Soil Liquefaction Potential Evaluation with Use of the Simplified Procedure T. Iwasaki and K. Tokida Ground Vibration Division, Earthquake Disaster Prevention Department, Public Works Research Institute, Ministry of Construction, Tsukuba Science City, lbaraki-ken, Japan F. Tatsuoka Associate Professor, Institute of Industrial Science, University of Tokyo, Tokyo, Japan SYNOPSIS A simplified method based on both a liquefaction resistance factor, FL and a liquefaction potential factor, PL has been proposed for evaluating soil liquefaction potential. The factor FL indicates the liquefaction potential at a given depth of a site, and the factor PL indicates the one at a site. The effectiveness of the proposed method is investigated by calculating the factors FL and PL at both liquefied and non-liquefied sites during past typical earthquakes in Japan, and carrying out shaking table tests. INTRODUCTION As a result of various and detail studies on the liquefaction of sandy soils, several simplified and complex methods have been proposed to evaluate the liquefaction potential. The authors, Iwasaki et al. (1978), proposed a simplified method with use of a liquefaction resistance factor FL and a liquefaction potential factor PL • Based on the simplified method, the liquefaction potential of sandy soils can be estimated from its N-values, its unit weights, its mean particle diameters, and the maximum acceleration at the ground surface. In this paper, the simplified method is described and to prove the effectiveness of the method, the factors FL and PL at 64 liquefied sites and 23 non-liquefied sites during past various earthquakes are calculated according to the proposed simplified method, and also the factor FL is calculated for the model ground in the shaking table tests on soil liquefaction. where N is the number of blows in the standard penetration test, Ov' is the effective overburden pressure (in kg£ /cm2), and Dso is the mean particle diameter (in mm). L in Eq. 1 is the dynamic load induced in the soil element by a seismic motion, and can be estimated by asmax Ov (3) rJ/ g where 'max is the maximum shear stress (in kgf/cm2), <Xsmax is the maximum acceleration at the ground surface (in gals), g is the acceleration of gravity(= 980 gals), avis the total overburden pressure (in kfg /cm2), and rd, the reduction factor for dynamic shear stress, accounting for the deformation of the ground. In 1971, Seed and Idriss proposed a relationship between rd and depth. However, in this paper, the relationship, SIMPLIFIED METHOD In the proposed simplified method an ability to resist the liquefaction of a soil element at an arbitrary depth can be expressed by the factor of liquefaction resistance (FL). R 00 ] ( 1) L N .J: a. where R is the in- situ resistance (or undrained cyclic strength) of a soil element to dynamic loads and can be simply evaluated, based on undrained cyclic shear test results, as follows : for 0.04 R ~ 7IU1l • 0.0882 R = 0.0882 D,o · 0.6 ~ J07+Q? + A Oy' N + 0. 7 0.225 log - 0 05 . 10 D;; F~ W(z) 2.0 10 5 5 10 10 15 15 20 20 Cli a TIUII 0.35 . (b) (a) (2a) (2b) Fig. l 209 Integration of FL 210 rd =l - 0, 0 15 Z Nishi (4) Oh- hat a D5o 0I where Z is the depth in meters, is used, 02 o---o 0 0 10 It is obvious that the damage to foundations due to soil liquefaction is considerably affected by the severity of liquefaction, As only the ability to resist liquefaction at a given depth can be evaluated by FL , an index of liquefaction potential, PL, can be introduced to express the severity of liquefaction as, Cho (mml ( 20 30 Ni igata City el'ltimsted ) 05 N( after in I0 earthquakt•)---... 40 50 0 0 FL I0 20 ks' 0 17 r, oJ-0.015Z --¥= (5) $ N ----~ in which F = l - FL for FL 1,0 and F = 0 for FL > 1,0 as illustrated in Fig, l(a), and W (Z) = 10- 0,52 (Z in meters), as illustrated in Fig, l(b), For the case of FL = 0, 0 for the entire range from Z = 0 to Z =20m, PL becomes 100, and for the case of FL 1,0 for the entire range from Z = 0 to Z = 20 m, PL becomes 0, 0, I0 tJ t 050 + I } 15 CASE STUDIES OF PAST VARIOUS EARTHQUAKES Kuribayashi et al, (1974) accumulated data on liquefaction observed during past 44 earthquakes in Japan, and made clear the distribution of liquefied sites and damage of structures due to liquefaction, Furthermore in 197 8 liquefaction was observed at about 30 sites during the Miyagi-ken-oki Earthquake (Iwasaki et al, (1980) ), Both the liquefaction resistance factor, FL and the liquefaction potential factor, PL were calculated for liquefied sites and non-liquefied sites where geotechnical information was available, during each of the following 6 earthquakes : the Nobi Earthquake ( 1891), the Tonankai Earthquake ( 1944), the Fukui Earthquake ( 1948), the Niigata Earthquake ( 19 64), the Tokachi-oki Earthquake (1968) and the Miyagi-ken-oki Earthquake (1978). Calculations were made for 64 liquefied sites and 23 nonliquefied sites, The geotechnical and seismic data at the sites are summarized in Table l, Fig, 2 Relationships between FL and Z at the NonLiquefied Site Shows Bridge in Nii~ata City (Bori~ Not) Dso lmml 01 02 c:--<> 0 0 10 10 05 ( a f tf"r ear thcpake) --....... 20 30 40 50 00 I 0 20 * § N Figs, 2 and 3 show the typical variation of FL with depth at a liquefied and a non-liquefied site, respectively. It can be seen that FL is, in general, less than 1,0 in the liquefied layers, and greater than l, 0 in the non-liquefied layers, The tendency of FL at other sites was similar, FL ks' 0.17 r, 'i-0.015Z ---- Fig, 5 summarize the calculations of FL with depth at all liquefied and non-liquefied sites in Niigata Earthquake (see Table 1), The liquefied layers shown by black dots in the figure were estimated based on damage to structures (see Fig. 3). It can also be seen that FL is mainly less than l. 0 in the liquefied layers and the liquefied layers are mostly located at shallower depth than 10 m, 10 ----- Dso ~~>X '' X 15 * lL is estimated from Fig. 3 the damage to piles Relationships between FL and Z at the Liquefied Site Geotechnical Data at Liquefied Sites and Non-Liquefied Sites (B) Non-Liquefied Sites Table 1 Liquefied Sites (A) Sot! Data Earthq.ldke S1te No, Deptn of WHer Table D5o ~-Om M _ MaJor SoLI Type Fme to Me<l. Sand 2.) M 0. 3 £,:-.1 2.<; M " 0. 0 -- Jtndoji K-~-g~ne-.-~-ho 4 -: -~:~~~;;~ho- 20.2 18.3 Br. 5 0.0 E.~ 39.3 Br. 7 0.0 E,M lb.l Br.!. 0.0 Br. l 1.50 " " 0.0 0. 0 E Br. 2 0.0 " " l:lr.3 ~Lt'o)ata C1ty :'\ 1 q~a t" 0.0 , L9o-l, M:7.S Br. 2. o.o B Br. 3 19.6 l,l>j Br.l Br. 1 Br. 2 Br. 3 l. 2 ~ BCll-2 ~--~~---···-· 14.3 ~--< ll. 7 \1 C'Jarse Sand 2.8.6 " " " " ·" fu1e Sand 20.1 5.8 F1ne to Med. Sand -~~----- 13.3 F1ne S«nd 20.1 ~ G.fe~ Prei. l ~''l' M;:;~, Ctty l'"H.O, M=:~. F U.u, 45 __ 4_~ __ i__Ma_~~ka :-.lo.Z Pref. 47 j Gravelly Sanr:! M " 0.9 0 48 J Morth o[ Ab:lklHT\.1 YurLa_g_e_~k_amL 49 50 Yurtage Br1r:lge __ M~7. 56 57 T M~7. 2.4 4 Uomao;;hi Estimated from Damage to Structures 2.~7--~ (!J 6 36_._~ Recorded Value at Hachinohe Estimated by the Empincal Equation for Alluv1al Deposits ( Estimated by Using Fq;:. 4 Esttmated by Dynam1c '" BRI (19651 K1shida {1970) U,l 18) Yasur:la et al. 11980) ~and Co<>r~.- ~er:!. ~ ------ S.on-1 ::. .. nr:lv Slit to Mecl. Sand eta, to 5 173 Co"r~e S.!.r~d Sand 180 20.-1 180 10,3 180 9.9 11:15 1.0 185 fi o. ~ 185 ~ .! l. ~ 190 210 6 ZIO :vlc·l. to :>dty Sand • Cldy to Coarse Sand ~ 2.30 6 ns 61 -1---- :\u.l 0.0 62 :\·4 0.5 .\1 1.3 M fme to Coarse Sand ~ 1-1.1 ?.7.1 as 6 11:1.2 1!:10 fi 12.3 11:10 6 5,6 ·---- S·lt to ftne Sane! 36.? 185 125 Sdt to Me<:!. Sand 4.1 4.1 23 0 f'tne ""n-1 - ;, .. ..,..jy Analyses of Ground Reference Ohashtetal. (19771 ::.ar~d ~~!sponse BRI 11969) fme toM<·!. :.and A l Japanese Soc1ety of CIVil Eng1neers 0.0 ! ' I 295--t--i·l~-,- and !3-Z Estlmated from Recorded Value at Other S1tes (6) (31 0.0 W-G M ! Sdt to Med. Sand I ' ' ~~ : 1 0. 0 j 18.7 ~ j t M t-; 295 .~ E , M 4. } ---1-M ~-S•l~_y_to~~Sand_+~ 1 -Fin~-~~~~ -~--~~:; (2) ..... _, 4 7 v. ~toCoarseSand · 180 --·. -·--·· ..----+--Slit to Silty Sand : Me d. to ;·M- ;- Co~-rs; Sa-n~ 195 ,6 - (J) (8} t--m-:; I Fme Sand to Clay '·' 0.0 Sandy S1lt to Gravel Med. to Stlt~_Sand 17.1 0.0 F'tne to ~ed. Sand 3.7 --' I N B~l Ka.wagishi~Gho (I) ~o.l :-.-5 Recorded Value at {21 :"<o.l " 1 4. 0 8.0 M: Measured 19.5 " I Wabucht F1ne Sand to Silt ~_:~.:_6_j ~ 4. 6 I 1- - + ~ I I Fme to Mt-d. Sand M 1 A : So1l Data after Earthquake 2.3.7 Shtomi -- ~4 0.90 3,l5 Z70 59 63 1 '-' 60 -------+---------- A ., 210 !.72 ::-lakamura I 170 uu~t~;;;-~;_;-;:-;:;-;;;:,;.0;•---i ·'"- .._1 2.50 ; 13.0 :\o.l?. ---+--------- ~ -:----L~-3~~- 13 ll_Q ~~- -~-rhfu __ ___,___ I (71 .\i"t·~. 0.0 ' A 0.85 3,9 Compacted by Sand Compaction Piles, near Uornachi ll.-1 \.lecJ. to " " E I M_t' :m_e -~~.=dty Sand 4. 3 M1yagi-kenOk1, 1978, M=7.4 I Estunated by Vs1ng Table 2 ~~ • :>andy s,l\ to 0.?.6 ~7 M1yag1 Pre!. B: Soil Data before Earthquake E (ll J.S.S.M.f.E. (19761 Ftn" to Mt··i. ;,ancJ 0. 0. I ~ed1um Sand E I __; ·- (51 (6) M 9.3 I Wabuchi l·L'l <.7 l17'i, A-2 31') :\o.l MIYil'll-kcn· 0. 0 1.8 ;o..;o.Z .\1.--: . .">an-:: to Gr,.,,·e! F,n._. to Ok1, toCoarse~~~-d-~ FtneSand .l- A·l Uomach1 Ishihara (1976) .)dt to Coarse Pre!. : MtnamiSendal {51 ~ \i•J.2 55: 23 'Med. I ... ~~ ~----· {4) \{ ~l.!Y"O:' 20 21 M M Br. 2 17.7 ~5 '\o,i ;\lo.l a.1 ~~ Yama;.akt ! Otri (IJ -+- EaL Bndge 32; l. 1.3 -+ r, .....'>«nd 0. 2 " l ·o Coarse :::ian'! !•.) Y·Z ~o. Br.1 2.6.3 • Y-l )(o.) Abukuma Brtdge zoo ;,and C"J.l.T»<' o.o - -+-- 3 .\l!"dl-J!ll S<1nrl C?arse Sand .J 52 53 to Grav. Sand 4.?. R1ve: 51 54 ~and ;,,:v.- O.!l FcllH.a, \1 Abuk"ma Br~~-~--- ----~- 235 0.7:; 1.2 -~~- -~52_____4___ ... Med•urr1._S_and -~~_L Ta_~~y_a l-16':1 46 " ().9 O.o 17 ... )._~---- --- -- t.l 0 l"onank-<>, :--/a~o)'a zoo -----·-·- :-;Obi, Pg ---~~?- fme Sand -·· 0.95 O.:i7 Ktnnou Budge 5.1 9. 7-- ----~~- Tokacht·Ok•, 19611, M=7.9 :--laton Rtver, 3.2 Km 22 1._3_3------~--F'~? ~d. Sand ----~- _ _ -1_._:1 !lakodate Ctty 15 ~:.-_'_':,~_to.Coarse~.~n_d__j l.l 3. 5 ~--o.ol 1 1 16 0.0 f1ne Sand 0.0 A l Yunage-kami Kttakaml R1ver E I Rei. P, (gall I ~--- I 14 MaJor Soil Type 18.9 Mer:hum Sand l:lr.l ~-a-~~-ya "' ~- Br.Z : ' 14.5 1.2 BCI1 ~ :\akamura 13 19 -~-~~- C0arse Sanrl -~~-~~.:!. + (-1) 10.5 _______1:2. BCZI-l ' .. --r A ,___ j A 12 16.5 110 A I :::;, Br.l 11 28.2 Coarse Sand \led. to Coarse Sand ~ 0.63 Gotanda Bridge I 2.3m 2.5 ____ ~-~ Ni•gata, 1964, M=7.5 fuku1, 1948, M«7.3 13.1 Br.Z l:lr.l 8 23.2 '-' Br. l City 32.9 Coarse Sand Q. 0 '·' o.;, ~iigata 1 (3) , Dso l -~-·'----~--~-~---+---M·~~J.~:ns~ ~--s Br, 5 2-1.0 Med. to Coarse Sand M Sr. L 1 A 1.~ ~---~ 0.6 -----~~~- _..,_ __Br.!. . • Bn , "'.l_j Mats~a~--·---~--~ +-Shtn ' -~---~ H•gash 1 Kosen 1.3 Soil Depth of Data i Water Table Site 5.8 ftne to Me d. Sand E, '-1: ;\lo, 9.0 ~1 0. 0 Rel. 24.'J Fu'l.C to Coarse Sand ------- 2.5 P, (gal! (1:1) 212 Table 2 Average Values of the Unit Weights and Mean Particle Diameters of Different Type of Soil (This table was used only when these values were not tested) Unit Weight, lt( t/113) Soil Type Fe Mean Particle Diaaeter, Dso (-) Surface Soil 1.7 0.02 Silt 1. 75 0.025 Sandy Silt 1.8 0.04 Silty Sand 1.8 0.07 Very Fine Sand 1.85 0.1 Fine Sand 1.95 0.15 I: .... a. UJ 0 Mediua Sand 2.0 0.35 Coarse Sand 2.0 0.6 Gravel 2.1 2.0 <lJ u ~ 200 ... :::J (./) 100 Fig, 5 Relationship between FL and Z at the Liquefied and Non-Liquefied Sites during Niigata Earthquake "'0 c ~ 50 (.9 Fig, 7 summarize the calculations of PL at all liquefied and non-liquefied sites in Table 1, i,e,, both relation between number of case and PL and relation between accumulative percentage of PL and PL, According to Fig, 7, it is found at non-liquefied sites PL is less than 20 and the probability that PL is less than 5 is 70 %, on the other hand at liquefied sites the probability that PL is less than 5 is only 20 %and 50 %of the sites range more than 15, Based on the above results, the assessment for soil liquefaction potential using PL can be clone as follows, ~ ;:n c .Q ;:n ... <lJ a; 20 10 ~ ,_~lion USod 5 (Kuribayasht & Iwasaki ,1980) u u <{ E :::J E x Ill ~ Measured Value 2 30 50 100 200 Liquefaction potential is very low and detail investigations on soil liquefaction aren't needed in general, 500 1000 IJ (km) Epicentral 01stance, Fig, 4 Relation between Maximum Acceleration at the ground surface, ftsmax , and Epicentral Distance, L1, during the Miyagi-ken-oki Earthquake Fig, 6 shows the frequency and accumulative incidences of FL values for both liquefied and non-liquefied layers at all sites in Table 1" Hereupon the liquefied layers were estimated based on damage to structures or if not estimated by soil conditions, i, e,, the saturated sandy layers whose N-value is less than 15 and whose D_, 0 ranges from 0,02 mm to 2,0 mm were regarded as liquefied layers, The distribution of FL at liquefied layers is very different from that at non-liquefied layers, At liquefied layers most (about 87 o/o) of FL values distribute in the range less than 1,0, and while at non-liquefied layers most (about 89 %) of FL values distribute in the range more than 1,0, However it must be noticed that about 13 % of FL values exceed 1, 0 at liquefied layers and about 11% of FL values indicate less than 1,0 at nonliquefied layers, O<PL 5 --- Liquefaction potential is low but detail investigations on soil liquefaction are needed only for specially important structures. 5<PL 15 -- Liquefaction potential is rather high and detail investigations on soil liquefaction are needed for important structures and countermeasures of soil liquefaction are neededed in general, ---- Liquefaction potential is very high and detail investigations and countermeasures on soil liquefaction are needed, 15 < PL As mentioned in the above, it has been shown that the liquefaction potentional factor PL may be used to assess the liquefaction potential at a certain site reasonably, Moreover the nee es sity for detail investigations on soil liquefaction also can be judged based on the factor pL calculated by the proposed simplified method, 213 ~ ~ 3.0 Depth Estimated Liquefied Loyer 0 ! 0 H 2.5 20 2.0 2.5 0 30CM 60CM BOCM 0 0 6 0 0 0 0 ~ 0 t==·;iJ~g ~ 20 0 100 ~ 0 3.0 ~ 0 ~ ll lO Oi 5 15 -' c '"' "- ~ -l <l 10 10 j "" ~ 00 0.5 1.0 1.5 2.0 25 ~ & 3.0 "' FL 0 0 Fig. 6 Distribution of FL Values and Their Accumulative Incidences, in Percentage, Comparing Liquefied Sites with Non-Liquefied Sites in Table 1 Non-Lq.Jefoction ELAPSED TIME ISEC.I Relationships between Pore Water Pressure and Acceleration of Non-Liquefied Sand Layers and FL Values in Shaking Table Tests Fig, 8 Uquefoction (•4) ·~~~~~~~~~ ~ § 0 ! ~ ~ ~ ~ 0~-L~~--~~~~~~~~~~~~~~~~~~~ .~ "5 10 ~ j 50 ~ ~ a ;j 30 0 100 Depth 0 ('%) Fig. 7 ~ Distribution of PL Values and Their Accumulative Incidences, in Percentage, Comparing Liquefied Sites with Non-Liquefied Sites in Table l SHAKING TABLE TESTS ON FL H [ 30CM 60CM BOCM l== 0 20 -' "- ~~ ' cig ;J'U 100 8 15 100 ~ ::::: <: 0 g. !? :30 ~ ------------ 1.0 50 "' <l 'lS ~ § ~ ;_ "" ~ l; l ~ I? ,.. .••../, ~ 80 Fig, 9 0 0 a; "i i ELAPSED Figs, 8 and 9 shows the relationships between ground acceleration, pore water pressure and FL for nonliquefied and liquefied test, respectively. In these figures, FL values were estimated by equations (2) and (3) based on test results, It can be seen that according to the increase of pore water pressure, FL values decrease to less than 1.0 in the liquefied layers (see Fig, 9) and on the other hand FL values are more than 1, 0 in the non-liquefied layers (see Fig, 8), ~ 0 0 flo The authors carried out shaking table tests to clarify the effectiveness of FL for assessing liquefaction potential of sandy soil. A loose saturated sandy ground model with about 0, 95 m depth, 6 m length and 3 m width was prepared on shaking table and shaked by sinusoidal wave, The frequency of the inputted motion was 7 Hz and the magnitude of the table acceleration ranged from 30 gals to 250 gals, The acceleration and pore water pressure of ground model during shaking were measured, 0 0 TIME ISEC.I Relationships between Pore Water Pressure and Acceleration of Liquefied Sand Layers and FL Values in Shaking Table Tests 214 Fig, 10 summarize the relation between F L and the rate of ground liquefaction, du/ <Jv' ( du: an excessive pore water pressure, Ov' an effective overburden pressure) for liquefied layers, FL decreases according to the increase in du/ oy', and on the average FL is less than 1.0 when,JU/Ov'is more than 0,5 andwhendu/ov'is 1,0, i, e,, the sand layer liquefy perfectly, FL decreases to less than about 0, 6. As mentioned in the above, it's been clarified in these shaking table tests that FL is adequately equivalent to the liquefaction phenomena and may be used to estimate the soil liquefaction potential of saturated sandy layers, I 0 I o \ 0 \ 0 \ \ \ ~ o\ ~~ 1.0 co \ \ ob, ' 0 0 0 ~---0 0 0.8 -----~---..;:..:.-~.:..--o- -- __o_o_g~-~~ _':-.._ ____f!__ ~ -:--0----- __ Kishida, H. (1970), "Characteristics of Liquefaction of Level Sandy Ground during the Tokachi-Oki Earthquake", Soils and Foundations, Vol.X, June, No.2, 0 0.6 Fig, 10 Japanese Society of Civil Engineers, "The Report on the Damage during the Niigata Earthquake of 1964" (in Japanese), Japanese Society of Soil Mechanics and Foundation Engineering ( 197 6), "Report on Earthquake Damage of Subground Streets and Structures, "March (in Japanese), oo '......., ,o BRI ( 1969), "Investigation on Liquefaction of Saturated Sand and Some Problems on Soil-Structure-Interaction, "The Building Research Institute, Ministry of Construction, No, 55 (in Japanese), 0 d\ 00 0 BRI (1965), "Report on Damage to Building during the Niigata Earthquake, "The Building Research Institute, Ministry of Construction, No, 42, 1965 (in Japanese), Ishihara, K, (1976), "Report of Liquefaction Tests of at the Site of Shinanogawa Water Gate, "Report to the Hokuriku Regional Construction Bureau, the Ministry of Construction (in Japanese), If 0 REFERENCES Relationships between FL Values and the Rate of Ground Liquefaction du/ Ov' in Shaking Table Tests CONCLUSIONS The simplified method based on the liquefaction resistance factor, FL and the liquefaction potential factor, PL proposed to assess the liquefaction potential was investigated by calculating the factors at 64 liquefied and 23 non-liquefied sites during past 6 Earthquakes in Japan and shaking table tests, From these studies, it was found that most values of FL are less than l, 0 at liquefied layers, and are larger than 1,0 at non-liquefied layers, Further, the values of PL and their incidences at liquefied sites differ from the ones at non-liquefied sites. Therefore, the liquefaction potential can be predicted reasonably by calculating the factors FL and PL , ACKNOWLEDGMENTS This study was greatly assisted by Dr, S, Yasuda, Kisojiban Consultants Co,, Ltd, and S, Yoshida also greatly assisted in conducting shaking table tests, The authors wish to express their thanks to them, Ohashi, M,, Iwasaki, T., Wakabayashi, S, and Tokida, K. (1977), "Statistical Analysis of Strong-Motion Acceleration Records", 9th Joint Meeting, U.S. -Japan Panel on Wind and Seismic Effects, U.J.N.R., May, Yasuda, S, and Tokida, K, (1980). "Soil Liquefaction Evaluation with use of Standard Penetration Resistances", Proc., 7th World Conference on Earthquake Engineering, Instanbul, Turkey Iwasaki, T. and Tokida, K, (1980), "Studies on Soil Liquefaction Observed During the Miyagi-ken Oki Earthquake of June 12, 1978", Proc,, 7th World Conference on Earthquake Engineering, Istanbul, Turkey, Kuribayashi, E. and Tatsuoka, F. (1977), "History of Earthquake - Induced Soil Liquefaction in Japan", Bulletin of Public Works Research Institute, Ministry of Construction in Japan, Vol. 31, Iwasaki, T,, Tatsuoka, F., Tokida, K, and Yasuda, S, (1978), "A Practical Method for Assessing Soil Liquefaction Potential Based on Case Studies at Various Sites in Japan", 2nd International Conference on Microzonation for Safer Construction Research and Application, pp. 885-896,
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