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175 Cards in this Set
- Front
- Back
most important soil moisture parameters in agriculture
|
field capacity
& permanent wilting pt |
|
field capacity
|
maximum h2o content without drainage
(before gravity drainage starts |
|
permanent wilting pt
|
water content when water held too tightly for plant uptake
(unavailable to plants) |
|
soil moisture cycle
|
fall: rainfall recharge
winter: MAX soil storage spring: some evaporative loss summer: most depleted |
|
porosity equation
|
n = Vv / Vt
Vv = volume voids Vt = total unit volume n = porosity |
|
porosity expressed as
|
percent or
decimal fraction |
|
porosity (rock v soil)
|
rocks lower porosity than soil
(less pore space in rocks) |
|
porosity and hydraulic conductivity
(n and K) |
higher n usually = higher K
higher porosity = higher hydraulic conductivity [[hydraulic conductivity = the ability of medium to transmit fluid]] --{depends on fluid's properties and porous medium's properties} **CLAY SOILS EXCEPTION** |
|
when does higher porosity not result in higher hydraulic conductivity
|
CLAY SOILS
higher porosity doesn't increase clay's ability to transmit fluid |
|
infiltration
|
movement of water into soil
|
|
infiltration varies with time
|
varies with TIME
as a function of: -precipitation intensity -changes in soil tension -hydraulic conductivity with changing soil moisture |
|
infiltration varies with (not time)
|
previous moisture conditions
slope |
|
precip rate < infiltration rate
|
all water that reaches surface infiltrates
|
|
precip rate > infiltration capacity
|
get depression (detention) storage
|
|
if ground is sloping depression storage..
|
depression storage may be small
-- overland flow will begin soon after depression storage filled |
|
infiltration if ground is already saturated
("saturated from below") |
depression storage occurs immediately
if W(t)>Fc(t) |
|
measuring infiltration
(pt measurements) |
1. ring infiltrometer
2. dbl-ring infiltrometer 3. observing soil water changes 4. sprinkler plot studies |
|
measuring infiltration
(over an area) |
1. use stream discharge records & precip records
2. rain gage data used to determine amt of rain that fell on drainage basin 3. analyze hydrograph (determine amt of runoff) precip - runoff = infiltration |
|
factors influencing infiltration
|
1. permeability of surface material
2. slope 3. antecedent (previous) moisture conditions 4. human activities |
|
"desertification"
|
loss of productive / marginally productive land
due to poor land use practices **soil becomes dry **loss of vegetation **reduced soil fertility **hardening of soil --> infiltration decreases --> erosion increases |
|
causes of desertification
|
-overgrazing
-woodcutting -poor farming practices -poor water management on cultivated lands -climate change over irrigation... |
|
over-irrigation
|
can lead to salinization of soils
--salts precipitate from evaporation irrigation water --contributes to DESERTIFICATION |
|
F
|
amount of infiltration
(cumulative infiltration over time period) |
|
f(t)
|
infiltration rate
f(t) = dF/dt (change in amt of infiltration over change in time) **depends on w(t) |
|
w(t)
|
water input rate
(snowmelt or precipitation intensity) |
|
f -sub-c (t)
|
maximum rate at which infiltration can occur
|
|
infiltration rate
f(t) |
HIGH if soil initially dry
if w(t) (water input rate) is constant, f(t)decreases to near-constant value (~Ksat) |
|
K
|
hydraulic conductivity
in velocity units --describes soil in cylinder w/ water moving thru it |
|
darcy's law valid for
|
groundwater flow in any direction
|
|
hydraulic conductivity (K) is function of
|
fluid and medium
|
|
K relationships
|
K increases with increasing h2o content
K at max at saturation saturated K depends strongly on grainsize Ksat depends on soil texture |
|
darcy's law based on
|
experiment
(empirical) |
|
pressure developes in groundh2o when
|
it flows thru porous mediums
|
|
"fluid potential"
|
water flow due to potential
= the mechanical energy / mass fluid *related to elevation / pressure |
|
fluid flow (happens due to fluid potential)
|
-must overcome water-soil friction
-must transfer mechanical energy -> thermal energy -flows from higher mechanical energy to lower mechanical energy |
|
"bulk density"
|
density of a dry sample
|
|
"porosity"
|
volume of voids : volume of solids
(ratio) |
|
"volumetric water content"
|
water volume: soil volume
|
|
"soil wetness"
|
degree of saturation
*the proportion of pores that contain water |
|
"capillary fringe"
|
the pt when air begins to appear in the soil pores
|
|
in unsat,
hydraulic conductivity v water content |
hydraulic conductivity increases with increasing water content
... then levels off and becomes constant (when soil is saturated) |
|
what's darcy's law used for
|
calculating the rate of floow
in a given direction based on the resistence of the medium and the applied gradient |
|
direction of flow
(according to darcy's law) |
flow occurs in direction of decreasing hydraulic gradient
(goes from high to low hydraulic gradient) (-) hydraulic gradient = water is moving up |
|
(-) hydraulic gradient
(h2o movement) |
water is moving up
|
|
(+) hydraulic gradient
(h2o movement) |
water is moving down
|
|
"groundwater"
|
subsurface water below the water table
--in saturated soil and geologic formations |
|
groundwater
(geology / chemistry / hydrology / technology) |
GEOLOGY:
-flow (qualitative) -fluid mechanics -groundh2o behaves as field CHEM: -contaminants, -dating groudh2o HYDRO: -flow -applied math TECHNOLOGY: -drilling / maintaining wells -sampling -logging |
|
"aquifer"
|
saturated permeable geologic unit
(can transmit sign. amt of h2o) |
|
"aquiclude"
|
saturated geologic unit that canNOT transmit sign. amt of h2o
|
|
"aquitard"
|
less permeable geologic bed
|
|
thruflow occurs
|
in unsat zone
(above h2o table) (below surface) |
|
artesian well
|
when confined aquifer in saturated zone has well
(well punctures into aquifer below water table) |
|
water-table well
|
well in the water table
-- height of water = height of capilary fringe |
|
cone of depression
|
depression of water table around well (in h2o table)
|
|
"mass density"
|
curved p
(1000..) |
|
"weight density"
|
greek y
(weight per unit volume) = curved p * gravity |
|
Specific Gravity (G)
|
ratio of (something's)density to water
|
|
viscocity
|
greek u
(property of liquid's resistence to motion) |
|
compressability
|
greek B
= stress (fluid pressure) / strain properties |
|
"piezometers"
|
measure hydraulic head in aquifer
-open at bottom -intake of h2o only |
|
"specific storage"
|
volume h2o released from aquifer due to unit
DECLINE IN HYDRAULIC HEAD |
|
"storativity"
|
unit h2o released by aquifer per unit decline hydraulic head NORMAL TO SURFACE
|
|
ET includes
|
1. E from surface h2o
2. E From land surfaces 3. E from soil 4. SUBLIMATION snow / ice 5. TRANSPIRATION |
|
RO =
|
runoff =
P - ET |
|
evap losses from
|
man made reservoirs huge
|
|
errors in rainfall / RO measurements often due to
|
ET
|
|
measuring ET
|
difficult
.. usually models used |
|
evap models based on
|
1. water balance
2. energy balance 3. mass transfer 4. combo approach |
|
evap pans
|
-measure free water evap
-moniter precip (depth in pan) E = W - (V2 - V1) evap = precip (total depth) - change in depth "pan coefficients" = correction factors to convert pan data to lake estimates |
|
"pan coefficients"
|
correction factors for evap pans to convert data to lake estimates
|
|
bowen ratio
|
H / LE
sensible heat flux / latent heat flux |
|
lake evap
|
function of wind speed, temp, humidity gradient
-related to solar energy **measured by 1. mass transfer, 2. energy budget 3. pan evap |
|
green-ampt equation describes
|
infiltration into dry soils
... h2o progesses downward -- sharp wetting front seperates unsat soil below from sat soil above... this front progresses downward as infiltration occurs - assumes wetting front infinitely sharp (horizontal) *so the flux in the sat upper portion equals the infiltration rate ((IE the hydraulic gradient is uniform)) |
|
green ampt equation
|
i = -Ks [[(-pressheadf + 0)/Lf ]+1]
i = infiltration rate (= spec discharge) Ks = sat conductivity pressure head symbol sub f = pressure head at wetting front Lf = depth to the wetting front |
|
most imp factors governing infiltration of water
|
1. precip rate
2. K of soil (hydraulic conductivity) 3. initial soil moisture 4. slope / roughness of surface |
|
soil moisture affects
|
1. soil moisture tension
2. K (hydraulic conductivity) 3. how much storage available |
|
as water moves deeper (with infiltration)
|
the ratio of
soil moisture tension at wetting front : depth of the wetting front becomes smaller bc total volume h2o is distributed over a greater depth (and i decreases) *as ratio becomes very small i (or f(t)) approaches Ksat |
|
"logging for water"
|
WANT: to log to increase snowmelt
RESULTS: when trees removed: -more snow collected in the openings -more h2o ran off into streams in spring |
|
why logging increases snomelt
|
snow that is intercepted by trees sublimates (turns directly from snow to h2o vapor) -- never reaching the ground
|
|
prob with logging for snowmelt
|
it doesnt work everywhere
when it does work: -increased RO pollutes streams with sediments (degrades fish habitat) -the increase in RO is only measurable in spring -- new reservoirs need to be built to capture extra h2o |
|
eddy flux instrument
|
measures latent heat
(knowing latent heat can convert to mm sublimation) ** can have instrument below and above forest canopy** ---can measure sublimation below and above --ie canopy sublimation and below canopy sublimation |
|
precip and sublimation
|
increase precip = increase sublimation
canopy sublimation greater than snowpack sublimation |
|
eddy covariance systems indicated..
|
substantial loss of winter snow accumulation by SUBLIMATION
(canopy more than snowpack) **more than 100% precip lost to sublimation |
|
max sublimation occured
(eddy covariance experiment) |
immediately after snowmelt
-driven by canopy interception *HIGH LE flux |
|
below canopy sublimation driven by
(eddy covariance experiment) |
driven by high H (sensible heat) gradients
--- warm canopy pumping heat into cold atmosphere high H gradient ==> high spec humidity gradient -RH (relative humidity) = 100% at snow surface -RH much lower above snow surface -----> lead to high snowpack sublimation |
|
sublimation higher when intercepted by veg than on the ground ...
|
bc leaf surface is higher temp
-leaf = greater surface area -trees radiate longwave -higher air temp around canopy -- INCREASE IN SAT VAPOR PRESSURE |
|
decreasing interception by cutting trees =..
|
increases volume of snowpacak
increases water yield |
|
the more trees removed...
|
the greater the SWE increased
(snow water equivilant) |
|
as size of opening increases
(logging experiment) |
its snow trapping efficiency decreases
(to the pt where there is a net loss) --- due to increased wind scouring and sublimation losses |
|
influence of wind in logging experiment
|
more wind = less efficient
- SWE greatest on leeward side of clearing - SWE least on windward side of clearing |
|
flow increased most...
(logging experiment) |
during wet years
(opposed to droughts) |
|
(-) of logging for snowmelt
|
-increases in discharge = increase erosion / flooding
-need additional reservoirs to store water for low flows -logging related activities (including road construction..) = increase erosion and Sedimentation NUTRIENT LOADING: -increase in nutrient loading -increase in DOC -increase in ion concentrations increases in nitrate concentrations ..due to ((reduced nutrient uptake bc less vegetation)) ((nutrient release from decomp of trees)) ((increased soil N transformations)) -remove habitat -maintanence required to maintain yields ($$$) --h2o flow off trees increases with age.. |
|
debate: "dual purpose of logging"
|
1. increase water yeild
2. reduce fire risk (but logging at high elevations [[not high fire risk]] -wont reduce high fire risk of low elevations |
|
higher elevation = less ET
|
less trees at high elevation
colder air temps with elevation |
|
"PBL"
|
planetary boundary layer
(layer of atmosphere where air motion strongly influenced by interaction with earth surface) **CHARACTERIZED BY TURBULENT AIR FLOW** - imagined as horizontal flow of mult rotating eddies (each eddy has 3d component including vertical wind component) |
|
eddie covariance experiment
uses |
IRGA
-IR gas analyzer -sonic anemometer *measures evap flux and LE flux |
|
each parcel of air has a particular..
(eddy covariance experiment) |
1. trace gas concentration
2. temperature 3. humidity |
|
vertical flux
(eddy covariance experiment) |
eddie flux:
F = (density air)(w)(s) latent heat flux (on eq. sheet) |
|
"footprint"
(eddy covariance experiment) |
'field of view'
-area that contains the sources / sinks contributing to a certain measurement pt (reflects surface's influence on the measured turbulent flux) |
|
assumption
(eddy covariance experiment) |
pt measurements represent upwind area
footprint contains only area of interest flux is fully turbulent (vertical transfer done mostly by eddies) |
|
"bulk density"
+ eq |
bulk density is the density of DRY SOIL
Pb = Mm / Vs bulk density = mass of dry matrix / total soil volume |
|
porosity eq
|
pososity = void space / total volume
(Va + V) / Vs air volume + water volume / total soil volume = 1 - (bulk density / particle density) |
|
moisture content (theta)
eq |
= Vw / Vs
volume water / soil volume = (Mswet - Msdry) / (Pw*Vs) |
|
soil wetness
ie DEGREE OF SATURATION (S) eq |
moisture content / porosity
= volume water / (volume air + volume water) |
|
capillary fringe defined as
|
pt at which air begins to appear in soil (VERY CLOSE to saturization -- if not completely saturated)
|
|
moisture content (PWP)
eq |
PWP =
(porosity)*{[abs value pressure head -sub ae]/1500}^1/b pressure head -sub ae = air entry tension b = describes moisture curve |
|
how does K change with increasing moisture content
|
increasing moisture content
= increasing hydraulic conductivity (eventually levels off to constant Ksat (K under saturated conditions) |
|
the pt of saturation:
|
when moisture content no longer increases (stays constant) with increasing pressure head
|
|
h =
|
hz + hp
elevation head + pressure head |
|
hz
|
elevation head
= z - z0 (elevation minus the arbitrary datum) |
|
hp
|
pressure head
= water pressure / weight density of h2o |
|
(-) hydraulic gradient means water is moving
|
up
|
|
green-ampt equation
|
i = - Ks [{(-pressure head sub f) / Lf}+1]
i = infiltration rate Ks = saturated conductivity Presshead f - pressure at wetting front Lf = depth to wetting front |
|
I
(green-ampt) |
total infiltration
= Lf * change moisture content Lf = depth to wetting front change in moisture content = saturated - initial |
|
time to ponding related to initial miosture content
green-ampt |
time to ponding decreases with increasing initial water content
|
|
low initial moisture content v
high initial moisture content the rate the wetting front increases ... |
wetting front increases faster in soils with high initial moisture
(fewer voids to fill --- must fill all voids b/c wetting front is "SATURATED ZONE" |
|
"time of ponding"
green-ampt equation |
when the top of the soil becomes saturated
|
|
after 'time of ponding'
|
ie after top of soil = saturated,
the rate of infiltration increase decreases slightly |
|
hydraulic conductivity :
aquiclude v aquifer |
aquifer = high hydraulic conductivity
aquiclude - low hydraulic conductivity |
|
Unconfined aquifer:
what is pressure head at water table? |
pressure head is 0 @ water table
-- hydraulic head = the elevation head (ie h = z +0) |
|
transmissivity
|
T = Ksat*b
b= thickness of aquifer |
|
when comparing heights of the water table
for spec discharge |
q = -K dh/dl
q = -K * [(Pressure2 + z2) - (pressure1 + z1)]/l2-l1 **CAN ELIMINATE PRESSURE HEAD bc PRESSURE HEAD = 0 at height of water table |
|
simplified hydraulic equation
|
Qstream = PPT - ET
|
|
area
|
A = pi*r^2
|
|
volume
|
V = A * Depth
|
|
mass =
|
m = pv
mass = density * volume |
|
change in depth (for pan method of evap)
evaporation? |
change in volume / AREa
evaporation is in change in depth / time |
|
LE flux from pan method
|
LE = (change depht / change T)*(latent heat of evaporation)
(Levap given) |
|
pan technique used for basin
|
E/A = (d1 - d2)*(fpan)
evap / basin area = (depth 1 - depth 2) * (pan coefficient) |
|
energy balance
to calculate ET |
LE = K + L + Aw - G - H - changeQ/changeT
latent heat flux = net radiation + water advected energy - heat loss due to ground - sensible heat loss to atms - heat loss from storage simplified: LE = R - H *replace H w/ bowen ratio* LE = R - LE(H/LE) LE + LE(H/LE) = R LE*(1+ H/LE) = R LE = R / (1+H/LE) |
|
"stream gauging"
|
measuring stream flow
(discharge) |
|
velocity of stream varies with
|
width and depth across stream
-fastest in middle - less friction |
|
measuring stream surface velocity
|
float method
time orange for 30m |
|
measuring stream discharge (accurate)
|
velocity area method
|
|
avg velocity of stream is
|
0.6x total depth from SURFACE
|
|
K
sat v unsat |
K constant in saturated
(depends on grain size) *hydraulic conductivity highest at least depth in saturated zone ... less compaction unsat K varies with moisture content **less moisture = more tension = h2o flows (is sucked) faster = greater hydraulic conductivity |
|
springs
|
when water table (sat zone) hits a dip in the topography
|
|
water flows from
(tension) |
low tension to high tension
|
|
field capacity
|
available water for plants
PWP < availh2o < FC |
|
artesian system
|
confined aquifer -- boundaries don't move -- pressure is released
|
|
cone of depression
|
occurs with unconfined aquifer
-- depression in h2o table --- results in velocity increasing with proximity to well |
|
three types of ET measurements
|
1. Pan Approach (DIRECT MEASURMENT)
2. Energy Balance Approach -- MEASURES LE ---eddy covariance ---aerodynamic profile --- bulk transfer ---bowen ratio 3. Water balance equation - solve for ET **most common **least precise |
|
best measurement of ET?
|
eddie covariance
-over large area -integrated (not just pt measurement) -measures in 3d -measures at high frequency -low margin of error -----disadvantage--- -a lot of interpreting after data collection |
|
laminar flow
|
viscous forces dictate the nature of the flow
--maj of groundwater flow since pore spaces small |
|
cone of depression equation
|
Vcone = Vpumped / Sy
Sy = specific yield |
|
pan evap -- for basin
|
E/A = (d1 - d2)fpan
|
|
measures hydraulic head for UNSAT
|
tensiometer
|
|
measures hydraulic head for SAT
|
piezometer
|
|
each parcel of air
has (eddy) |
1. trace gas concentration
2. temperature 3. humidity |
|
K independent of pressure
v K function of pressure |
SAT - K independent of pressure
UNSAT - K and moist.content function of pressure |
|
K at max
|
saturated
|
|
pressure head > 0
|
saturated
|
|
pressure < 0
|
unsaturated
|
|
PWP eq
|
PWP = porosity * [(air entry tension)/15000]^1/b
|
|
pt of saturation
(K compared to moisture content |
K no longer changing with changes in h2o content
|
|
hp
(pressure head component of hydraulic head) |
hp =
p / Yw p = water pressure Y(greek)w = WEIGHT DENSITY h2o |
|
"thruflow"
|
unsat zone
|
|
perched aquifer
|
--> SPRINGS
above impervious layer (perched h2o table and aquifer lay above main h2o table) |
|
greek u
|
dynamic viscosity
|
|
greek v
|
kinematic viscocity
greek u / p |
|
greek B
|
compressability
|
|
k
|
permeability
= K(greek u) / pg |
|
water level in unconfined aquifer
|
= water table
= hydraulic head (elevation + press head) |
|
wind etc - to measure EVAP
|
E = Ke * Va * (e.s - e.a)
Ke = turbulence factor Va = wind speeed e.s = vapor pressure at saturated surface of h2o e.a vapor pressure above water |
|
bulk transfer
measure evap |
E = 1.26 x 10^-6 Va (e.s - e.a)
Va = velocity of air (WIND SPEED) e.s = vap pres in saturated zone at water surface e.a = vap pres above surface ****PAREMETERS VARY GREATLY WITH TIME (don't do more than a day at a time) |
|
rate LE transfer
and fick's law |
LE = densityh2o * latent heat of vaporization * evaporation
---> put into fick's law E = Ke * Va * (e.s-e.a) ..... LE = (density water)(latent heat vaporization) (turbulence) (air velocity) (vap pres sat - vap pressure above) |
|
bowen ratio
|
H / LE
|
|
adv / disadv for whole energy balance equation
|
+ -- using bowen ratio elimates need for wind speed
--- need lake temp / inflow / outflow / volume |
|
i must equal
|
negative of the total infiltration over time
((-) flux means down!!!) i = - dI/dt = - change moisture content * dLf/dt (dLf = depth of wetting front) I = Lf*change moisture content ... infiltration = Ksat * [ (-presshead @ front * change moisture content)/Lf}] |
|
water table aquifer
|
unconfined aquifer
-- water table is binding surace on top --PUMPING WELL DROPS THE H2o table |
|
confined aquifer
|
artesian aquifer
confined by aquiclude (overlain by it...) water is UNDER PRESSURE piezometer measures water pressure in aquifer *pump w/o decreasing h2o table -- pressure forces water up well above h2o table |
|
name for unsat zone
|
vadose zone
*between surface and water table |
|
pore spaces partly full
|
vadose
|
|
"soil moisture"
|
water in vadose zone
-- goes to ET and to recharge ground |
|
capillary tension
|
h2o withdrawn, air enters pores
-air-h2o interface presenet h2o pulled up inside of tube due to NEGATIVE PRESSURE (pulled up from pressure head of 0-- like sponge in bowl h2o) "capillary pressure head" = applied neg pressure |