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田富强
2012.09.19《高等水文学》第三讲水文过程及其观测
Hydrological
Processes
&Its
Observation2.1全球水文循环全球水文循环主要特征Coupling
and
feedbacks:
Ocean‐atmosphere‐landinteraction
—
single
coupled
earth
systemPrincipal
players:
Hadley
circulation,
thermohalinecirculations,terrestrialvegetationdistributionandsoilmoisture,snow/ice
albedoOscillations
and
variability:
decadal,
inter-annual,
intra-annual,
seasonal,sub-seasonal,dailyCharacteristics
at
different
space
and
time
scales:
largescales
feed
the
small
scale,
and
small
scales
feed
thelargescalesGlobal
water
cycle:
moisture
movement
in
all
its
phases
asadriver
andresponseoftheaboveelements大气:Hadley
CirculationThe
Hadley
cell
carries
heat
and
moisture
from
thetropics
to
the
northern
and
southern
mid-latitudes.Hadley
cellThe
Hadley
cell,
named
after
GeorgeHadley,
is
a
circulation
pattern
thatdominates
the
tropical
atmosphere,
withrising
motion
near
the
equator,
polewardflow
10–15
kilometers
above
the
surface,descending
motion
in
the
subtropics,
andequatorward
flow
near
the
surface.
Thiscirculation
is
intimately
related
to
thetrade
winds,
tropical
rainbelts,
subtropicaldeserts
and
the
jet
streams.海洋:Thermohaline
CirculationThis
collection
of
currents
is
responsible
for
the
large-scaleexchangeofwatermasses
intheocean,includingprovidingoxygentothedeep
ocean.Theentirecirculation
patterntakes~2000
yearsThermohaline
CirculationThe
term
thermohaline
circulation
(THC)
refers
toa
part
of
the
large-scale
ocean
circulation
that
isdriven
by
global
density
gradients
created
bysurface
heat
and
freshwater
fluxes.
The
adjectivethermohaline
derives
from
thermo-
referring
totemperature
and
-haline
referring
to
salt
content,factors
which
together
determine
the
density
ofsea
water.
Wind-driven
surface
currents
(such
asthe
Gulf
Stream)
head
polewards
from
theequatorial
Atlantic
Ocean,
cooling
all
the
whileand
eventually
sinking
at
high
latitudes
(formingNorth
Atlantic
Deep
Water).
This
dense
water
thenflows
into
the
ocean
basins.多
要
素
的
耦
合El
Niño/La
Niña-Southern
Oscillation,
or
ENSO,
is
aquasi-periodic
climate
pattern
that
occurs
across
thetropical
Pacific
Ocean
on
average
every
five
years,
butover
a
period
which
varies
from
three
to
seven
years.
It
ischaracterized
by
variations
in
the
temperature
of
thesurface
of
the
tropical
eastern
Pacific
Ocean
-
warming
orcooling
known
as
El
Niño
and
La
Niña
respectively-
andair
surface
pressure
in
the
tropical
western
Pacific
-
theSouthern
Oscillation.
The
two
variations
are
coupled:
thewarm
oceanic
phase,
El
Niño,
panies
high
air
surfacepressure
in
the
west
Pacific,
while
the
cold
phase,
La
Niña,panies
low
air
surface
pressurein
the
west
Pacific.Mechanisms
that
cause
the
oscillation
remain
understudy变异性年际尺度为例泰国洪水(2011.10)变异性气候变暖的影响耦合与反馈Feedback蓝圈:正反馈红圈:负反馈实线:增强
虚线:减弱Stomatalresistance2.2流域和山坡水文过程流域水文过程山坡水文过程Figure
fromSidle
et
al.,
2001
HP实际山坡照片Maimai试验流域(新西兰,2009年,1570mm/y)密云水库流域(2012.07.20,
492mm/y)巴音布鲁克草原(2012.09.17,
276mm/y)2.3主要水文过程计算及观测主要水文过程蒸发蒸腾地下水运动土壤水运动降水入渗蒸散水文过程地表径流汇流水文过程-降水降水是水分从 大气输送到地 球表面的主要 途径。降水通常包括 降雨、雪、冰 雹、雨加雪等 形式。TRMM
(The
Tropical
RainfallMeasuring
Mission
) Precipitation
Radar
(PR):
designed
toprovide
three-dimensional
maps
of
stormstructure.TRMM
Microwave
Imager
(TMI):
passivemicrowave
sensor
designed
to
providequantitative
rainfall
information
over
awide
swath
under
the
TRMM
satellite. Visible
and
Infrared
Scanner
(VIRS):
oneof
the
three
instruments
in
the
rain-measuring
package
and
serves
as
a
veryindirect
indicator
of
rainfall. Clouds
and
the
Earth's
Radiant
EnergySystem
(CERES): measures
the
energy
atthe
top
of
the
atmosphere,
as
well
asestimates
energy
levels
within
theatmosphere
and
at
the
Earth's
surface. Lightning
Imaging
Sensor
(LIS):
detectsand
locates
lightning
over
the
tropicalregion
of
the
globe.水文过程-植被截留植被截留是林冠在短时间内截持并 释放出雨水的现象。植被的截留类似于土壤的渗透现象,降雨进入林冠后产生初始截留强度,林冠饱和后,仍有一定截留能力-稳定截留强度,可用Horton入渗理论描述:水文过程-蒸发水分通过蒸发从地表向大气输送,在 此过程中水分由液态变为气态。约有80%的蒸发来自于海洋,20%来 自于内陆水体和植被。发生在土壤表 面的蒸发称为土面蒸发,发生在植物 叶面的称为植物蒸腾。风将水汽输送至全球,并影响着世界 各地的空气湿度。水面蒸发水
面
蒸
发水文过程-蒸发土壤辐射、气温、湿度和风速等气象因素土壤中含水率大小和分布E大气蒸发能力E0土壤供水能力土
面
蒸
发土面蒸发表土蒸发强度保持稳定的阶段:表土蒸发强度随含水率变化的阶段:水汽扩散阶段:田间腾发量的估算1.
理论方法紊流扩散法能量平衡法Bowen比风速 水汽压田间腾发量的估算综合法(Penman公式)干燥力田间腾发量的估算-经验方法,空气湿度:如,,水面蒸发:利用单一气象因素估算腾发量:太阳辐射:太阳辐射气温:如平均气温积温水汽压空气饱和差水面蒸发强度田间腾发量的估算-经验方法与多个气象因素复相关的经验公式:如Dalton空气动力学类型的公式,一般形式为:其中f(u)为某一适宜高度处风速u的经验函数Christiansen与Hargreaves(1969)公式:以太阳总辐射为指标,综合考虑了气温、风速、相对湿度、日照百分数和高程等因素的的影响。蒸发器直径=61.8
cm水圈直径=161.8
cm一般每日8时观测一次,则得到逐日蒸发的水深(mm)。蒸发皿蒸发量的折算问题E
w
'
q
'涡度相关法(Eddycorrelation
method)蒸发量可以通过测量垂直方向上风速的脉动量和水汽浓度的脉动量,并计算一定时间长度内两个脉动量的互相关得到。尽管这种方法在理论上很严密,但实际观测对仪器的要求非常严格。例如,当在距离地表几米处测量时,响应幅频应至少达到5~10Hz,即每秒测量5~10次。直到1990年代才实现仪器的商业使用,但仪器仍然非常昂贵而且使用要求很高,目前还仅限于在实验观测。清华大学位山生态水文试验基地水文过程-地表水运动1. 一维洪水运动波-圣维南(St.Venant)方程组A-过水断面面积;Q-流量;y-水深;i0-河底比降if-摩擦比降V-断面平均流速水文过程-地表水运动平面二维非恒定流动的基本方程:连续方程:动量守恒方程:x方向:y方向:水文过程-入渗水文过程-入渗降雨的入渗过 程可分为两个 阶段供水控制(通 量控制)阶段土壤入渗能力 控制(剖面控 制)阶段水文过程-入渗边界的简化入渗边界有三种简化模型:地表含水率已知——灌溉模型地表通量已知——降水模型地表积水——积水模型水文过程-入渗对于均质土壤,初始含水率分布均匀时, 可用解析或半解析的方法求解前二种情况 下的土壤水分运动方程。对于初始含水率不均匀,或土壤非均质, 或地下水埋藏较浅以及实际问题必须按较 复杂的二维或三维问题处理时,目前还只 能用数值解法。用解析方法求解时,主要困难在于该微分 方程的非线性,在求解时一般采用线性化 方法将其近似为线性偏微分方程。常用入渗公式4.
Holtan公式:饱和含水率Green-Ampt公式:稳渗率Philip公式:吸渗率 稳渗率Horton公式:稳渗率土壤初始入渗率容许储水量Green-Ampt模型Green-Ampt模型又 称活塞模型,模型 研究的是初始干燥 的土壤在薄层积水 时的入渗问题。基本假定:入渗时 存在明确的水平湿 润锋面,将湿润和 未湿润的区域截然 分开。Green-Ampt模型1.
由达西定律可求得地表处入渗率:2.
由水量平衡原理求得入渗量联立以上两式,并代入边界条件,可求3.
由得:水文过程-土壤水运动非饱和土壤水流动的达西定律:通量 水力传导度 土水势非饱和土壤水流动与饱和土壤水流动的区别:非饱和饱和土水势主要考虑重力势和基质势主要考虑重力势和压力势导水率是含水率的函数饱和导水率非饱和土壤水运动的基本方程质量守恒运动方程连续方程达西定律非饱和土壤水运动的基本
方程或
z
y
z
t
x
x
y
zx
y
K
K
K
水文过程-地下水运动渗流基本定律-达西定律适用范围:Re不超过1~10;水力坡度大于起始水力坡度J0;多数情况下粗砂中的地下水运动是符合达西定律的。非线性运动方程(Re>1~10)常用的是P.Forchheimer公式:或水文过程-地下水运动1.
渗流的连续性方程:2.
假设地下水为不可压缩液体,密度为常数,含水层骨架不可压缩,则方程可简化为:水文过程-流域汇流坡面汇流与河网汇流各有不同特点:流态不同;蒸发和下渗的影响不同;汇流速度不同;调蓄作用大小不同;坦化程度强弱;非线性程度的差别。汇流分析模型:分散型模型:对坡面流采用流速公式代替动力方程的运动波模型,以Woolhiser-Ligget的无因次化方法为代表(1967)集总式模型:用水文学方法以蓄泄关系代替动力方程,以
Horton-Izzard法等为代表(1938~1944)水文过程-流域汇流常用流域汇流计算方法:单位线法;瞬时单位线法;综合单位线法;等流时线法;单元汇流法;河道汇流常用马斯京根法。2.4地表产流机制:超渗产流和蓄满产流Infiltration
Excess
Runoff
(Hortonian
Runoff)Saturation
Excess
Runoff
(Dunne
Runoff)Hortonian
overland
flowRobert
Elmer
Horton
(1933)
at
the
age
of
58
laidthe
foundation
of
what
is
now
called
the“Hortonian
overland
flow”Soil
acts
like
a
sieve
separating
rainfall
into “infiltration”
and
“runoff”
or
“overland flow”He
believed
that
excess
of
rainfall
intensity
overinfiltration
capacity
is
the
only
source
of
runoffquick
enough
to
produce
streamflow
hydrographpeak
and
all
infiltration
posses
into
groundwaterand
constitute
the
sole
source
of
baseflow.This
idea
fitted
very
well
with
Sherman’s
(1932)“unit
hydrograph”
theory
of
basin
runoff.Horton’s
overland
flow
from
rainfall
excess
eEssential
elements
ofHorton’soverland
flow
theoryRainfall
in
excess
of
infiltration
capacity e
runoffInfiltration
capacity
decreases
with
rainfall
due
to
change
insurface
moisture,
rain-drop
packing
of
surface
particles,entrapment
of
air,
closing
of
sun
cracks,
swelling
and
washing
offine
particles.Overland
flow
will
occur
more-or-less
simultaneously
over
theentire
watershed
if
rainfall
intensity
is
greater
than
lower
limitinginfiltration
capacity
(assume
uniform
over
the
watershed)The
hydraulic
of
the
overland
flow
plays
an
important
role
inerosion.
At
some
distance
downslope
of
the
watershed
divide,
thedepth
of
the
sheet
of
overland
flow
is
sufficient
to
generate
a
shearstress
competent
to
entrain
the
surface
soil
particles.
Erosionoccurs
firstly
in
the
form
of
rills
which
can
subsequently
coalesceto
form
new
stream
channels.c
0
cwherefc
is
final
infiltration
rate,f0
is
initial
infiltration
ratef)e
kt
f
(
f
fHorton’s
Infiltration
EquationConsequence
of
the
above
theorySoil
surface
provides
a
sharp
division
of
bothhydrologic
and
geomorphic
processes,
withinfiltrating
water
contributing
only
to
longer-termsoil-
and
ground-water
recharge
and
to
baseflow,and
being
irrelevant
both
as
far
as
the
stormhydrograph
peak
and
surface
erosion
areconcerned.Notice
that
although
the
unit
hydrograph
andHorton
overland
flow
models
tied
in
extremelywell
together,
they
are
fundamentally
different.The
unit
hydrograph
a
“Black
box”
modelwhere
as
Horton’s
theory
is
based
oninvestigation
of
physical
processes
and
theirinter-relationships.Problem
with this
theoryKirkby
(1969):
Hortonian
overland
flow
willoccurinstantaneously
over
a
basin
only
if
it
is
small
and
hashomogeneous
soil,
soil
moisture,
interception,
anddepression
storage
and
infiltration
condition.Some
surface
runoff
can
exist
for
a
time
as
subsurfaceflow
which
has
been
returned
to
thesurfaceKirkby
&
Charley
(1967):
where
there
isappreciablesoil
and
vegetation,
especially
where
there
is
humus
orlitter
covers,little
overland
flow
may
be
expected
tooccur
over
much
of
the
drainage
basin,
except
in
mostextreme
storms.Many
storms
may
be
expected
to
produce
overlandflow
from
limited
contribution
area
at
much
lowerrainfallintensities
than
are
required
to
exceed
theinfiltration
capacities
over
the
whole
basin
and
so
toproduce
universal
Hortonian
overland
flow
theselimited
areas
area:Zone
at
the
slope
base,
immediate
marginal
to
stream
channelswhere,
despite
the
usually
thicker
soil,
lateral
soil
drainagecommonly
produces
high
antecedent
moisture
conditions
in
theupper
layers.
The
extent
of
such
contributing
areas
is
initiallycontrolled
by
the
soil
characteristics
and
antecedent
moistureconditions,
but
as
the
storm
continues
the
zone
of
saturation
mayextend
upslope
to
an
extent
determined
by
the
temporal
pattern
ofstorm
intensity
and
the
characteristics
of
the
slope
soil
profile,including
hydraulic
efficiency
and
available
soil-moisture
storage.Concavities
or
topographic
hollow
where
surface
flowlinesconverge.
Stream-head
hollows
are
for
this
reason
especiallysusceptible
to
surface
runoff.Areas
of
thin
soil
coverSaturation
overland
flowThe
above
have
lead
to
the
concept
ofsaturation
overland
flow
which
occurswhere
the
soil
is
saturated
(partly
bylateral
flow
in
the
soil)
even
though
thelocal
infiltration
capacity
has
not
beenexceed
by
the
rainfall
intensities.
Suchoverland
flow
is
non-Hortonian.Saturation
overland
flow
may,
undercertain
circumstance
of
rainfall
intensityand
contribute
areas,
dominate
the
stormrunoff
of
catchment.Variable
Source
AreaKirkby,
1978.
Hillslope
Hydrology产流机制的统一性分析各种径流成分(超渗地面径流、饱和地面径流、地下径流、壤中水径流)的产流机制可知,任何一种径流成分都是在两种不同透水性物质的界面上产生的,而且上层介质的透水性必须好于下层介质的透水性。从这个意义上说,任何径流量都是由“超渗”作用形成的。对任一界面以上的微分厚度土层均可写出下列形式的水量平衡方程式:芮孝芳,2004.水文学原理I
E
We
W0
F
R产流机制的统一性I
—通过界面以上介质到达界面的供水量,当界面为地面时为降水E
—通过界面的蒸散发量F
—通过界面进入下层介质的入渗量(We-W0)—界面以上介质含水量在时段内的变化,当界面为地面时,该项为0R
——积聚在界面上的自由重力水芮孝芳,2004.水文学原理主导产流类型的影响因素Dunne,
1978.
in
Hillslope
Hydrology,
edit
by
KirkbyDunne论
产
流组合产流的类型和基本产流模式sint1.R
型
超渗地面径流型(2.
Rs
Rint)型
超渗地面径流和壤中水径流组合型(3.
Rsat
Rint)型
饱和地面径流和壤中水径流组合型(4.
Rs
R
g
)型
超渗地面径流和地下水径流组合型5.(
Rint
+R
g
)型
壤中水径流和地下水径流组合型6.R
型
壤中水径流型g7.(Rs
Rint+R
g
)型
超渗地面径流、壤中水径流和地下水径流组合型(8.
Rsat
Rint
+R
g
)型
饱和地面径流、壤中水径流和地下水径流组合型9.R
型
地下水径流型来源:芮孝芳,2004,
水文学原理,P1522.5多源观测数据RadarGaugeLABZMultiple
Sources
for
Rainfall
ObservationsGeosynchronous
SatellitesVIS,
IR,
SoundingPolarOrbiting
SatellitesMV,
and
Space
RadarPrecipitation
is
among
the
single
most
important
hydro-meteo-climatic
variable;Precipitation
measurement
is
one
of
the
KEY
hydrologic
challenges, particularly
in
high
latitude,
ocean,
or
remoteregions.How
to
obtain
Precipitation
Information,
Globally?“Satellite
Remote
Sensing
is
not
an
Option
but
the
only
option
to
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