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Laboratory studies of the adfreeze bond between small- scale model
piles and frozen sand
Parameswaran, V. R.
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National Research
Conseil national
Council Canada
de recherches Canada
LABORATORY STUDIES OF
THE ADFREEZE BOND BETWEEN SMALLSCALE
MODEL PILES A N D FROZEN SAND
':+LYZED
by
V.R
Parameswaran
0
Reprinted,
with
permission, f b m
Vol.
1,
Proceedings 3rd International Conference
on Permafrost
held
in Edmonton, Alberta, 10
13
July 1978
p.
714 720
DBR Paper No.
813
Divirtoa of
Building
R e r e d
LABORATORY STUDIES OF THE ADFREEZE BOND BETWEEN SMALL-SCALE MODEL PILES AND FROZEN SAND
V.R. Parameswaran, D i v i s i o n of B u i l d i n g R e s e a r c h , N a t i o n a l R e s e a r c h C o u n c i l of Canada, Ottawa, O n t a r i o , KIA OR6
The a d f r e e z e s t r e n g t h developed d u r i n g f r e e z i n g of c y l i n d r i c a l p i l e s t o f i n e Ottawa sand mixed w i t h 1 4 % by w e i g h t of w a t e r was measured under c o n s t a n t r a t e s of
I n a c r e e p p i l e d i s p l a c e m e n t on a n I n s t r o n t e s t i n g machine and under c o n s t a n t l o a d
equipment]. Four t y p e s of p i l e were s t u d i e d : n a t u r a l B.C. f i r , c o n c r e t e , s t e e l c o a t e d w i t h a r e d o x i d e p r i m e r , and c r e o s o t e d B.C. f i r . C o n s t a n t r a t e t e s t s showed t h a t a d f r e e z e s t r e n g t h i n c r e a s e d w i t h i n c r e a s i n g l o a d i n g r a t e . P r e l i m i n a r y d a t a from t h e c o n s t a n t l o a d c r e e p t e s t s i n d i c a t e t h a t t h e l o a d dependence of t h e s t e a d y - s t a t e c r e e p r a t e f o r p i l e s i n f r o z e n sand a g r e e s w i t h t h e d i s p l a c e m e n t r a t e depen- d e n c e of t h e a d f r e e z e s t r e n g t h s d e t e r m i n e d by e x t r a p o l a t i o n of t h e r e s u l t s of t h e c o n s t a n t r a t e t e s t s . I n g e n e r a l , maximum a d f r e e z e s t r e n g t h developed w i t h n a t u r a l B.C. f i r , and t h e minimum w i t h c r e o s o t e d B.C. f i r . V.R. Parameswaran, D i v i s i o n d e s r e c h e r c h e s e n b z t i m e n t , C o n s e i l n a t i o n a l d e r e c h e r c h e s du Canada, Ottawa, O n t a r i o KIA OR6
L t a d h 6 r e n c e due a u g e l d e p i e u x c y l i n d r i q u e s 5 du s a b l e f i n d ' 0 t t a w a c o n t e n a n t 14% d ' e a u , a u p o i d s , a 6t.G mesur6e s o u s d6placement d e s p i e u x
h
v i t e s s e c o n s t a n t e , d a n s une machine d ' e s s a i I n s t r o n , e t s o u s c h a r g e c o n s t a n t e (dans un a p p a r e i l Provo- q u a n t l a r e p t a t i o n ) . Q u a t r e t y p e s d e p i e u x o n t 6 t 6 6 t u d i 6 s : en s a p i n d e Colombie non t r a i t s , e n b g t o n , en a c i e r r e c o u v e r t d ' u n p r i m a i r e a u minium d e plomb e t en s a p i n d e Colombie c r 6 o s o t 6 . Les e s s a i s 2 v i t e s s e c o n s t a n t e o n t montr6 que lVadh.Grence duea u g e l augmente a v e c l e t a u x d e m i s e en c h a r g e . Les r E s u l t a t s p r 6 l i m i n a i r e s d e s e s s a i s d e r e p t a t i o n b c h a r g e c o n s t a n t e i n d i q u e n t que l e r a p p o r t e n t r e l a c h a r g e e t l a r e p t a t i o n
h
v i t e s s e c o n s t a n t e d e s p i e u x d a n s l e s a b l e g e l 6 c o r r e s p o n d a u r a p p o r t e n t r e l e t a u x d e d t 5 ~ l a c e m e n t e t l a f o r c e d e lfadh.Grence due a u g e l e x t r a p o l 6 d e s r g s u l t a t s d e s e s s a i s h t a u x c o n s t a n t . Dans l ' e n s e m b l e , l q a d h 6 r e n c e maximale s e mani- f e s t a i t a v e c l e s a p i n d e Colombie non t r a i t 6 e t l ' a d h 6 r e n c e minimale, a v e c l e s a p i n d e Colombie cr.Gosot6. CuJIa C M e p 3 a H P i R Q P i J I l 4 H A p M ~ e C K P i X C B a f i C M e J l K 0 3 e p H H C T M M n e C K O M , C M e u a H wc
1 4 Bet.% BO-,a 3 ~ e p ~ n a c b
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n o c T o R H H H x C K O P O C T R X c M e u e - H U R C B a R H a U C n b J T a T e J 7 b H O R M a l L l M H e MHCTPOH W n p H IIOCTORHHOR H a I ' P Y 3 K e/ ~ a
M a u u H e n n R u c n u T a H w R H a n o n s y s e c ~ b / . H a y s a n a c b s e T H p e T u n a csah: C O C H O B a R ; ~ ~ T O H H ~ R ; C T a J I b H a R , I l O K p b I T a R C Y p W K O M ; W C O C H O B a R , I I p O n u T a H - H a R K p e 0 3 0 T O M . ~ T MW C l T H T a H H R l l O K a 3 a J l W , s T O C M n a C M e p 3 a H H R B O 3 P a C T a e Tc
y s e n w s e H w e Mc ~ o p o c ~ w
H a r p y x e H w x . n p e n s a p u ~ e n b ~ M e n a H H b l e u c n M T a H n f i H a l T O J I 3 y s e C T bnpu
n O C T O R H H 0 R H a r p y 3 K e y K a 3 M B a E O T H a T O , s T 0 3 a B H C W M O C T b C T a 6 u J I b ~ o f i C K O P O C T M n O J I 3 y W 3 C T H O T H a r p Y 3 K W A J l R C B ~ R B M e P 3 J I O M n e C K e C O r J I a C Y e T C R C 3 a B H C U M O C T b I O M e m y C K O P O C T b I O C M e u e H U R I4 CUJ-IOR c M e p 3 a H n R r O n P e A e J I R e M O f i n y T e M 3 K C T p a I I O J I R Q b i X - i p e 3 y J I b T a T O B H C ~ T H T ~ H H ~ ~ . O T M ~ ~ ~ H O , YT.0 M a K C H M a J I b H a Rcwna c ~ e p 3 a ~ w ~
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I I p O n H T a H H H X K p e 0 3 0 T O M .LABORATORY STUDIES OF THE ADFREEZE BOND BETWEEN SMALL-SCALE MODEL PILES
AND
FROZEN SANDV.R. Parameswaran
Division of Building Research, National Research Council of Canada Ottawa, Ontario, KIA OR6
T~ is the adfreeze strength at the pile-
soil interface, INTRODUCTION
Af is the pile-soil interfacial area in Pile foundations incorporating an air space the permafrost zone,
between the structure and the ground surface are
-rd
is the frictional drag stress between used extensively in permafrost areas to transfer the pile and the unfrozen soil (if the structure loads through the unstable active present) over the permafrost zone, layer to the more stable permafrost. Varioustypes of piles, including timber, steel pipes and
Ad is the pile-soil interfacial area in H-sections, and precast concrete piles, may be this zone,
used. Wood piles are the most common, however, L is the structural load, because they are available locally in many parts
of the permafrost regions. Cast-in-place concrete
T~ is the stress due to frost heave in the
piles have been used occasionally in special cases., active layer in the ground As a rule of thumb, a minimum depth of embedment
Ah is the pile-soil interfacial area in the
in permafrost of
3
metres or three times the active zone, maximum depth of the active layer during thedesign life of the structure (whichever is larger) U is the uplift load due to wind is recommended for piles in permafrost regions.
Bv knowing the distribution of the allowable
A
pile foundation must resist uplift forces due to frost heave in the active layer and loads due to wind and the weight of the structure. Pile foundations in frozen ground transfer superimposed loads by two mechanisms: end bearing, and shear along the pile (adfreezing). The total bearing capacity of a pile is therefore the sum of the calculated contributions of the two mechanisms. Empirical formulae for these calculations have already been proposed by several workers in the Soviet Union (Vyalov and Porkhaev, 1969), based on their experience in building in the North.The end bearing capacity of a pile can be ob- tained from the value of the compressive strengths of the soil determined under confined and unconfin- ed conditions. The shearing resistance developed at the pife-soil interface has two components: that due to adhesion of ice to the pile; and that due to soil grain friction at the pile-soil interface. The supporting capacity for a pile erabedded in permafrost results primarily from the shearing resistance at the pile surface. In general, for a pile supporting a structure in permafrost the following condition should be met:
where P is the end-bearing capacity for the pile, as determined from the compressive strength of the soil under the pile, the cross-
sectional area of the bottom end of the pile, and a suitable factor of safety,
-
adfreeze strength, T ~ , along the length of the pile, the depth of embedment in permafrost required to carry the applied load L can be calculated. Thus it is imperative that T~ be determined accurately to permit reliable design of foundations for structures in permafrost regions.
Although measurements of the adfreeze strength between piles and frozen ground have been taken since 1930 (mainly in the Soviet Union),
sufficient information is not yet available to make it possible to design for different founda- tion materials such as concrete, wood, and steel in various soils. The early tests were done by freezing a pile into the ground, then pushing it through or pulling it out of the completely frozen ground at a relatively fast rate and measuring the force required. The results of early work in the Soviet Union from short-term tests have been given by Tsytovich and Sumgin (1959), Tsytovich (1975) and Vyalov (1965). Crory (1966), Crory and Reed (1965) and Sanger (1969) have reported the results of pile load tests in the permafrost regions of North America for adfreeze strength, pile settlement under loads and heave of piles due to freeze-back of the active layer. Some of the tests were short term, and others were carried out ovCr periods of several weeks.
There has been no systematic laboratory measure- ment of the adfreeze strength between piles and soils. Recently, Laba (1974) measured the
c a l l e d i t ) b e t w e e n f r o z e n s a n d and c o n c r e t e u n d e r l a b o r a t o r y c o n d i t i o n s by p u s h i n g f r o z e n s a n d from a n i n n e r c y l i n d r i c a l c a v i t y i n a c o n c r e t e b l o c k a t a r a t e o f 1 . 2 mm p e r m i n u t e . These r e s u l t s i n d i c a t e , i n g e n e r a l , t h a t " f r o s t g r i p " d e c r e a s e d r a p i d l y w i t h i n c r e a s i n g p o r o s i t y , t h a t i t i n c r e a s e d w i t h i n c r e a s i n g i c e c o n t e n t i n t h e s a n d and t h a t " f r o s t g r i p " i n c r e a s e d w i t h d e c r e a s i n g t e m p e r a t u r e . L a b o r a t o r y s t u d i e s h a v e b e e n i n i t i a t e d o n t h e i n f l u e n c e o f v a r i a b l e s s u c h a s l o a d i n g r a t e , t y p e o f p i l e and p i l e s u r f a c e , t e m p e r a t u r e , m o i s t u r e , e t c . , on t h e a d f r e e z e s t r e n g t h and b e a r i n g c a p a c i t y o f p i l e s i n f r o z e n s o i l s . Some p r e l i m i n a r y r e s u l t s of measurement of t h e a d f r e e z e s t r e n g t h d e v e l o p e d a t t h e i n t e r f a c e between model p i l e s and f r o z e n s a n d - i c e m i x t u r e s a r e p r e s e n t e d i n t h i s p a p e r .
EXPERIMENTAL METHOD
Measurement o f A d f r e e z e S t r e n g t h u n d e r C o n s t a n t R a t e s of Displacemen!
The a p p a r a t u s used f o r t h e e x p e r i m e n t s i s i l l u s t r a t e d i n F i g . I . The model p i l e (A) was 76.2 mm i n d i a ~ . e t e r and 304.8 mm l o n g . Ottawa f i n e s a n d (ASTM S p e c i f i c a t i o n C-109, p a s s i n g S i e v e No. 3 0 and r e t a i n e d on S i e v e No. 1 0 0 ) mixed w i t h 14% by w e i g h t of w a t e r was p l a c e d and compacted a r o u n d t h e p i l e i n f i v e l a y e r s , e a c h 3 8 . 1 mm t h i c k , t o a n optimum d e n s i t y o f a b o u t 1 , 7 0 0 kg m-3, a s d e t e r m i n e d by a s t a n d a r d P r o c t o r t e s t . Box (B) was o f 25.4 mm t h i c k P l e x i g l a s p l a t e s , and t h e p l u g (C) and t h e b a s e (D) w e r e aluminum. The box c o n t a i n i n g b o t h p i l e and s a n d was p l a c e d i n a c o l d room ( m a i n t a i n e d a t -6Oc f 0.2"C) f o r f o u r d a y s t o e n s u r e c o m p l e t e f r e e z i n g of t h e s a n d . A thermo- c o u p l e (T) p l a c e d i n t h e m i d d l e of t h e sand w a s used t o d e t e r m i n e t e m p e r a t u r e
.
A f t e r c o m p l e t e f r e e z i n g t h e p l u g (C) was removed and t h e p i l e pushed o u t by a ram a t t a c h e d t o t h e c r o s s - h e a d of a f l o o r model I n s t r o n t e s t i n g machine (25000 kg c a p a c i t y ) i n s t a l l e d i n t h e c o l d room. Each t e s t was c a r r i e d o u t a t a c o n s t a n t r a t e of c r o s s - h e a d movement. D i s p l a c e m e n t of t h e p i l e was t a k e n t o b e e q u a l t o t h e d i s p l a c e m e n t o f t h e c r o s s - h e a d l e s s t h e d e f l e c t i o n o f t h e p l a t e (D), measured by a d i a l gauge o r a DCDT p o s i t i o n e d u n d e r t h e p l a t e n e a r t h e p i l e . Four t y p e s o f c y l i n d r i c a l p i l e s w e r e s t u d i e d : N a t u r a l B.C. f i r w i t h a smooth s u r f a c e f i n i s h . C o n c r e t e p i l e s w i t h a smooth s u r f a c e f i n i s h . T h e s e w e r e c a s t i n t h e l a b o r a t o r y from a commercial d r y mix, S a k r e t e , t o which w a t e r was added i n t h e recommended p r o p o r t i o n . A f t e r c a s t i n g i n P l e x i g l a s t u b e s h a v i n g a n i n t e r n a l d i a m e t e r of 76.2 mm and w a l l t h i c k n e s s of 1 2 . 7 mm, t h e c o n c r e t e mix was v i b r a t e d u s i n g a n e l e c t r i c v i b r a t o r t o e l i m i n a t e a s much o c c l u d e d a i r a s p o s s i b l e . The f i n i s h e d and c u r e d c o n c r e t e ' c y l i n d e r s had a d e n s i t y of 2250 kg m-3. S t e e l p i l e s made from m i l d s t e e l t u b e s h a v i n g o u t s i d e d i a m e t e r o f 76.2 mm and w a l l t h i c k n e s s o f 6 . 3 5 mm c l o s e d a t t h e b o t t o m end w i t h a welded s t e e l p l u g and a t t h e t o p by a r u b b e r s t o p p e r . T h e s e p i l e s w e r e p a i n t e d w i t h a r e d o x i d e p r i m e r t o p r e v e n t r u s t i n g i n t h e wet s a n d . C r e o s o t e d B.C. f i r . B.C. f i r p i l e s , machined t o a smooth s u r f a c e f i n i s h , were c r e o s o t e d i n a h i g h p r e s s u r e a u t o c l a v e i n t h e E a s t e r n F o r e s t P r o d u c t s L a b o r a t o r y , Department o f Environment, Ottawa. F o l l o w i n g c r e o s o t i n g , t h e wood was found t o h a v e a b s o r b e d , o n a n a v e r a g e , 9 6 . 3 kg m-3, i . e . e a c h p i l e would h a v e a b o u t 0.136 kg o f c r e o s o t e . R e s u l t s o f C o n s t a n t R a t e T e s t s When a p i l e was l o a d e d a t a c o n s t a n t r a t e , t h e l o a d - d i s p l a c e m e n t c u r v e was v e r y s i m i l a r t o t h e s t r e s s - s t r a i n c u r v e f o r a f r o z e n s o i l i n uncon- f i n e d c o m p r e s s i o n , a s shown i n F i g . 2 f o r a n u n t r e a t e d B.C. f i r p i l e . The l o a d r e a c h e d a p e a k , t h e n dropped q u i c k l y , i n d i c a t i n g t h a t t h e bondbetween t h e wooden p i l e and s a n d had broken. A
s i m i l a r c u r v e was o b t a i n e d f o r c o n c r e t e p i l e s . F o r a p a i n t e d steel p i l e , t h e l o a d r e a c h e d a maximum, t h e n dropped a b r u p t l y , i n d i c a t i n g a c l e a n s h e a r o f t h e p i l e from t h e s o i l . I n F i g . 2 t h e l o a d d e c r e a s e s l e s s a b r u p t l y , i n d i c a t i n g t h a t t h e r e i s s t i l l some a d h e s i o n a t t h e i n t e r f a c e . A d f r e e z e s t r e n g t h was c a l c u l a t e d by d i v i d i n g t h e maximum l o a d a t t h e p e a k of t h e c u r v e by t h e s u r f a c e a r e a o f c o n t a c t between t h e p i l e and t h e s o i l . The I n s t r o n c r o s s - h e a d s p e e d s w e r e v a r i e d
between 0.0005 and 0 . 1 mm min-l. At t h e s l o w e s t
r a t e i t t o o k a b o u t 50 h o u r s t o r e a c h a p e a k , and a t t h e f a s t e s t r a t e o n l y a b o u t 30 m i n u t e s . D i s p l a c e m e n t a t peak l o a d was a b o u t 0 . 5 t o 1.5 mm, d e p e n d i n g upon t h e t y p e o f p i l e and t h e r a t e o f l o a d i n g . V a l u e s o f a d f r e e z e s t r e n g t h o b t a i n e d f o r t h e v a r i o u s p i l e s a t d i f f e r e n t r a t e s o f l o a d i n g a r e shown i n T a b l e I . F i g u r e 3 g i v e s a d f r e e z e s t r e n g t h s p l o t t e d a s a f u n c t i o n of l o a d i n g r a t e on a l o g - l o g s c a l e f o r t h e f o u r k i n d s of p i l e s . A d f r e e z e s t r e n g t h , T ~ v a r i e s w i t h r a t e of p i l e , d i s p l a c e m e n t
L,
a c c o r d i n g t o : The v a l u e s o f m and n , o b t a i n e d by 1 i ~ i e a r r e g r e s s i o n a n a l y s i s , a r e a s f o l l o w s : - B.C. f i r C o n c t e t e 0.2161 4 . 6 3 P a i n t e d s t e e l 0.1661 6.02 C r e o s o t e d B.C. f i r 0.1862 5 . 3 7The maximum a d f r e e z e s t r e n g t h was f o r u n t r e a t e d B.C. f i r and minimum f o r c r e o s o t e d B.C. f i r and p a i n t e d s t e e l p i l e s . The a d f r e e z e s t r e n g t h v a l u e s o b t a i n e d f o r c o n c r e t e p i l e s w e r e l a r g e r t h a n t h o s e f o r . c r e o s o t e d B.C. f i r and p a i n t e d s t e e l , b u t c o n s i d e r a b l y lower t h a n t h o s e f o r u n t r e a t e d B.C. f i r . Constant-Load T e s t s I n a c t u a l p r a c t i c e , a p i l e f o u n d a t i o n s u p p o r t i n g
a structure is subjected to constant loads rather
than constant rates of load application. Creep is
the process of deformation under such conditions,
occurring at the interface between the pile and the
soil. To simulate these conditions in model
studies, a constant-load creep apparatus was built
for which the Plexiglas box with pile shown in Fig.
1 could be used.
Figure 4 is a schematic diagram of the creep
frame with the pile inside the sand box. Weights
were placed on the loading pan (B).
This load was
magnified by a factor of 4 at pile A due to the
ratio a n
(C).
The load on the pile was measured
by means of a BLH load cell (D) having a capacity of
4550 kg. The BLH load cell was calibrated on the
Instron load cell which was, in turn, calibrated
by a proving ring.
Two DCDT's, one positioned under the pile and the
other under the plate supporting the block of
frozen sand, monitored deflections due to the load.
Net pile displacement was taken to be equal to the
difference between the two deflections.
Results of Constant-Load Creep Tests
Figure 5 shows a typical net displacement-time
curve obtained for a painted steel pile. The load
on the pile was 1130.57 kg, corresponding to a
stress of 2.43 ?Pa on the pile head and 0.243
MPaalong the pile soil interface. This curve
resembles a classical creep curve, with a primary
region (A) where the creep rat? decreased to a
steady value, a short secondarg region (B) of about
8 hours, for which the steady-state creep rate was
1.04 x
nunmin-l, and a tertiary region (C)
where the creep rate accelerated until failure of
the pile occurred after about 34 hours.
The results of preliminary tests are shown in Fig.
6. The straight lines 1 to 4 are extrapolations
to the lower-rate regions of the adfreeze strengths
vs loading rate lines shown in Fig. 3; the plotted
points indicate the rates of motion of the piles
in the steady-state creep region under constant load
(region B in Fig. 5).
In Fig. 6, line 5 for creep
of painted steel has about the same slope as line
3, the adfreeze strength vs loading rate. For
concrete and creosoted B.C. fir, the data obtained
from the constant-load creep experiments are in
reasonable agreement with the results of the
adfreeze strength tests under constant rates of
loading, extrapolated to the lower strain rate
regions.
DISCUSSION
AND CONCLUSION
1
Data available in the literature on the adfreeze
strength of piles in ftozen soil are meagre, and
most laboratory tests to determine adfreeze
strength have been done at fast rates (Tsytovich
1975, Laba 1974, Rooney 1976).
The preliminary
results now presented indicate that adfreeze
strength decreases with decreasing rate of loading.
Preliminary data from creep tests indicate that
the load dependence of the steady-state creep rate
for piles in frozen sand appear to agree with the
displacement rate dependence of the adfreeze
strength determined by extrapolation of the results
of the constant rate tests. Long-term creep tests
give more realistic values for the long-term
adfreeze strengths and hence for the bearing
capacities for piles. The results obtained from
rapid tests cannot be used to calculate the long-
term bearing capacity of piles in frozen soil
unless a large factor of safety is used.
Few tests have been carried out to date and
further work must be done to determine the
behaviour of piles in various soils at different
temperatures and to obtain reliable data for design
of foundations in frozen soil. Work is in
progress in the cold rooms of the Division of
Building Research, National Research Council of
Canada, on the behaviour of steel H-section piles
in frozen sand, group piles (groups of 4 and 6)
in frozen sand and piles in frozen natural soils
under conditions of constant rates of load
application and constant loads.
ACKNOWLEDGEMENT
The author sincerely thanks G. Mould, Technical
Officer, DBRINRC for his help in designing the
equipment and carrying out the tests. This paper
is a contribution from the Division of Building
Research, National Research Council of Canada,
and is published with the approval of the
Director of the Division.
REFERENCES
Crory, F.E., 1966. Pile Foundations in
Permafrost. PERMAFROST. Proc., First
International Conference on Permafrost,
Lafayette, Indiana, National Academy of
Sciences, Washington, p. 467-476.
Crory, F.E. and Reed, R.E., 1965. Measurement
of Frost Heaving Forces on Piles. U.S. Army
Cold Regions Research and Engineering Laboratory,
Hanover, N.H., Technical Report No. 145,
p.31.
Laba, J.T., 1974. Adfreezing of Sands to Concrete.
U.S., National Research Council, Transportation
Research Board, Record No. 497, p. 31-39.
Rooney, J.W., 1976. Driven H-pile Foundations in
Frozen Sands and Gravel. Presented, Second
International Symposium on Cold Regions
Engineering, University of Alaska, Fairbanks.
Sanger, F.J., 1969. Foundations of Structures in
Cold Regions. U.S. Army Cold Regions Research
and Engineering Laboratory, Hanover, N.H., Cold
Regions Science and Engineering Monograph 111-C4.
Tsytovich, N.A., and M.I. Sumgin, 1959.
[Principles of Mechanics of Frozen Grounds],
U.S. Army Corps of Engineers, SIPRE Translation
No. 19, (now U.S. Army CRREL).
Tsytovich, N.A., 1975. THE MECHANICS OF FROZEN
GROUND. McGraw-Hill, New York, p. 426.
Vyalov, S.S., 1965. Rheological Properties and
Bearing Capacity of Frozen Soils. U.S. Army
Cold Regions Research and Engineering Laboratory,
Hanover, New Hampshire, Translation No. 74.
718
Vyalov, S.S. and Porkhaev, G.V., 1969. Handbook R e s e a r c h Council o f Canada, T e c h n i c a l T r a n s l a t i o n
f o r Design of Bases a n d F o u n d a t i o n s of B u i l d i n g s TT-1865, Ottawa, 19 76.
and 0 t h e r S t r u c t u r e s on P e r m a f r o s t . N a t i o n a l
TABLE I
/ VARIATION OF ADFREEZE STRENGTH WITH RATE OF LOADING
Cross-Hefd Adf r e e z e S t r e n g t h ( T ~ ) , MPa
Speed
(II)
P a i n t e d C r e o s o t e d -1 mm min B .C. F i r C o n c r e t e S t e e 1 B.C. F i r 0.0005 1.140 0.525 0.497 0 . 4 0 3 0 . 0 0 1 1.175 0.553 0.496 0.487 1.29 0.002 1 . 1 1 3 0.671 0.648 0.690 1.247 0.505 0 -005 1 . 6 1 0 . 7 3 3 0.677 0.720 0 . 0 1 1 . 5 6 0.866 0.679 0.813 0.940 0.02 1.936 1 . 1 6 0 . 9 7 3 0.920 0.05 2.231 1.293 1.026 0.875 0.10 ' 2.42 1 . 6 1 1 1.146 1.220 F i g u r e 1 Schema t i c Diagram o f t h e E x p e r i m e n t a l Set-Up t o Measure t h e Adf r e e z e S t r e n g t h Under C o n s t a n t R a t e of Cross-Head Moti.on A P i l c , 3" DiaB P l e x i g l a s Box
C P l u g
D Base P l a t e
E Upper Compression Member from I n s t r o n Load C e l l
T Thermocouple
F i g u r e 2 Load-Dis t a n c e Curve f o r an U n t r e a t e d B.C. F i r P i l e i n F r o z e n Sand
(T
= ~ O C , Cross- Head Speed = 0 . 1 d m i n ) 10 I 1 1 1 1 1 1 1 1 I I 1 1 I 1 I l l - 1 I I I I I l I J - B C F I R --
C O N C R E T E-
-
-
P A I N T E D S T E E L 0 C R E O S O T E D B C F I R-
-
-
F i g u r e 3 V a r i a t i o n o f A d f r e e z e S t r e n g t h w i t h R a t e of Loading 0 I I I 1 1 1 1 1 1 I I I I 1 I ~ r f I I 1 1 1 1 1 l o ' 2 1 0 - I C R O S S - H E A D S P E E D , r n m l m i n F i g u r e 4Schematic Diagram of t h e Set-Up t o S t u d y t h e Creep o f P i l e s i n F r o z e n Sand Under C o n s t a n t Load (A
-
P i l e , B-
Loading Pan, C-
R a t i o A r m ( 1 : 4 ) , D-
BLH Load C e l l , E - F r o z e n Sand)F i g u r e 5
Creep Curve f o r a P a i n t e d S t e e l P i l e i n Frozen Sand
(T
= 6.Z°C, Loaded = 1130.57 kg)720
0.6 0 . 5 - c ; 0 . 4 - Z u5
> o I '0 . 3 - u 1-
0.2 0. O.' I I I I I I-
C R E E P R A T E =r
1 . 0 4 x rnrnlrnin-
i-
i
I d I I7 -
-
AI/
-
;
y
i
-
/
I
!
I 1-
./
I - 0 n I I 1 I I I 5 10 15 20 25 30 35 TIME, h 1 0 . 0-
I 1 1 1 1 1 1 1 1 I 1 1 1 1 1 1 1 1 I 1 1 1 1 1 1 1 -8 . 0 6 . 0 4.0 u-
B . C . F I R --
----
m C O N C R E T E - 0 P A l N l E D S T E E L-
---
0 C R E O S O I E D B . C . F I R --
F i g u r e 6 V 4 .d V a r i a t i o n o f A d f r e e z e S t r e n g t h (Under 2 - 2 . 0 --
C o n s t a n t Load) w i t h Creep Rate i n t h e -
-
S teady-S t a t e Creep Region 0
Y, 1.0