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I log T- /0
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4.
4
TABLE V SF 85 (6Preconsolidation Pressure Mechanisms (For Horizontal Deposits with eostatic Stresses)
43 ",chonical"
a) C/I) Oeriurden
2) rior s/ica3) Gcia~ioi
aa-= .- A
4) WoMc -EZ ( Qod/$, /978 9,d)
OT't Adr nwveiJ /.341 A/s tla &d-f
D=
0.92= =
...OOO==<--ooo ~o
;. .a
Vru Z1r
Stress In situCategory Description History Stress Remarks / References
Profile Condition
A) Mechanical 1) Changes in total vertical Uniform Ko, but value Most obvious and easiestOne Dimensional stress (overburden, with at given OCR to identify
glaciers, etc.) constant varies for
2) Changes in pore pressure ( axe rload vs.(water table, seepage withconditions, etc.) seepage)
B) Desiccation 1) Drying due to evaporation Often Can deviate Drying crusts found atvegetation, etc. highly from Ko, e.g. surface of mostland depo-
erratic isotropic sitsi can be'at depth2) Drying due to freeing capillary within deltaic deposits
stresses
C) Drained Creep 1) Long term Uniform Ko, but not Leonards and Altschaeffl(Aging) secondary compression with necessarily (1964); Bjerrum (1967)
constant normallya / Ovo consolidated
value
D) Physico-Chemi 1) Natural cementation due Poorly understood andcal to carbonates, silica, often difficult to prove.
etc. Not No Very pronounced in eastern
2) Other causes of bonding Uniform Information greyCanad (1972), ayBi, errgum (1973San-due to ion exchange,thixotropy, "weathering"Quigley (1980)etc.
Consnf···/~~~~~~~-- _
kfu
CCL 33'8 7 /3222b7 2/?9 J
4
2cxlh Cy) #O/fom)
,-
16--- 7 i il 9t->/°oj
/ /r-/0 (WI 9g4 cuui)
IS~d~i
roAitc, .
To ko)j rTu,') Ongtok
1 4 5/rscQ/on (Sryenisc#r )
) Evct ora/ t - v c/e t , edA.
t'*C>t?+C42 (XDP @L) tjnr cvcoy YaX
2) /Frost
0 t0 C - K &t A J o- sCvdu 5M
Ko or t
C,-.-Tl ~ ~ 0
f(~en W I '- .-r ObservTc dt/Acu; f/oodIp/47,
T Tdad knd O /a dce/oo, (h,D/cr)
6/ UIL. ,,.w nr 7. P v .
Se 0/(vz y (/m 4) p54
I.
I
7..
1Iv
t,' I
Ik
4re
b) Ahriqs/On - -
Pump /ng
A-di Lr
I f fI _ · · · __··_ I --1 r// -v Pc ?4~4Z
+1 f
b) 6 i a Ovu dda Q I
/) Wq r 7-c 4 /
-T,
3
" ,. . .. -,s ---
Limit of ice
LEGEND
ShellGyttja
PeatWood
80o 75o
Extent of the "classical" Wisconsin glaciation of North America
70o 65o 60o 55o
40o
U.S.A Advance
?
?Lake Erie
Lake Ontario
Canada
10,85010,63010,70010,55010,200
Y - 215Y - 216L - 604 AL - 604 BL - 604 D
9,450I(GSC)-3
9,5705-100
10,870GCS-90
Nicolet
Drummondville
Champlain Sea
Quebec
Bersimis
North BayLake
Huron
11,950I(GSC)-2911,570
Y-691
Ottawa
10,600L-604C
11,370Y-233
12,100L-678
14,250W-735
13,800L-598A
&
11,950W-947
13,325I(GSC)-7
12,720GSC-102
12,940GSC-B9
11,950GSC-75
12,410GSC-101
Gulf of St. Lawrence
St. Lawrence River
12,080W-883
13,280Y-502
14,240Y-950/51 Boston
Atlantic Ocean
12,100 date, yrs. B.P.L-678
80o 75o 50o55o60o65o70o
45o
50o
50o
45o
40o
Figure by MIT OCW.
Figure by MIT OCW.
-600
Time, Years before Present
Boston, Sea-level and Post-Glacial Crustal Movements
02,0004,0006,0008,00010,00012,00014,00016,000
-160
-120
-80
-40
met
ers
40
1.7 ft.2.3ft.18ft.29ft.
55 ft.min.95 ft.min.
27 ft.min.23 ft.min.
5 ft.min.
ca. 30ft.?
?
Movement of a pointlocated today at sea level
Sea-level curve from Fig1
-400
-200
Pres
ent-d
ay E
leva
tion
(fee
t)
0
200
5o
Germany
Poland
Baltic Sea
Sweden
OsloNorway
Skagerak
North Sea
Extent of the Weichsel Glaciation of Europe
Scotland
England
Denmark
Finland
0o5o 10o 15o 20o
50o
25o
55o
60o60o
55o
50o
25o20o15o10o5o0o5o
Lim it of ice advance
Figure by MIT OCW.
/,322 /-D %F(
4 7 /o , I
4.r ar4linec/Crc (Sc.GCo6r. qr)
*4 Alo t: 5 oi' r, c t 4tIe p J O i.iLK ,O PAysleche
-- ITp
c/<Ice ao45sNA, cyc/es
2
3
CR o (/:V6)
oce
/.23/Of ~VC
C Mes ri e C4so (J66 3/81)
C, 1r Olt -A tR / /v)
. t,4 7/'
. /6-,./,
C/ ICR
OC(/) m m-EC /-f > /-cNf: or5^%rcufJ'3 6><V/SCLSS/o,
')$ Dop' h-i m FOR Pa &AoLof d4t rPra
2) Tyto r 3q /a Bjerum (O72) /nc4 aW w,^ 9 Ip
Pc
COx
PLASTICITY INDEX, PI(%) rp
Fig. 39 Precompression of late glacialand post glacial clays attributedto aging.
Why , ffkp1a S"IlutCCLr,4, IC4j) ?
404.Ja;e A- t, < /4.R"w-1G i sw or mj Sf 'l
3) Wudc YGt 47r;;
0 Yetl " AICr A4 oi- IPWatclj62 y " A C , f t t;
? s , $,. ,,
(CL 3'/37
M"
mmoI -11-"c
1-1
z"1-14 1/3o
- I I61
sOcP·et i( Ip)
-1 .
Par- Ir I :
8? /.322 _
2/fPAscc7 -ec/
PX Y.5 / C - C1 encrll a (3ec Table v,o4)
i) /2J/sYSS/o1 ( C7,O on r O cui'as of "o'ndn )
"Ce.,0, ; tc*0 ,~l,4L .' / "a-F m a ~p ~A4 t ' /f7.
,i, <- ~ h~, · e,g,4 Ahc .a2) 4aggep- JIs rdy -6 (p8)
Sh, c av /z h r $yn4/ ta ?o
I-D07Tt$V > d"Op
f/r x a Ift s 'O a c ;
· b~roo acdr da& clab 16 0 o 2 O/m vu.e*0O,- oo o41So B4'77 /6 O 200 ' .a * G 0* 80 a a c , M v o v.Ic *, L
,alS c +-eh~c~, ("3//is.j) cnd A dhirvcy C/4ancg sw -z + At' d 4 ko on3 cie t~tr - L
-;Cc~d: i/( tt 4 5?dA27 (W 4p#
- G~VLC~c nC °/, CGG C03^lU~M/78/JrA'4ogr9 (D9a) aL8 frl,&/4)
-C-
.mi,Xr
r-
71 2
V I 7 ff l -/, P, L 71
Z, 0
I
I J.5 cyj-/, 4 Vt.
20
Dep
th, z
(m)
18
16
14
1210
86
42
0
Crust
Marine Clay
LacustrineClay
Till
0 1 2 30Profile
Indices10 20 30 IP
IP(%) CKoU
'σvo
IL
IL
100Stress History (kPa)
200
Selected profile
σp on Blocksamples'
300
Frost}
Test Locations
Symbol Sample
James Bay B-5Marine:Block
AGS CHMArine:Tube
9
42
2.8
0.6
95
85
Ip(%) IL σvo'
1026
24
20Verti
cal S
train
, εv(
%)
Log Scale σvc (kPa)'
16
12
8
4
0
20 40
CasagrandeConstruction
Min. Max.
Min. Radius
Probableσvo'σp'
σp'
100 200 400 1000
σp'
a
b
B-6
0
20
16
12
8
4
0
100 200Consolidation Stress, σvc (kPa)
Verti
cal S
train
, εv
(%)
Compression curves for clays having different preconsolidation pressure mechanisms(a) Semi-Log scale; (b) Natural scale.
'300 400 500 600 700 800
James Bay: CementationAGS CH: Mechanical and/or desiccation
Note:Most likely mechanism causing σp > σvo' 'B-6
Laboratory σvc
q/σp
In situ σp
'
'
q/σp'
p'/σp
φ'= 35o
'
σvo/σp' '
σp'
'
0
0
0
0.1
0.2
0.3
0.4
0.5
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0
0
0.1
0.2
0.3
0.4
0.5
a) Normalized Stress-Strain Data from CKoUC Tests
b) Normalized Effective Stress Paths and Yield Envelopes
1 2 3Axial Strain, εa(%)
4 5 6 7 8
0.34
1.33
Destructured
Intact
0.80
Intactyield envelope
Destructured yield envelope
TC ESP atin situ OCR
Kc = 0.36Large Strain TCat in situ OCR
(a) Normalized Stress-Strain, (b) Effective Stress Paths and Approximate Yield Envelopes from CKoU Tests on James Bay B-6 Marine Clay.
σvo = 60 kpa, ' σp = 145 - 150 kPa'
At z = 6.3mIp = 16%, IL = 1.3
At in situ OCR:
Normally Consolidated: TC and TE (Destructured)
Triaxial Compression (TC)Triaxial Extension (TE)
' ' 'Lab σvc in situ σp: Peak qp(TC)/σp<
Figures by MIT OCW.
0
40
0.1 0.5
104LEGEND
55
Plasticity Index, %Range of apparent maximum past pressure, casagrandeconstruction (Data from Geotechnical Engineers, INC.)
Data from this study and McKown
Apparent Maximum Past Pressure vs. Log CalciumCarbonate Content for Pierre Shale Specimens
10487
61
62
57
2 tests
2 tests 3 tests
76
50
52
70 4238
44
69
7055
59
46
σp =70 15+_'
1.0Calcium Carbonate Content, %
App
aren
t M
axim
um P
ast
Pre
ssur
e,
σ vm
, kg/
cm2
5 10 50 100
5
10
15
20
25
100
200
300
σ vm
, MPa
Figure by MIT OCW.
Adpated from:
O O
I
0
0 0N r
U°5 nfi
o 0 0- N
I I I
0I
0
0I
0I
0 0I
0 0 0 0( - 00
I I I I
ov0- CQ 0 0 0 =0 0 - - (
m m cn mn (1 a
3l * < ( o-e~ooo.
(IJ) NOILVA'Ia
L 3/3/3 /,32Z2/27/97
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!r C
< <00<1
E-
z0
0U)
z
4 >
z'I) 0-0o>z'C
ZO
o
#s E
-!b!
-4
(O Uo06
oE-
r,) OU2
CW
0ocq o
O
(0
rbU-) -
)
12z
o0
1 I I I 1 I I~~~~~~~~~~~
............... . .. ....... .... ... .... ... .... ........... ...... . ..... ...... .... . ... .... ... . . .... ... W ... ..... . ... . ...... .... .. .. .........-- .
....... .. .. ....... .. ... .
O.
. .. .... .. . ..... ... .... . ... ... ....-
e 0 0............... ...... ..................... . ...................-
'O r
6
j - - - - 1CCL 3/3/67 /1 322 )/gS
3/1/6 3 2/97 /Cq
5. S 8PLtO DISTWV6AJcE (Ste r-F. 2-6, i4 )
I
NE- Vo/Ibdi/y ofpQr,//ozsumplion vs cchnistr;
(W4t4L fC&midg)
I
B~
I
/03 vc.
5,2 Ecs of /Dl/rnce
2) Ob5ct r Jsadly ower sf. p
3) 5,gn;fance /ntr. rCOmorassovn ComrqSf,&,/h
,'. Jho3cu/d /¢C/ude ?
4) :t/,. /o,C r/gn co,pn?,',/,,y
* dc/ 2-2 -/ow-o1decr 5
,^CC~rt s CR CI ~//5t05 c bt Cn cm mucAr
rOsfo v/r gs 02s-, a,7 (pi/) 1
roou~ o,~,- o.s*6 l{n~i/b
'Mu
.,11
14zG
5.,/ schemlac
mode, o /htrb(n
f ! * · vl -- · �' - II1/-'O -Pr PGf
I-
IIN,
('kd4
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- Rconstrctl n of In s/fu Compr.ss5/onOCurve u/5i7y9 chmnrt1monns M/lfhod
gsK(l1Ss) V"104r. Ad c, cd', /95t ThN 4sc ;/20, /20OI-/2
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UVO
5042 7p/e)
;0,42(,
As/um ed
3hould b tymwactrol Obouf --r " I
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Consoid aton trSX J s
-I t,,, P -L
(CCt 3/2/9
o.
.0
3:OA
.,
- -
- - I~~~~T.,., (0-,5Lmdncj) = T
alv (10,q co/,Z
-40-
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6 GP#C/)L ETHOID -O ,ST/MztT£ pf
lf 2 Csrg/ndc(AC)
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Add ,i/n -m. >
6,3 ckten mnqn(Fn . 2-6 , oAX/o0) E 0
/Vo ltlhcci usc t 5incz s* /iClvn,7Lgge -, /fl/,lLCrv% .,7
'/* r A4 L/cAY- co LOW OCR* CCL pq&i Led44y f (not Ccu j /LAuAwOU -_ Wq
L- it, rA1 h4 :%1 e t S- A , VCL7-e -~1;45 4 wr0 SelhQD, VLs LVI..I/i~ .*ij7P4~f·T. .'J
gil 2u/e"r-I/td (/?7? Jed, Ao)
/o ( t)-
./,3(I/O(/ -E)]
,---- - /f Mont vch hoaky\c cit - ,WT y r /e ce n no vah/i
'a~\ -· 'Ci-"'~~(e,9. 1zi .v4)
I
6,/ S~ ran Frr y -- rk/jtn; Vodo (Cv& /31)
Sat p /2 fp/e ( d A d W 'eYdcA,4 t; "o t, CR Am VCL)
U d4oO Ce-'4 ·.- j, -la.ty . 0 4c' , COrmenda-oS,. ̂ ~ ~ c , ,~c y uLo
6. ~5 F r4~4 o-'cj . 6/ au47 i.* pt
) /c, SE Zoci t I PoV
.
14 `
II
i~ ~ I
11,
/1322 1-D rl A.a PrCc 3 1,322z i /
0 . Z
0 0 0 0 0 = () e^
//O,,/ it 757$ (laej) uoWIAe l30f0Jd
jN - tv~~
- 4.- -)
o t~ , '
Q
4
C 0=
w, -I-
0 E
to - -
Y,~~~~~~1
0 :ZEIC
Ladd et al. (I 9e?)
o
11
0.1
-20
0
20
Proj
ect E
leva
tion
(fee
t)
40
60
80 0.095
0.2 0.3 0.4Compression Ratio (CR)
Virgin Compression Ratio vs. Elevation at SB and
EB Test Sites
0.5 0.6 0.7 0.8
Oedometer - DisturbedOedometer - TubeOedometer - BlockCRSC - TubeCRSC - Block
SB C
rust
CKo - TX
EB C
rust
0.125
20
Verti
cal S
train
, εv
(%)
Vertical Effective Stress, σv (KSF)
Typical 1-D Compression Curves for Boston Blue Clay at SB Site
'
15
10
5
0
1 10
(0.2)
(0.18)
(0.19 constant)
(0.48)
OED 8EI.9.5
Possible curve
CRS 24EI.55.1OCR=3.20
CRS 19EI.4.0OCR=1.12
100
σvo CR( )' 'σp
Figure by MIT OCW.
Figure by MIT OCW.
Adapted from:
I I ..4
Y" S79RA/#1 IER 4'c/w -'Woey PEa uAIr Voiu7E6
() Crobs Gronn (/le7), eyfc (6(2)
(2) 4vVenac, f (7f), of. 2()
(3) ¢ckr, Crooks, een , getr-aes (/e87), Con.,o-7,, 4(4)
Sir,- FhQrg work' , O/zum ( 'rd, ;e, , d,, , t d,3)f kO0dnomflSiAr Wvf/Vd, = (CA ev) or a , no
R'41' 3) 'rVCA, Jts 0T6e tqfurgt
7Qcihniwae 'A WRa4) : o641 60fa YEDTY
/ /51/7u skAsscs,
(Jee p l2e)
I
/I
/
,/ o - /,-,,IU/_ n/0 i
0 I/ 'O/O~ ~ c~~~~~ I'P b b,:~~~~~~~~
e > 9CCO
w2 -7 v2
i v; 'r
1.u~V-1
II
14'cOCI'
I
TO
I
WI
~4J
bt,I
1C1- 0-'II
(/)
Fno / a,
Se I -- I
orJ
,f , ,_ - _ , , , , {-
Fl"n / c- -
CCZ /7,/Qc
_ _--�-"
I
I
10PJ
,--O--- I -- 4wl
, loccllJr
I
'-O-O -=
/I ? 2 I -D cf PK
20
40 See detail above
W (k
J/m
3 )
W (kJ/m3)
60
80
00
4
8
12
16
200 400Stress (kPa)
600
Depth = 25.8m below Seabed
Vertically trimmed oedometer sample
800
100
120
00 400 800
Horizontal Effective Stress (kPa)
Work per unit volume interpretation of VTO test on overconsolidated Beaufort Sea clay.
1200 1600 2000 2400 2800
A
A
'σhy'σh
'σho
B
{{
Beaufort Sea Clay
Figure by MIT OCW.
N#MP
CCt I"/#/df
e/26'11 322 LCCt 3sr/c t'It.~~ ~ 1 1 1 1 1 I i I . t i 1 1: ! 1 12c:' A<T'- 1 ---1-1.-- -i -
.. l.. I iI i : I : I i: t I: : I ....~~~~~~~~~~~~~~~~~~~~_ ..i ' !::i!r:::~ -' '/ :.-.-... .. ..... ... ..... .m · .a ,.... . ... .
__~tA s 4 {Ac) - /, 751 0,718 (p (J- (se)
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; Ccc�l�crSofr�t;�/O
Fi Componon of Precanml/daoonPremurq,5r;natte froCOrisopnda 01nd Shvi4Fn fryy rchmn vos for I7 OCdontartRs4s on B8C (flac/pzstdn smO/c 16o s Oawo4)
A Cosogronde aI, (sl)
?C / 27/97 1322 Como/, /arff32/?9 3/9
7 /55 F55*16/T O EFFEC5 OF 54#PLE D/s5rpjA'ccr OCA1
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a) cdL~ '~ac 4acliA~p~ W41A-tcar
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2) 5-S, e, aS Ivvs<P4 /
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3) £v ct dv &a 4iA C/ 5, S(p 14
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4) 7PPm('9) Sb/c (PacbY dviSfl6hn ( 46j) OCO< 4l PIfi4/ Psap1#,Ad5( 0 ^a4 T 4°Vc c. 4· LhtO I9/~iP tU4 In·Gb- (i p/^d) ~
... 3 gr;>>>os_,a_v$.r__ _ _ _ l.
rz-oty
" r..C8E'); z,:Ei
- r ' 9
_ .r _ $_v
7
0.10
4
8
12
0.2 0.5
Consolidation Stress, σvc
Coe
ffic
ient
of
Con
soli
dati
onc v
(10
-4 c
m2 /
sec)
(kg/cm2)
1 2 5
30
25
20Ver
tica
l S
trai
n, ε
v (%
)
15
10
Symbol
2nd
2nd testOCR = 1.15CR = 0.36
Effect of Disturbance on Oedometer Test Data:
Sample F1S57 (Depth = 128 FT)
1st test"OCR" = 0.56
CR = 0.25
σvm=1.35
18 66.5 0.51
Test No. TV (TSF)wN (%)
5
0
10
1st 12 64.8 0.30
σvm=2.75
σvo
Figure by MIT OCW.
Adapted from:
0
WaxTube
Note:1) Stresses in kg/cm2
2) EST. σvo = 2.403) Onboard TV = 0.48
Engineering Tests
Markings
Void
128.0
UUC no. 4su = 0.14wN = 72.2%
OED no. 12, wN = 64.8%σvm = 1.35, CR = 0.25
NP
QR
ST
UV
WX
YZ
E-
127.5
Dep
th (
ft)
127.0
0.1 0.2
su (kg/cm2)
0.3
Torvane Onboard
0.4 0.5
OED no. 18, wN = 66.5%
Comparison of Oedometer and Strength Data with Radiograph for Push Sample of Orinoco Clay
σvm = 2.75, CR = 0.36
TorvaneUUC
Figure by MIT OCW. Adapted from:
0.4 2 4 6Measured εv at σvo (%)'
Mea
sure
d σ p
/Bes
t Est
imat
e σ p
''
8 10 12
0.5
0.6
0.7
0.8
0.9
B
A
1.0
1.1
1.2
Boring
E1F1
56-13427-128
Note: A and B Denote Tests in Fig9-a
Recompression Strain vs. PreconsolidationPressure from Oedometer
Tests in the Soft Orinoco Clay
1.051.20
0.030.07
+__+
3755
510
+__+
Symbol z(ft) OCR Ip (%)
-160
Water Content, % Preconsolidation, TSF Pore Pressure, TSF
SOIL PROPERTIES PROFILE
Compression Ratio
Cc / (1+eo)1st series of tests2nd series of tests
PiezoconePiezometer
CRS tests
Plastic limit Liquid limit
Natural water content
0 20 40 60 0 1 2 3 0 1 2 3 4 0 0.1 0.2 0.3
-140
-120
-100
-80
Elev
atio
n, F
eet
Elev
atio
n, M
eter
s
-60
-40
-30
FillSand
Marl
Varved Clay
-20
50
12
0 100 200 300 0 100Preconsolidation, kPa Pore Pressure, kPa
200 300 40020
30
40
20
10
0
Apparent consolidationprofile from 1st and 2nd series of tests
Pore water pressure if soilis not underconsolidated
Average effectiveoverburden stress
Adapted from
Adapted
Figure by MIT OCW.
Figure by MIT OCW.
I
I
/3d
/32t eConso/,c3r4id
,2/97
4/)X Ad ? r S Mdtk eV " i" 1
H «vP &44 "S 2
80
3ksf 60
40C
. 2
0,, 2 0a).
O M?)X-42 0
-40(
Axial Strain at Overburden Stress (%)
® &Ds. o4dqo"vr: m1Al ocratJ c/drs u ex*,ro; - n ec.AnoI;4erte L4UQd piano ware i ct bos bt hreed6 B6C I sktIy f;e
Figure 5-14: South Boston Elevation vs. Axial Strain at Overburden Stress from CKoand Typical Oedometer Tests
119
CC 3/r2
I
q-,
CcL_- 3 /3 ·3 a I - '
ztq7 /5 31/f 3/4/O1
. FFECT OF 7T0 r AlO EOP
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2) rypcL /;C4ercece 0<,fa F vJ / dy : sts
3) S/t prccfiiQrz (4sT D213s-a d.pL0CoRshzft tc Ku 'X)- k *Zt fc 2e Z4rf lsr)
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\\
= X
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--
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&rM, D 486 -e¢? "'a 3 CRSC (WaA/s cf4 t W/DQ C/a)
4IfE ,.J AlD, 9 7(10)
/) Pncp/t +ow opro-k7r TV o 7 - 3
k - _ H_2�q .
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2) Eecs of on heSu/-d a-, -eep/6
4) dvn7Ioe ¢Co,,, dcda.* /o tlC
3) /kesrj S Ca.4o
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s) k 4k Pt J
es) k, ko~l oo Jkbm I & I/ '17Z
*/ 7ro &S / 'i4 a' 9oAI * // C CA / A vcjim edt
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(Mrf:; i /006"nr EOP rm U6 Z I k PIE sA b l)
cRs& 1A C&nu T cc ttk cv
a C G T (ami,4ns conef i Ml/)
/o0 k
Ck d/ 01,4
khAy Vcr0bl can -- erroneoi5 compressl Cuevc
A4AI C., IAA£
8,3 C 4) i 9 Ow ww*o/6
0 rlP3e dq Aon A.I, -Ai6 t
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/ogot j B*1vi f4I7-4 tRAe) &tVY 44-
4ve 6 MP /a~ 5z
I/nec,ry
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7
/I~-D 'lc;~~%I~~~ Part~II-P ?,cl PartZ ~~~~~~~~~~~~I..1 1 4'?7 i
er CAN./983) C H .. VOL. 20. 19
CAN. GEOTECH. J. VOL. 20, 1983
TABLE 1. Geotechnical properties of clays Chyo/wn /
Number Cuand Depth w St field vane Ko rpo.v
Site symbol (m) (%) WL Ip IL fall cone (kPa) (kPa) (kPa) Reference
Berthierville 11 3.7 72 59 34 1.4 15 14 21 47 Samson et al. 1981Morin et al. 1983
St-Cesaire 2+ 4.2 89 68 42 1.5 22 25 55 80 Samson etal. 1981St-Cdsaire 2+ 6.8 85 70 43 1.3 19 27 68 90Gloucester 3x 3.7 88 52 28 2.3 70 20 35 65 Samson etal. 1981
Leroueil et al. 1983Gloucester 3 x 4.1 76 53 29 1.8 35 20 38 67Gloucester 3 x 7.5 93 53 29 2.4 88 25 58 87Varennes 4* 8.9 62 65 39 0.9 28 60 64 216 Samson et al. 1981Joliette 5* 6.7 65 41 19 2.3 108 29 40 110 Samson et al. 1981Ste-Catherine 60 3.8 88 60 35 1.8 30 18 20 60 Samson et al. 1981
Morin et al. 1983Mascouche 7V 3.8 65 55 30 1.3 52 70 34 270 Leahy 1980
Marchand 1982St-Alban 8A 3.9 60 40 18 2.1 13 25 55 Leroueil etal. 1978a
Leahy 1980Fort Lennox 90 6.1 60 45 22 1.7 30 30 54 105 Leahy 1980
Paquin 1983Louiseville 100 9.2 75 70 27 1.1 22 45 58 160 Leahy 1980
Leblond 1981Batiscan 110 7.3 80 43 21 ' 2.7 85 25 60 88 Bouchard 1982Other sites Authors' files
XI'no
b
v
l6flasI-V
litrVERTICA STRAIN RATE ;, ,l /0-'-
IvrS
OTTAllWA ,CRAM;ORD,1 .i| / xOTHER SITES AND SYMSOU ,SE. TABLE I x
-~~~,o .
__'__ _O. _ __ __ O ---. 0 - - )b~/ U
0.7 -
. .. , , ,
ia4 -V -4
FIG. 7. Normalized preconsolidation pressure - strain rate relationship.
me7on / ra.e 'gyoic oe .af /dayIf It f. , It .. I' IL Ub Or
. s;O /I CC
I CCL 37 1.322
806
-::v. .
.
:c.
il<
0X
'rU
ri:,
CcL 3,/87 /. 32. / - (rc~ 4Lff3/O?/ 9 3/iq 3///O
q, / C E L 'Vi " 9S
9./ r4cnn.r oaJ aldwi*/1osn, CG- Td 807-825
/) &4,s/A for &c Sl/t (See//7c)
2) tAcr retu/s (sep/7ic)
f L(2o'1 ) -~T:9/O0 -5 -/olr/' ()3 a6r /o%
3) 6 7- cht rt ' ~J~t
e
PRT
I
7ypcd I/fl31 . Tj JC!! C
-Cd 7 Uk
m S'C 0@Ud. f A G. /flejo
A >> e - y?
, Hot (R-4)
· Conocf 5tso
/tcr Wajer q-dJo/phon
h'/t lercr. T /n)Cr. ?
W
,J Schpe.a/ -/ , X //4z c4/ac/
(R<4)
Lachlro'
Frts(R>4 ) -/. 4~~,. * -J V(.I "/ ,7 -V¢
2) 0 / cr P e al/ c hcr
r
Om77
R.#. (4Mc
fJne cdie,
/7 i.
h
CCLt /89
0
5
w
zC,,
nJ
I>
10
15
20
25
1561, 3Z2
CONSOLIDATION STRESS o\c (KSC)
Sample No. MP - B2 -S7
Depth 16.3'
Soil type Gray ClayeySilt (MH)
o At tp*At f
COMPRESSION CURVE
WN(%) 52.1
WL (%) 66.3Wp (%) 31.3Ip (%) 35.0
Remarks
TEST NO.
EstimatedoaCo 0.402 op 1. 7 KSCCR 0.168 RR 0.027
Gs 2.78 e o 1.494S(%) 97.0
Corrected for apparatuscompressibility.OED - B2 S7TC -I
Figure 4-14 Compression Curve for Temperature ControlledOedometer Test (OED-B2S7TC)
/M/ Ce,n'7/- cI, 7,'; fXcC/ensc /,n O ,Xar En:
so rheis -(85s)
Akcr/c s/C7t/rso' say, 41akf
A
A i 2/Iion 1 I-,io4C PA,4'rI f(L-L .'fi:Y~ tR.L I I _ rw" , .1 - _~L,(.. 31.I:~Y ~,,,c~ t t,,,~~~~~~~~~~~~~~~4*7
I
U.
W
...< cs
M==OCO
oocwroo,qq~9 2"II
- 7GGS,
r Irs>>
zl<
(Aj><41.
170
60
150so- so
C0oc
t 30
0 o 20 30 40 50 60Temperature C
FIG. 6-Preconsolidation pressure as a function of test temperatureforspecimens taken at 7 m depth at Bllckebol. Full line shows results of linearresression analysis.
r 7r, iJ o Sc, C/2( /4
T- Dal'a 4 veihjh C/4U .
FIG. S-CRS test with varying temperature. Clay from Blckebol.
00
Fq
0I - . i
4) 40 S0~~~~~~~~ - -1I/o
I 0
* _ IS
_ __ _ I-
/2
o
t`
IQ
_6'- q
0 7d IS' //f14r4(l8) SdvThCI4ysi lrcar rcessuon a Fty.6
l. LQdd f scA er (96gS) &Bson 8/,, C/ay
tnt %(r)(ls) , esr)d 4r ,tSiT r* " /Ia^i;6ag i (/Lq3) /temddcd93
Orani c/ay (,2( *Ao)
r From dsplaccmc e of coomprtss'MCurve for ctl'cyctc.s W, 6T10
8
4-
.'A
--
I
. .,...
,in
I
I!I I
l, oi, V 810
U1, (11/0
4 t0.
0.60
Variation of the Normalized Preconsolidation Pressure (σp/σp(20oC)) with Temperature' '
σ p /
σ p (T
= 2
0oC
) '
'
0.70
0.80
0.90
1.10
1.30
1.40
Note:For symbols, see table 2
5% per 10oC
10% per 10oC
0 20 40Temperature, oC
60 80 100
1.00
1.20
Figure by MIT OCW.
CCL 3/87 /, ~32z
,/ 9 3 /qAl o o C
3)/hChk & eC c ofC #a' conc, 0 n 6, cCiA 4 19
4) E cf o jo// on 1aJcdted eJ
' wUoc¢l w- W,,L
· sot GC ' ~W4s 9'kt(- 2.3)
C =- conc, 9/cc 4
./Coe, s W' V t c I-/)
W3 /-C -.',.f)
.- , onjl-fqef
{ GSL C o,/Sogcc
Popic Corr/a/rempirics.! Corrc/4 luf
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l crytc r t$cA o A' L -P/Q 1 iic cAarU -
i b. cbC&n.SI Ln ( a, DnIJ4/
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See /lq prc.6/,m - Clqs /3cqO5sson On
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2 s5IecA, e / Qn.JwCrc r7- /zr
( - sot)
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-
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EXe p/c (,C 2 33 -ct 4r -O0)
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C ~ 571 -4 Z -/ - 6/0, (s- 4'0 ,* )Wo o -~/ - 0./so(0. I2Z9;O.S4-15
2) cirecas f w / loo :(i,' c#J)
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(at Wp)
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t.u. d . .. , (s'/.- 4o6,)/o6 -. ,fQ2 ? ....JL - (60,o-476)/64.3 0,/?2
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