000rg000095. Expressing the Amount of Water in Soil Volume percentages of soil components Air Water Mineral Organic Gravimetric water content: mass of water/mass of dry soil [g of water/g of soil] Volumetric water content: volume of water/volume of soil [m 3 of water/m 3 of soil] Molecular Structure of Water Source: http://www.physicalgeography.net/fundamentals/8a.html Lecture 3, Soil Water 4

Surface Tension (Cohesion) Figure 5.3 Everyday evidences of water s surface tension (left) as insects walk on water and do not sink, and of forces of cohesion and adhesion (right) as a drop of water is held between the fingers. (Photos courtesy of R. Weil and E. Tsang) Water Arrangement Around a Charged Surface (Adhesion) Source: http://www.physicalgeography.net/fundamentals/8a.html Summary of Concepts Water is retained in soil in small crevices: cohesion Dry Wet adhesion Sat. The smaller the pores the greater the forces retaining the water in place. Lecture 3, Soil Water 5

0.1 mm A and B are pores filled with water, C is an empty pore. Courtesy of Prof. Haim Gvirtzman, Inst. of Earth Sciences, The Hebrew University of Jerusalem The Concept of Energy Work, W, is the product of a force, F, acting over a distance, s: W = Fs [ Nm ] = [ J ] Work done on fluids can either increase or decrease their Energy. There are different types of energy. According to the principle of conservation of energy when energy is transformed in exactly equivalent amounts. Bernoulli s Equation A v A 1 P v 1 DATUM P 1 z 1 z 1 1 [ P + ρ g z + ρ v ] 1 = [ P + ρ g z + ρ v ] pressure gravitational kinetic In practice, losses of energy occur as a result of nonnegligible viscosity and a term accounting for the losses caused by friction or drag should be considered. Lecture 3, Soil Water 6

Energy in Water Figure 5.8 Whether concerning matric potential, osmotic potential, or gravitational potential (as shown here), water always moves to where its energy state will be lower. In this case the energy lost by the water is used to turn the historic Mabry Mills waterwheel and grind flour. (Photo courtesy of R. Weil) Figure 5.7 Relationship between the potential energy of pure water at a standard reference state (pressure, temperature, and elevation) and that of soil water. If the soil water contains salts and other solutes, the mutual attraction between water molecules and these chemicals reduces the potential energy of the water, the degree of the reduction being termed osmotic potential. Similarly, the mutual attraction between soil solids (soil matrix) and soil water molecules also reduces the water s potential energy. In this case the reduction is called matric potential. Since both of these interactions reduce the water s potential energy level compared to that of pure water, the changes in energy level (osmotic potential and matric potential) are both considered to be negative. In contrast, differences in energy due to gravity (gravitational potential) are always positive. This is because the reference elevation of the pure water is purposely designated at a site in the soil profile below that of the soil water. A plant root attempting to remove water from a moist soil would have to overcome all three forces simultaneously. Lecture 3, Soil Water 7

A Look at the Units Each term in the following equation is expressed in units of pressure, kpa: 1 P + ρ g z + ρ v What is the relation between the definition of work, W, and the energy terms in the Bernoulli s equation? N N m = 3 m m J W = 3 m volume Expressing Potential Energy of Water in Soils Type of Expression Units W vol W Weight J N = = 3 m m W J = mass kg = J = kg ms m kg ms kg ms Pressure (kpa) No special unit Length ( head ) Three dimensional view of pores in sand W D Lecture 3, Soil Water 8

Energy in Soils A A 1 P P 1 DATUM z 1 z 1 Water moves slowly in soils. Thus, ρ v ~ 0 and: [ P + ρ g z] = Total Potential [ kpa] Where P is pressure or matric potential and ρgz is the gravitational potential. Water Potentials 50 ml Darcy s Experiments h 1 ΔH = H 1-H A H 1 Sand h z 1 L H Q/A = q z Reference Level or Datum (z = 0) H H L q 1 H H1 q = K S L Lecture 3, Soil Water 9

Justification of Darcy s Law Energy loss is caused by frictional force, F d, and is measured as: H. H 1 Water movement in soil is slow (laminar). Thus, Fd v Fd q Note: q=q/a, where Q is flux (L 3 /T) and A is area (L ). Since W = F L ql H H or d 1 H H q 1 L H H q K = 1 s L Examples of Darcy s Law D = R D = R 1 H WATER SOIL L h 1 Q SOIL L h Ref. Level WATER Q H h z H h z H 1 (inlet) h L H (outlet) 0 0 H H 1 -h -L H (inlet) H 1 (outlet) H 1 H h 0 -h 0 L L Example Darcy s Law The diagram below shows a ditch intercepting seepage under a roadbed. The saturated hydraulic conductivity of the pervious material is 0.4 m day -1. Assuming that the length of the ditch is 400 m, calculate the volume of water seeping into the ditch during one day. Diagram 1. Ditch intercepting water flowing underneath a road. Lecture 3, Soil Water 10

Conceptualization of Soil Pore Systems CT representation of pores in a sandy material Soil pores represented as capillary tubes What is soil hydraulic conductivity? The ease of water flow through soil A r 4 π r ρ g Δ P Q = 8 μ L Q (Poiseuille s Law) Q 4 A r r ρg Ks = 8 μ Saturated hydraulic conductivity is proportional to the square of pore radius Adhesion and Cohesion in Soil Pores Large Pore Small Pore Large pores drain faster and retain less water than small pores. Large pores are predominant in sandy soils, while small pores are typical of clay soils. Lecture 3, Soil Water 11

Water Movement in Capillary Pores Small Pore Large Pore Figure 5.13 Saturated flow (percolation) in a column of soil with cross-sectional area A, cm. Sandy Soil Clay Soil >> Q Q 1 Lecture 3, Soil Water 1

Texture and Soil Permeability This diagram shows a general relationship between soil permeability and soil texture. In a profile, the texture of the least permeable horizon must be considered. Remember, however, that soil structure is also very important in determining permeability. Unsaturated Soil The capillary model The soil water retention curve Field capacity Wilting point Hygroscopic water Unsaturated hydraulic conductivity Infiltration Lecture 3, Soil Water 13

Saturated vs. Unsaturated Water Flow Saturated Flow water air Unsaturated Flow Capillary Action Large pore Small pore Dry glass beads glass beads + water Pipette Water removal: stage 1 Water removal: stage Adapted from: www.wtamu.edu/~crobinson/soilwater/capact.html#1 Figure 5.4 The interaction of water with a hydrophillic surface (a) results in a characteristic contact angle (a). If the solid surface surrounds the water as in a tube, a curved water air interface termed the meniscus forms because of adhesive and cohesive forces. When air and water meet in a curved meniscus, pressure on the convex side of the curve is lower than on the concave side. (b) Capillary rise occurs in a fine hydrophillic (e.g., glass) tube because pressure under the meniscus (P) is less than pressure on the free water. Lecture 3, Soil Water 14

Hydrophobic Surfaces Analysis of Capillary Rise Capillary Tube Radius (r), Material (Glass) Properties of Interest Fluid (Water) Surface Tension (γ), Contact Angle (α), Density (ρ) Analysis of Forces Adhesion + Cohesion (upward) π r γ cosα Gravity (downward) m g = ρ V g = ρ π r h g Final Expression h = γ cosα ρ gr Final Expression Simplified h = 0.15 r [h and r are in cm] The Capillary Model in Soils Dry Wet The pressure or matric potential is determined by the shape of the water-air interface: Dry Wet Sat. Saturated Lecture 3, Soil Water 15

Dry soil: Water retained in small pores, high energy required to remove water from these pores. Water moves extremely slowly. Wet soil: balanced content of air and water in pores. There is enough O and water movement is rapid enough to sustain most aerobic processes. Saturated soil: all pores filled with water. Highest flow rate of water, but typically O is absent. Thus, anaerobic processes dominate the system. Capillary Effect in Field Soils h i Mostly saturated soil Saturated soil h i h i Figure 5.9 The matric potential and submergence potential are both pressure potentials that may contribute to total water potential. The matric potential is always negative and the submergence potential is positive. When water is in unsaturated soil above the water table (top of the saturated zone) it is subject to the influence of matric potentials. Water below the water table in saturated soil is subject to submergence potentials. In the example shown here, the matric potential decreases linearly with elevation above the water table, signifying that water rising by capillary attraction up from the water table is the only source of water in this profile. Rainfall or irrigation (see dotted line) would alter or curve the straight line, but would not change the fundamental relationship described. Lecture 3, Soil Water 16

Figure 5.17 The wetting front 4 hours after a 5 cm rainfall. Water removal by plant roots had dried the upper 70 to 80 cm of this humid-region (Alabama) profile during a previous 3-week dry spell. The clearly visible boundary results from the rather abrupt change in soil water content at the wetting front between the dry, lighter-colored soil and the soil darkened by the percolating water. The wavy nature of the wetting front in this natural field soil is evidence of the heterogeneity of pore sizes. Scale in 10 cm intervals. (Photo courtesy of R. Weil) Figure 5.6 As this field irrigation scene in Arizona shows (left), water has moved up by capillarity from the irrigation furrow toward the top of the ridge. The photo on the right illustrates some horizontal movement to both sides and away from the irrigation water. The Soil Water Retention Curve h θ v Lecture 3, Soil Water 17

Water Retention Measurement Ceramic Plate h Saturated Soil Sample Hanging Water Column Pressure Plate Extractor P (kpa).9 5.9 9.8 33.3 100 00 500 1000 1500 θ v 0.5 0.45 0.30 0.0 0.15 0.1 0.11 0.06 0.04 Figure 5.4 Water content matric potential curve of a loam soil as related to different terms used to describe water in soils. The wavy lines in the diagram to the right suggest that measurements such as field capacity are only approximations. The gradual change in potential with soil moisture change discourages the concept of different forms of water in soils. At the same time, such terms as gravitational and available assist in the qualitative description of moisture utilization in soils. Animations: software Lecture 3, Soil Water 18

Figure 5.3 Volumes of water and air associated with a 100 g slice of soil solids in a well-granulated silt loam at different moisture levels. The top bar shows the situation when a representative soil is completely saturated with water. This situation will usually occur for short periods of time during a rain or when the soil is being irrigated. Water will soon drain out of the larger pores (macropores). The soil is then said to be at the field capacity. Plants will remove water from the soil quite rapidly until they begin to wilt. When permanent wilting of the plants occurs, the soil water content is said to be at the wilting coefficient. There is still considerable water in the soil, but it is held too tightly to permit its absorption by plant roots. A further reduction in water content to the hygroscopic coefficient is illustrated in the bottom bar. At this point the water is held very tightly, mostly by the soil colloids. (Top drawings modified from Irrigation on Western Farms, published by the U.S. Departments of Agriculture and Interior) Figure 5.5 General relationship between soil water characteristics and soil texture. Note that the wilting coefficient increases as the texture becomes finer. The field capacity increases until we reach the silt loams, then levels off. Remember these are representative curves; individual soils would probably have values different from those shown. Lecture 3, Soil Water 19

Figure 5.15 Generalized relationship between matric potential and hydraulic conductivity for a sandy soil and a clay soil (note log scales). Saturation flow takes place at or near zero potential, while much of the unsaturated flow occurs at a potential of 0.1 bar (10 kpa) or below. Infiltration: Lab Experiment Early Stage End of Experiment Sandy loam Silt loam Is there a model (mathematical expression) to quantify our observations? Examples of Motion Distance, x a x t a>1 a=1 a<1 When a=1, the motion is easy to solve: linear function. When a 1, the equation is linearized: log( x ) alog( t ) Which case represents water movement in soils? Time, t Lecture 3, Soil Water 0

Water Movement in Soils 1.6 1.4 1. log (x) = 0.61 log (t) - 0.59 R = 0.9971 log (x/cm) 1 0.8 0.6 Sandy Loam Silt Loam 0.4 0. log (x) = 0.4 log (t) - 0.5 R = 0.9845 0 0 1 3 4 log (t/s) Sandy Loam x = 0.6 t 0.61 v=dx/dt=0.16 t -0.39 Silty Loam x = 0.30 t 0.4 v=dx/dt=0.13 t -0.58 Two ways to Represent the Data distance, cm 30 5 0 15 Δy dy 10 Δx dx 5 0 0 1000 000 3000 4000 time, s x = 0.6 t 0.61 Sandy Loam: 1 Silt Loam: Predicted 1 Predicted d[ax B ]/dy= AB x B-1 velocity of wetting front, cm/s 0.045 0.040 0.035 0.030 0.05 risky: no data 0.00 0.015 0.010 0.005 0.000 0 1000 000 3000 4000 time, s v=dx/dt = 0.16 t -0.39 Sandy Loam Silt Loam Extrap. Sandy Loam Extrap. Silt Loam From Wetting Front to Infiltration Rates q = velocity x porosity If porosity = 40% q, cm/s 0.018 0.016 0.014 0.01 Sandy Loam 0.010 Silt Loam 0.008 Extrap. Sandy Loam 0.006 Extrap. Silt Loam 0.004 0.00 0.000 0 1000 000 3000 4000 time, s 5.000 0.000 q, in/h 15.000 10.000 Sandy Loam Silt Loam Extrap. Sandy Loam Extrap. Silt Loam 5.000 0.000 0 0. 0.4 0.6 0.8 1 1. time, h Lecture 3, Soil Water 1

Infiltration and Runoff q, in/h 5.000 0.000 15.000 10.000 8 times the Design Storm 5.000 X X 0.000 0 0. 0.4 0.6 0.8 1 1. time, h Ponding Time Runoff in Silt Loam Runoff in Sandy Loam Sandy Loam Silt Loam Extrap. Sandy Loam Extrap. Silt Loam Rainfall Rainfall x 4 1.5 in/h Design Storm for Stormwater BMP s Lecture 3, Soil Water