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02/12/1434
1
3 th
lect
ure
1
5-D
IME
NS
ION
ING
AN
DS
TAB
ILIT
YO
FW
EIR
:
02/12/1434
2
5-D
IME
NS
ION
ING
AN
DS
TAB
ILIT
YO
FW
EIR
:
Wei
ris
subj
ecte
dto
thre
egr
oups
offo
rces
1-D
eriv
ing
For
ces:
Due
tow
ater
thru
stan
daf
fect
sho
rizon
tal
lyon
the
wei
rwal
l
2-S
cour
:Due
tofa
lling
surg
eca
usin
gsc
our
ofth
ebe
dso
ilre
sulti
ngin
asc
our
hole
sat
the
dow
nst
ream
side
ofw
eirf
ound
atio
n.(S
cour
Leng
th).
3-S
eepa
ge:
Due
tope
rcol
atio
nof
wat
erin
the
unde
rlyin
gpe
rm
eabl
eso
ilbe
dca
usin
gbu
oyan
cyof
the
stru
ctur
ean
der
osio
nof
bed
soil
atdo
wn
stre
amsi
deof
foun
datio
n.(P
erco
latio
nLe
ngth
).
4
Flo
wn
et
A n
etw
ork
of s
elec
ted
stre
am li
nes
and
equi
pote
ntia
l lin
es.
SE
EP
AG
E T
HR
OU
GH
PE
RM
EA
BLE
MAT
ER
IAL
See
page
(Per
cola
tion)
Str
eam
line
is s
impl
y th
e pa
th o
f a w
ater
mol
ecul
es fr
om u
pstr
eam
to
dow
nstr
eam
, tot
al h
ead
stea
dily
dec
reas
es a
long
the
stre
am li
ne..
02/12/1434
3
5
Hyd
rau
lic
gra
die
nt
‘ i
‘ be
twee
n A
and
Bis
the
tota
l hea
d lo
ss p
er u
nit l
engt
h.
AB
BA l
TH
TH
i−
=
leng
th A
B, a
long
the
stre
am li
ne
Da
rcy
’s L
aw
Vel
ocity
(v)
of fl
ow i
s pr
opor
tiona
l
To th
e hy
drau
lic g
radi
ent (
i)
v =
ki
Per
mea
bilit
y
•or
hyd
raul
ic c
ondu
ctiv
ity
•un
it of
vel
ocity
(cm
/s)
Wha
t is
the
max
imum
H.G
. al
ong
all t
he s
truc
ture
life
?
6
For
curv
elin
ear
squa
res,
a=b
02/12/1434
4
7
Pip
ing
in
Gra
nu
lar
So
ils
At t
he d
owns
trea
m e
nd o
f fou
ndat
ion,
If i e
xitex
ceed
s th
e cr
itica
l hyd
raul
ic g
radi
ent (
i c),
first
ly th
e so
il gr
ains
at e
xit g
et w
ashe
d aw
ay. T
his
phen
omen
on p
rogr
esse
s to
war
ds
the
dow
nstr
eam
, for
min
g a
free
pas
sage
of w
ater
(“p
ipe”
).
lhi ex
it∆∆
=E
xit h
ydra
ulic
gr
adie
nt
datu
mW
EIR
impe
rvio
us s
trat
a
soil
h
∆h =
tota
l he
ad d
rop
∆l
exitc
pipi
ngii
F=
Typi
cally
5-
10
Fac
tor
of s
afet
y ag
ains
t pip
ing
no s
oil;
all
wat
er
unit
subm
erge
dic
'=
=γ
e1
1G
'
+−=
γ
8
i c>
i
PIP
ING
PH
EN
OM
EN
ON
WIL
L TA
KE
PLA
CE
ciLh
i=
=cih
L=
h 1
=
csa
fei
FL
So,
The
Cre
ep le
ngth
, “th
e sh
orte
st s
trea
m li
ne”,
mus
t not
less
than
L s
afe
to e
nsur
e sa
fety
aga
inst
pip
ing
at D
S o
f the
str
uctu
re fl
oor.
QU
ICK
SA
ND
CO
ND
ITIO
N,
σ v '
= 0
i=i c=
γ‘
σ v '
< 0
The
n,
02/12/1434
5
9
EM
PR
ICA
L D
IME
NS
ION
S:
mt
)7
5.0
5.0(1
−=
max
2)0.1
8.0(H
t−
=
mL
)0.50.3(
1−
=2/)
(5.0
dsw
BL
CL
L−
+=
max
6.0
HC
Lb
s=
AB
BA l
TH
TH
i−
=
10
A-
BL
IGH
’S T
heo
ry :
max
HC
Lb
B= B
ligh’
s co
ef. d
epen
ds o
n th
e so
il ty
pe
Max
. H
ead
diffe
renc
e =
WL
-
WL
us
d
s
CL
-
BL
Whi
ch is
big
ger
vH
act
LL
L
+
=
Per
cola
tio
n
Th
eory
Bli
gh
La
ne
02/12/1434
6
11
BLI
GH
TH
EO
RY:
�
Isus
edin
desi
gnin
gof
impe
rvio
usflo
orfo
rsu
bsu
rfac
eflo
w.
�It
isdi
rect
lyde
pend
ing
onth
epo
ssib
ilitie
sof
perc
olat
ion
inpo
rous
soil
onw
hich
the
floor
(apr
on)
isbu
ilt.
�W
ater
from
upst
ream
perc
olat
esan
dcr
eeps
(or
trav
el)
slow
lyth
roug
hw
eir
base
and
the
subs
oilb
elow
it.
�T
hehe
adlo
stby
the
cree
ping
wat
eris
prop
ortio
nal
toth
edi
stan
ceit
trav
els
(cre
eple
ngth
)al
ong
the
base
ofth
ew
eir
prof
ile.
�T
hecr
eep
leng
thm
ust
bem
ade
asbi
gas
poss
ible
soas
topr
even
tthe
pipi
ngac
tion.
�T
his
can
beac
hiev
edby
prov
idin
gde
epve
rtic
alcu
t-of
fsor
shee
tpile
s
12
Lim
itatio
ns o
f Blig
h's
theo
ry
1.T
his
theo
rym
ade
nodi
stin
ctio
nbe
twee
nho
rizon
tal
and
vert
ical
cree
p.
2.D
idno
tex
plai
nth
eid
eaof
exit
grad
ient
-sa
fety
aga
inst
unde
rmin
ing
cann
otsi
mpl
ybe
obta
ine
db
yco
nsid
erin
ga
flata
vera
gegr
adie
ntbu
tby
keep
ing
this
grad
ient
will
belo
wcr
itica
l.
3.N
odi
stin
ctio
nbe
twee
nou
ter
and
inne
rfa
ces
ofsh
eet
pile
sor
the
inte
rmed
iate
shee
tpile
s,w
here
asfr
omin
vest
igat
ion
itis
clea
r,tha
tth
eou
ter
face
sof
the
end
shee
tpile
sar
em
uch
mor
eef
fect
ive
than
inne
rone
s.
4.Lo
sses
ofhe
addo
esno
ttak
epl
ace
inth
esa
me
prop
ortio
nsas
the
cree
ple
ngth
.A
lso
the
uplif
tpr
essu
redi
strib
utio
nis
not
linea
rbu
tfo
llow
asi
necu
rve.
02/12/1434
7
13
)(
1
sw
HL
LL
L+
+=
)(
21
1t
yt
Lv
++
=2
2)
(t
BL
BL
dsus
+−
=
14
02/12/1434
8
15
)(
2
12
11
ss
ww
HL
LL
LL
L+
++
+=
)(
32
11
ty
yt
Lv
++
+=
32
)(
tB
LB
Lds
us+
−=
usB
L
dsB
L
16
max
HC
LL
L= La
ne’s
coe
f. D
epen
ds o
n th
e so
il ty
pe
Max
. H
ead
diffe
renc
e =
WL
-
WL
us
d
s
CL
-
BL
Whi
ch is
big
ger
vH
act
LL
L
31+
=
B-
LA
NE
’S
Th
eory
:
Lane
con
side
rs th
at th
e ve
rtic
al p
ortio
n of
cre
ep is
mor
e ef
fect
ive
in
resi
stin
g w
ater
flow
in th
e so
il th
an th
e ho
rizon
tal o
ne…
……
.WH
Y?
02/12/1434
9
17
In b
oth
case
s of
BLI
GH
or L
AN
E, t
he a
ctua
l len
gth,
Lac
t,s
houl
d no
t les
s
than
the
theo
retic
al c
reep
leng
th, L
Bor
LL
i-If
L
act=
LB
, the
per
cola
tion
is s
afe.
ii-If
L
act>
LB
, the
per
cola
tion
is m
ore
safe
., ca
lcul
ate
the
mod
ified
' b
C
max
'
HLC
act
b=
iii-
If
Lac
t<
LB
, the
per
cola
tion
is u
nsaf
e, in
crea
seth
e ac
tual
cre
ep le
ngth
DL
Lac
tB
+= If
D <
4m
, ext
ent f
loor
apr
on a
t DS
by D
If D
> 4
m, p
rovi
de s
heet
pile
s
-m
in. d
epth
of e
ach
row
is 2
.0m
and
the
No.
of r
ows
is d
efin
ed a
ccor
ding
to
D
-H
oriz
onta
l dis
tanc
e be
twee
n an
y tw
o ro
ws
not l
ess
than
sum
of i
ts d
epth
s
-S
ides
sho
uld
be c
lose
d
max
'
HLC
act
l=
' lC
18
iii-
If
Lac
t<
LL
, the
per
cola
tion
is u
nsaf
e, in
crea
seth
e ac
tual
cre
ep le
ngth
DL
Lac
tL
+= If
D <
(4/
3 )m
, ext
ent f
loor
apr
on a
t DS
by 3
D
If D
> (
4/3
)m, p
rovi
de s
heet
pile
s p
iles
( m
in. d
epth
of e
ach
row
is 2
.0m
and
the
No.
of r
ows
is d
efin
ed a
ccor
ding
to D
)
US
ING
LA
NE
’S T
HE
OR
Y
02/12/1434
10
19
20
Wha
t is
the
best
pos
ition
for
the
shee
t pile
s an
d w
hy?
02/12/1434
11
21
So
il t
yp
eB
lig
h’s
Co
eff
icie
nt
Cb
La
ne
’sC
oe
ffic
ien
t
CL
Cri
tica
l g
rad
ien
t
i cV
ery
fin
e
sa
nd
/sil
t18
8.5
0.12
Fin
e
s
an
d15
70.
14
Med
ium
san
d6
0.17
Co
arse
sa
nd
125
0.2
Fin
e
g
rav
el
40.
25
Med
ium
gra
ve
l3.
50.
29
Co
arse
gra
ve
l &
co
bb
les
30.
33
Bo
uld
ers
wit
h s
om
e co
bb
les
& g
rave
l5
-9
2.5
0.4
So
ftcl
ay
30.
33
Med
ium
cla
y2
0.5
Har
d
cla
y1.
80.
56
2
Lb
CC
≈
Per
cola
tio
n C
oef
fici
ents
:
22
Com
mon
cau
ses
of w
eir
failu
re in
clud
e:
•Exc
essi
ve a
nd p
rogr
essi
ve d
owns
trea
m e
rosi
on,
both
from
with
in th
e st
ream
and
thro
ugh
late
ral e
rosi
on o
f the
ban
ks.
•Ero
sion
of i
nade
quat
ely
prot
ecte
d ab
utm
ents
.
•Hyd
raul
ic r
emov
al o
f fin
es a
nd o
ther
sup
port
mat
eria
l fro
m
dow
nstr
eam
pro
tect
ion
(gab
ions
and
apr
ons)
res
ultin
g in
ero
sion
of
the
apro
n pr
otec
tion.
•Det
erio
ratio
n of
the
cut
off a
nd s
ubse
quen
t los
s of
con
tain
men
t
•Add
ition
al a
spec
ts s
peci
fic to
con
cret
e, r
ock-
fill o
r st
eel s
truc
ture
s.
02/12/1434
12
23
The
mai
n ca
uses
for
wei
r fa
ilure
incl
ude:
1. P
ipin
gP
ipin
g is
cau
sed
by g
roun
dwat
er s
eepi
ng o
ut o
f the
ban
k fa
ce.
Gra
ins
are
deta
ched
and
ent
rain
ed b
y th
e se
epag
e flo
w a
nd m
ay b
e tr
ansp
orte
d aw
ay f
rom
the
bank
face
by
surf
ace
runo
ff ge
nera
ted
by t
he s
eepa
ge,
if th
ere
is s
uffic
ient
vol
ume
of fl
ow.
2. R
uptu
re o
f flo
or d
ue to
upl
ift:
If th
e w
eigh
t of
the
floor
is in
suffi
cien
t to
resi
st th
e up
lift p
ress
ure,
the
flo
or m
ay b
urst
. Thi
s bu
rstin
g of
the
floor
red
uces
the
effe
ctiv
e le
ngth
of
the
impe
rvio
us fl
oor,
whi
ch w
ill r
esul
ting
incr
easi
ng e
xit
grad
ient
, and
can
cau
se f
ailu
re o
f th
e w
eir.
3. R
uptu
re o
f flo
or d
ue to
suc
tion
caus
ed b
y st
andi
ng w
aves
Hyd
raul
ic ju
mp
form
ed a
t the
dow
nstr
eam
of w
ater
.
24
PR
EC
AU
TIO
NS
AG
AIN
ST
PE
RC
OL
AT
ION
:
1-P
rovi
de
con
cret
e A
PR
ON
eit
her
at
the
US
or
at
the
DS
2-P
rovi
de
cut-
off
wal
ls
3-P
rovi
de
end
cu
t-o
ff
5-P
rovi
de
reve
rsed
filt
er
4-P
rovi
de
con
cret
e b
lock
s
6-P
rovi
de
dra
inag
e p
ipes
7-P
rovi
de
end
sill
8-P
rovi
de
dry
pit
chin
g a
t D
. S.
9-P
rovi
de
pit
chin
g in
mo
rtar
at
U. S
.
02/12/1434
13
25
UP
ST
RE
AM
PR
EC
AU
TIO
N
26
DO
WN
ST
RE
AM
PR
EC
AU
TIO
N
02/12/1434
14
27
bCt 1
bCy
bC1
bCt 2
b
sw C
LL
+
1
sL
wL
1L
Tota
l upl
ift
23 4
56
1’
2’3’
4’
5’ 6’
bCL 1
UP
LIF
T D
IAG
RA
M O
F P
LA
NE
FL
OO
R :
Po
int
Ele
va
tio
nP
oin
tE
lev
ati
on
5’4
’-(L
w+
Ls)
/cb
6’
5’-t
2/cb
=D
S
1’U
S2’
1’-t
1/cb
3’2’
-L1/
cb4
’3’
-y/c
b
Usi
ng B
ligh’
s M
etho
d
28
lCt 1
lCy
lC31
lCt 2
l
sw
C
LL
3+
1
sL
wL
1L
Tota
l upl
ift
23 4
56
1’
2’3’
4’
5’ 6’
lCL 3
1
UP
LIF
T D
IAG
RA
M O
F P
LA
NE
FL
OO
R :
Po
int
Ele
va
tio
nP
oin
tE
lev
ati
on
5’4
’-(L
w+
Ls)
/3cl
6’
5’-t
2/cl
=D
S
1’U
S2’
1’-t
1/cl
3’2’
-L1/
3cl
4’
3’-y
/cl
Usi
ng L
ane’
s M
etho
d
02/12/1434
15
29
bCt 1
bCy 1
bC1
bCt 2
b
sw
C
LL
11
+
b
sw
C
LL
22
+
bCt 3
bC1
bCy
2
3030
UP
LIF
T D
IAG
RA
M O
F F
LO
OR
WIT
H S
HE
ET
PIL
ES
:
Usi
ng
Blig
h’s
Met
ho
d
bCt 1
bCy
bCt 2
bC1
Tota
l upl
ift
sL
wL
bCd 12
02/12/1434
16
31
32
STA
BIL
ITY
OF
FL
OO
R :
Th
e fl
oo
r m
ust
be
stab
le b
y g
ravi
ty.
i.e. T
he
wei
gh
t o
f th
e fl
oo
r at
an
y se
ctio
n
mu
st b
e g
reat
er t
han
th
e u
pw
ard
bu
oya
ncy
fo
rce
“up
lift”
02/12/1434
17
33
1t
Diff
eren
tial u
plift
1h′
1h Tota
l
uplif
t
d
Co
nsi
der
sec
tio
n 1
-1,
Th
e u
pw
ard
lift
ing
fo
rce
is
Th
e d
ow
nw
ard
gra
vity
forc
e is
()
()1
11
ht
hw
w′
+=
=γ γγγ
γ γγγ
dt
wm
γ γγγγ γγγ
+=
1
So
, th
e u
pw
ard
forc
e <
do
wn
war
d fo
rce Ta
ke t1
as m
in. (
0.5
0 -
0.75
m)
()
dt
ht
wm
wγ γγγ
γ γγγγ γγγ
+<
′+
11
1
34
2t
Diff
eren
tial u
plift
2h′
2h
Tota
l
uplif
t
Co
nsi
der
sec
tio
n 2
-2,
Th
e u
pw
ard
lift
ing
fo
rce
is
Th
e d
ow
nw
ard
gra
vity
forc
e is
()
()2
22
ht
hw
w′
+=
=γ γγγ
γ γγγ
()2t
mγ γγγ=
As
crit
ical
; (
)2
22
th
tm
wγ γγγ
γ γγγ=
′+
()
()
wm
wt
hγ γγγ
γ γγγγ γγγ
−=
′2
2
()
()
()1
22
2−′
=−
′=
mw
mwh
ht
γ γγγγ γγγ
γ γγγγ γγγ
As
a fa
cto
r o
f sa
fety
incr
ease
the
wei
gh
t of
flo
or
by
20 –
30 %
()
21
1
22
.*
−′=
mht
γ γγγ
02/12/1434
18
35
bCt 1
bCy
bC1
bCt 2
b
sw C
LL
+
1
sL
wL
1L
Diff
eren
tial u
plift
. h’
23 4
56
1’
2’3’
4’
5’ 6’
bCL 1
Tota
l upl
ift ()
2.1*
12
2−′
=mh
tγ
' 2h m 0.
75 -
50.0(m
in)
1=
t