effects of boundary condition on shape of flow nets lecture 6 hydrology program, new mexico tech,...
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ERTH403/HYD503 Lecture 6
Hydrology Program, New Mexico Tech,
Prof. J. Wilson, Fall 2006 1
Effects of Boundary Condition
on Shape of Flow Nets
Seepage and Dams
Flow nets forseepage throughearthen dams
Seepage underconcrete dams
Uses boundaryconditions (L & R)
Requirescurvilinear squaregrids for solution
After Philip Bedient
Rice University
ERTH403/HYD503 Lecture 6
Hydrology Program, New Mexico Tech,
Prof. J. Wilson, Fall 2006 2
Flow Net in a Corner:
Streamlines !
are at right
angles to
equipotential
" lines
Flow to Pumping Center:
Contour map of the piezometric surface near Savannah, Georgia,1957, showing closed contours resulting from heavy localgroundwater pumping (after USGS !Water-Supply Paper 1611).
ERTH403/HYD503 Lecture 6
Hydrology Program, New Mexico Tech,
Prof. J. Wilson, Fall 2006 3
h = 92 m
Luthy Lake
h = 100 m
Peacock PondOrphanage
The deadly radionuclide jaronium was released
in Luthy Lake one year ago. Half-life = 365 daysConcentration in Luthy Lake was 100 µg/L.
If orphans receive jaronium over 50 µg/L, they
will poop their diapers constantly. How long
will it take for the contaminated water to get
to Peacock Pond and into the orphanage water
supply? Will jaronium be over the limit?
Example: Travel Time
Travel time
!
"ttotal = "ti1
4
# ="livi1
4
# =ni"liqi1
4
# = n"liqi1
4
#
!! ""
="="4
1
2
4
1
iitotall
hK
ntt
ii
i
i
ii
l
hK
l
hK
bw
!
!=
!
!==
h = 92 m
Luthy Lake
h = 100 m
Peacock Pond
Contamination in Kidnapper Bog
Travel time is only 129 years.
i
iii
l
wbhKQ!
!!=
,m/s10,m2,25.05!
=="= Khn
m900
m50
m100
m250
m500
4
3
2
1
=
=!
=!
=!
=!
totall
l
l
l
l
1
2
3
4
2l!
1l!
3l!
4l!
days! 131 time travel then,m/s106.3 ifBut 3=!=
"K
!
"ttotal simple =ltotal
vaverage=
nltotal
KJave arg e=
nltotal
K(4 #"h / ltotal )=
nltotal2
K(4 #"h)= 80days <<131days
Note: because of !l terms are squared,
accuracy in estimating !l is very important.
ERTH403/HYD503 Lecture 6
Hydrology Program, New Mexico Tech,
Prof. J. Wilson, Fall 2006 4
Two Layer Flow System with
Sand Below
Ku / Kl = 1 / 50
Two Layer Flow System with
Tight Silt Below
Flow nets for seepage from one side of a channel through two differentanisotropic two-layer systems. (a) Ku / Kl = 1/50. (b) Ku / Kl = 50. Source:
Todd & Bear, 1961.
ERTH403/HYD503 Lecture 6
Hydrology Program, New Mexico Tech,
Prof. J. Wilson, Fall 2006 5
SZ2005 Fig. 5.11
Flow nets in anisotropic media
Flownets in Anisotropic MediaExample:
Kx
Ky
Kx = 15Ky
ERTH403/HYD503 Lecture 6
Hydrology Program, New Mexico Tech,
Prof. J. Wilson, Fall 2006 6
Flownets in Anisotropic Media
Kx = 15Ky
Flownets in Anisotropic Media
Kx = 15Ky
ERTH403/HYD503 Lecture 6
Hydrology Program, New Mexico Tech,
Prof. J. Wilson, Fall 2006 7
Flow Nets: an example
• A dam is constructed on a permeablestratum underlain by an impermeablerock. A row of sheet pile is installed atthe upstream face. If the permeable soilhas a hydraulic conductivity of 150ft/day, determine the rate of flow orseepage under the dam.
After Philip Bedient
Rice University
Flow Nets: an examplePosition: A B C D E F G H I JDistance
from
front toe
(ft)
0 3 22 37.5 50 62.5 75 86 94 100
n 16.5 9 8 7 6 5 4 3 2 1.2
The flow net is drawn with: m = 5 head drops= 17
After Philip Bedient
Rice University
ERTH403/HYD503 Lecture 6
Hydrology Program, New Mexico Tech,
Prof. J. Wilson, Fall 2006 8
Flow Nets: the solution
• Solve for the flow per unit width:
q = m K
= (5)(150)(35/17)
= 1544 ft3/day per ft
total change in head, H
number of head drops
After Philip Bedient
Rice University
Flow Nets: An Example
There is an earthen dam 13 metersacross and 7.5 meters high.TheImpounded water is 6.2 meters deep,while the tailwater is 2.2 meters deep.The dam is 72 meters long. If thehydraulic conductivity is 6.1 x 10-4
centimeter per second, what is theseepage through the dam if the numberof head drops is = 21
K = 6.1 x 10-4cm/sec
= 0.527 m/day After Philip Bedient
Rice University
ERTH403/HYD503 Lecture 6
Hydrology Program, New Mexico Tech,
Prof. J. Wilson, Fall 2006 9
Flow Nets: the solution
From the flow net, the total head loss, H,is 6.2 -2.2 = 4.0 meters.
There are (m=) 6 flow channels and21 head drops along each flow path:
Q = (mKH/number of head drops) x damlength = (6 x 0.527 m/day x 4m / 21) x (dam
length)
= 0.60 m3/day per m of dam
= 43.4 m3/day for the entire 72-meter length of the dam
After Philip Bedient
Rice University
Aquifer Pumping Tests
Why do we need to know T and S (or K and Ss)?-To determine well placement and yield
-To predict future drawdowns
-To understand regional flow
-Numerical model input
-Contaminant transport
How can we find this information?-Flow net or other Darcy’s Law calculation
-Permeameter tests on core samples
-Tracer tests
-Inverse solutions of numerical models
-Aquifer pumping tests
ERTH403/HYD503 Lecture 6
Hydrology Program, New Mexico Tech,
Prof. J. Wilson, Fall 2006 10
Aquifer Equation, based on assumptions becomes an ODE for h(r) :
-steady flow in a homogeneous, isotropic aquifer
-fully penetrating pumping well & horizontal,
confined aquifer of uniform thickness, thus
essentially horizontal groundwater flow
-flow symmetry: radially symmetric flow
02=! h (Laplace’s
equation)
01
=!"
#$%
&
dr
dhr
dr
d
r
Steady Radial Flow Toward a Well
02
2
2
2
=!
!+
!
!
y
h
x
h (Laplace’s
equation
in x,y 2D)
(Laplace’s
equation in
radial
coordinates)
Boundary conditions
-2nd order ODE for h(r) , need two BC’s at two r’s, say r1 and r2
-Could be
-one Dirichlet BC and one Neuman, say at well radius, rw ,
if we know the pumping rate, Qw
-or two Dirichlet BCs, e.g., two observation wells.
Steady Radial Flow Toward a Well
ERTH403/HYD503 Lecture 6
Hydrology Program, New Mexico Tech,
Prof. J. Wilson, Fall 2006 11
We need to have a confining layer for our 1-D (radial) flow equation to
apply—if the aquifer were unconfined, the water table would slope down to
the well, and we would have flow in two dimensions.
b
h1h2
Q
Island with a confined aquifer in a lake
Multiply both sides by r dr
0=!"
#$%
&
dr
dhrd
Integrate1C
dr
dhr !=
01
=!"
#$%
&
dr
dhr
dr
d
r
Evaluate constant C1 using continuity.
The Qw pumped by the well must equal
the total Q along the circumference for every
radius r.
Steady Radial Flow Toward a Well
dhr
dr
T
Qw =!2
ODEConstant C
1:
Separate variables:
!
Qw = (2"r)Tdh
dr
rdh
dr=Qw
2"T= C
Integrate again:
!
Qw
2"T
dr
rr1
r2
# = dhh1
h2
#
!
Qw =Q(r) = KAdh
dr= K(2"r)b
dh
dr
= (2"r)Kbdh
dr=(2"r)T
dh
dr
ERTH403/HYD503 Lecture 6
Hydrology Program, New Mexico Tech,
Prof. J. Wilson, Fall 2006 12
b
h1h2
Q
r2 r1
Steady-State Pumping Tests
!
Qw
2"T
dr
rr1
r2
# = dhh1
h2
#
Integrate
( ) !!"
#$$%
&='
1
2
12ln
2
r
rhh
Q
T(
( )12
1
2
2
ln
hh
r
rQ
T!
""#
$%%&
'
=(
Thiem Equation
ERTH403/HYD503 Lecture 6
Hydrology Program, New Mexico Tech,
Prof. J. Wilson, Fall 2006 13
h
r
What is the physical rationale for
the shape of this curve (steep at
small r, flat at high r)?
Why is the equation logarithmic?
This came about during the switch to radial coordinates.
Steady-State Pumping Tests
(Driscoll, 1986)
As we approach the well the
rings get smaller. A is
smaller but Q is the
same, so must increase.dl
dh
Think of water as flowing
toward the well through a series
of rings.
ERTH403/HYD503 Lecture 6
Hydrology Program, New Mexico Tech,
Prof. J. Wilson, Fall 2006 14
The Thiem equation tells us there is a logarithmic relationship between
head and distance from the pumping well.
lch
r
rQ
T!
""#
$%%&
'
= 2
10ln
1
1
(
#hlc
one log cycle
(Schwartz and Zhang, 2003)
The Thiem equation tells us there is a logarithmic relationship between
head and distance from the pumping well.
lch
r
rQ
T!
""#
$%%&
'
= 2
10ln
1
1
(
( ) ( )xx log 3.2ln !
If T decreases, slope increases
lch
QT
!=
2
3.2
"
#hlc
one log cycle
(Schwartz and Zhang, 2003)
( ) 303.210ln !
ERTH403/HYD503 Lecture 6
Hydrology Program, New Mexico Tech,
Prof. J. Wilson, Fall 2006 15
Steady-State Pumping Tests
Can we determine S from a Thiem analysis?
No—head isn’t changing!