4
luther extensions to the Bishop 8c Morgenstezn slope stability charts RJ Chandler* and TA Peizinj s (118 I+ ~ ~ Is I I I ~ ~ i le imae ~ Qeameaeme eal 1'ean in ('u ir ~ I 1 ~ V ~ iul ( Sgiiil ieai.l 0 sM ~ 6 a ~asia Iaiai (igni aal tat 8 il IIae o leam> act 6 is m ~ ~ Yil i (in S I lan aTiTeaiiI eggs as ~ mgm we Bma 0 ia s. The design charts for the effective stress stabiTity analysis of slopes given by Bishop 8 Morgenstezn (1960)'nd O'onnor & Mitchell (1977) are extended to slopes of inclnation 0.5:1(horisontaLvertical) and values of the dimensionless stability factor c'/yH up to 0.15.The present results are shown to agree with those of the earlier workers, whose results, included here, enable slopes to be designed in the range of inclination O.S:1 to 5:1, for values of c'/yH =Oto0.16,andri'20 to40. Iatroduction Over the years the stabiTity charts presented by Bishop &Morgenstern (1960)have proved very valuable for the preliminary design of slopes in terms of effective stresses. The range of strength and slope inchnations that they considered was, however, limited to values of the stability coefficient c'/yH no greater than 0.0Sand slope inclinations in the range 2:1to 8:1(horisontaLvertical). The range of strengths was later extended by (YConnor 86 Mitchell (1977),who considered values of c'/yH up to 0.10. We have extended fuzther both the range of values of c'/yH (to 0.1S)and the slope incination(up to 0.5:1); following O'onnor &Mitchell we consider values of If('etween 20'nd 40 . The results are presented here in tabular fozm. This 'Depaztzrieztt of Civil Eztgineexiztg, hnpezial C(3Hegfg, London "'g llPE/ 63.ce sga 2:I- Bishop 6 Morgenstem u 3'1 (1960) ei =10 to ag 0 c u Sil- o 8 0 0 0.025 0.05 Values of c'/ YH d Connor Mitchell (1977) 6' 20'o 23. 60 16.3a Ia Ffg.l. 8lapelncllnatlans and values of c'/ylf caznddaredby the various authors. Unit weight of soil Y Urit weight ol water Y Pmaometric height h r ~ (tre ZY Efy'.2. D ttm<<ansofsyznbals usecL further extension of the method not only allows steeper slopes to be considered, but the higher values of c'/yH enable the design of slopes composed of relatively homogeneous soft rocks such as chalk and Keuper MarL The range of data which we provide is compared with those of the earlier publications in Efy; 1.We have included the results of Bishop & Morgenstern and O'onnor &Mitchell with our ownresults, so that the complete suite of stability coefficients is available to the potential user. Methods The analyses were canied out with a microcomputer, using the Bishop Simplified method for a circular arc failure suzface (Bishop 1988)s, programmed to locate the most critical failure surface. As described by Bishop &Morgerstern (1960),the Bishop Simplified equation for the factor of safety, F, maybe written in dimensionless terms. Thus F is dependant on the geometry of the particular problem. and on the parameters c'/yH, P'nd r where c'nd P're the effective stress strength parameters, y is the unit weight of the soil, H the vertical height of the slope and r„the average value of r„within the slope. The pore pressure parameter r„is de5ned incog. 2, as are the slope inclinat'on,(ti, and the depth factor, D. There is a linear relationship between F and r„for given values of c'/yH, P', P and D, which may be given (Bishop & Morgenstern 1960)as: F=m nr„ . (1) The mndts of the stabQity analyses may thus be expressed m terms of m and n. Our computations followed similar procedures to both Bishop 86Morgenstezn and O'onnor & MitchelL The former used 20 trial circular arcs to establish the critical arc, the latter 100. We used 24 (6 x 4 grid), guided by Spencer's observations (1967)gthat the contours of safety factor are approximately elliptical with their major axis normal to the surface of the slope, and that the centre of the critical arc is normally on or just upslope of the pezpendicular bisector of the slope. A check was made that a minimum value of F lay within the grid; where necessary, the calculations were repeated with anew grid location so that a minimum value of F was obtained. The values m and n in Eq.(1)were computed using a regression analysis applied to the F versus r„data. Bishop & Morgenstern and O'onnor & Mitchell canied out their computations using values of r„= 0, 0.3and 0.7;we used 0, 0.3and 0.6. We also investigated the inQuence of the choice of 20 or 40 as the number of slices used in the analysis on the resulting value ofF. For the case ofc'/yH = 0.100,D = 1.5, P = 4:1,with values of P'n the range 20'to 2:1 m n Oloifg ifadmafsfm 311 411 m n m 0 5:1 m 0 20' +0.1 +0.1 2 +OA +2.0 +1.0 +1.8 02 -1.1 30' +0.9 +2.8 0.8 -1.0 +0.3 +1.1 +0.3 +0.9 +0.1 +0.0 +0.3 +0.1 +0.4 +03 +0.4 +O.S +1.1 +2A +0.6 +1A +0.4 +2.0 1 +02 -02 0 +0.1 -0.2 -1.0 +1.2 +1.8 +0.6 +OA +0.2 0.7 +0.4 +0.8 Table 1.Differences(+ 96) ln values ofzn and n abtalned by (1) CYCennar*MtchaU (1972) and g) thfs paper, cenZpared with lmshop 00 Marffenstazn (1900), lo(r c'lylf = 0.09, D = 1.0. GROUND ENGINEERING MAY 1989 33

Further extensions to the Bishop & Morgenstern slope

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Page 1: Further extensions to the Bishop & Morgenstern slope

luther extensions to theBishop 8c Morgensteznslope stability chartsRJChandler* and TA Peizinj

s (118 I+~ ~ Is I I I ~ ~ i le imae ~ Qeameaeme eal

1'ean in ('u ir ~ I 1 ~ V ~ iul ( Sgiiil ieai.l 0 sM ~ 6 a

~asia Iaiai (igni aal tat 8 il IIae o leam> act 6 is m ~ ~

Yil i (in S I lan aTiTeaiiI eggs as ~ mgm we Bma 0 ia s.

The design charts for the effective stressstabiTity analysis of slopes given by Bishop8 Morgenstezn (1960)'nd O'onnor &Mitchell (1977) are extended to slopes ofinclnation 0.5:1(horisontaLvertical) andvalues of the dimensionless stability factorc'/yH up to 0.15.The present results areshown to agree with those of the earlierworkers, whose results, included here,enable slopes to be designed in the rangeof inclination O.S:1to 5:1,for values ofc'/yH

=Oto0.16,andri'20 to40.

IatroductionOver the years the stabiTity chartspresented by Bishop &Morgenstern(1960)have proved very valuable for thepreliminary design ofslopes in terms ofeffective stresses. The range of strengthand slope inchnations that theyconsidered was, however, limited tovalues of the stability coefficient c'/yH nogreater than 0.0Sand slope inclinations in

the range 2:1to 8:1(horisontaLvertical).The range of strengths was later extendedby (YConnor 86 Mitchell (1977),whoconsidered values ofc'/yH up to 0.10.

We have extended fuzther both the rangeofvalues ofc'/yH (to 0.1S)and the slopeincination(up to 0.5:1);followingO'onnor &Mitchell we consider valuesof If('etween 20'nd 40 .The results arepresented here in tabular fozm. This

'Depaztzrieztt of Civil Eztgineexiztg, hnpezialC(3Hegfg, London

"'g llPE/ 63.ce

sga

2:I-Bishop 6Morgenstem

u3'1 (1960)

ei =10 to ag

0cu Sil-o

800 0.025 0.05Values of c'/ YH

d ConnorMitchell(1977)6' 20'o

23. 60

16.3a

Ia

Ffg.l.8lapelncllnatlans and values ofc'/ylf caznddaredby the variousauthors.

Unit weight of soil YUrit weight ol water YPmaometric height hr ~ (tre

ZY

Efy'.2. D ttm<<ansofsyznbals usecL

further extension of the method not onlyallows steeper slopes to be considered,but the higher values ofc'/yH enable thedesign ofslopes composed of relativelyhomogeneous soft rocks such as chalkand Keuper MarL The range ofdata whichwe provide is compared with those of theearlier publications in Efy; 1.We haveincluded the results ofBishop &Morgenstern and O'onnor &Mitchellwith our ownresults, so that the completesuite of stability coefficients is available tothe potential user.

MethodsThe analyses were canied out with amicrocomputer, using the BishopSimplified method for a circular arc failuresuzface (Bishop 1988)s,programmed tolocate the most critical failure surface. Asdescribed by Bishop &Morgerstern(1960),the Bishop Simplified equation forthe factor of safety, F, maybe written in

dimensionless terms. Thus F is dependanton the geometry of the particular problem.and on the parameters c'/yH, P'nd rwhere c'nd P're the effective stressstrength parameters, y is the unit weight ofthe soil, H the vertical height of the slopeand r„the average value of r„within theslope. The pore pressure parameter r„isde5ned

incog.

2, as are the slopeinclinat'on,(ti, and the depth factor, D.

There is a linear relationship between Fand r„for given values of c'/yH, P', P andD, which may be given (Bishop &Morgenstern 1960)as:F=m —nr„ . (1)The mndts of the stabQity analyses maythus be expressed m terms of m and n.

Our computations followed similarprocedures to both Bishop 86Morgensteznand O'onnor &MitchelL The former used20 trial circular arcs to establish thecritical arc, the latter 100.We used 24 (6 x4 grid), guided by Spencer's observations(1967)gthat the contours of safety factorare approximately elliptical with theirmajor axis normal to the surface of theslope, and that the centre of the critical arcis normally on or just upslope of thepezpendicular bisector of the slope. Acheck was made that a minimum value of Flay within the grid; where necessary, thecalculations were repeated with anewgrid location so that a minimum value of Fwas obtained.

The values m and n in Eq.(1)werecomputed using a regression analysisapplied to the Fversus r„data.

Bishop &Morgenstern and O'onnor &Mitchell canied out their computationsusing values ofr„=0, 0.3and 0.7;we used0, 0.3and 0.6.

We also investigated the inQuence of thechoice of 20 or 40 as the number of slicesused in the analysis on the resulting valueofF.For the case ofc'/yH = 0.100,D = 1.5,P = 4:1,with values ofP'n the range 20'to

2:1m n

Oloifg ifadmafsfm

311 411

m n m 05:1

m 0

20' +0.1 +0.12 +OA +2.0

+1.0 +1.8 —02 -1.1

30'+0.9 +2.8 —0.8 -1.0

+0.3 +1.1+0.3 +0.9

+0.1 +0.0 +0.3 +0.1 +0.4 +03 +0.4 +O.S+1.1 +2A +0.6 +1A +0.4 +2.0

1 +02 -02 0 +0.1 -0.2 -1.0+1.2 +1.8 +0.6 +OA +0.2 —0.7 +0.4 +0.8

Table 1.Differences(+ 96)ln values ofzn and n abtalned by (1)CYCennar*MtchaU(1972) and g) thfs paper, cenZpared with lmshop 00 Marffenstazn (1900),lo(r c'lylf = 0.09, D = 1.0.

GROUND ENGINEERING MAY 1989

33

Page 2: Further extensions to the Bishop & Morgenstern slope

100-

80-H

(m) Usingeo- stability

coefficients

40-

(19/ 8),kPa,0.15m~

Table 2.c'/yH = 0; am vnlnea ofD.

Qopo 0.5:1 I:I 2:1m n m n m n

20'.182 0.910 0.364 0.728 0.728 0.91025'A3 1.166 OA66 0.933 0.933 1.16630'A9 1.443 0577 I.ISS 1.1$S 1.4433P OAO 1.7Sl 0.7N 1ASS IAN 1.75141P 0.420 2.NS O.N9 1.670 1.678 2.098

3:1m n

4:1m n

5:1m n

1.092 1.213 1.45d 1.547 1.820 1.8921.399 1554 1.865 1.982 2.332 2.4241.732 1.924 2.309 2.454 2.N7 3.Nl2.101 2.334 2.Nl 2.977 3.501 3.6392317 2.797 3.3S6 3.S66 4.196 4.362

20-cot (1

3:1 2.1 1:1 0.5:1 0.25:1I I I I I I I I

O 2O 40 eO 8O.Slope inclination, P

Hg.3. Cosuyns&on ofaloye beft7btveranafnclfnatfonrelatfonabl$ sdcalcnlatedby different tnethoda; carveJrnm Chandler(1 ON).

34

TaMe3. c'/yH= 0.2$;D = J.OO

Slope 0$nl 1:1m n m n

20'5230.733 0.707 0.76425'306 0.740 OAL39 0.97430'.667 OAI7S 0.9N 1.20235'.755 1.010 1.142 1.454OAIS7 1.1N 131S 1.731

2:Im n

3:1m n

4:1m n

5:1m n

1.124 1.022 1342 1.347 1.962 I.d98 2.380 2 NO1.356 IA2 1$75 1.69d 2AN Z 141 2.921 Zdftd1.606 1.567 2AS 2.078 2A73 2622 3300 Z 1911.NO 1.NS 2.Q5 2.505 3.396 3.160 4.1Sd 3,0492.190 2.247 3.090 2.993 3.904 3.778 4.NS 4.$92

TaMe4 c'lyH = O.2OJD = J.2O

Qopo ILS:1 1:1m n m h

20'.996 0.943 I AI76 1.N625' Ad 'I.'198 IAS IAI

1A72 IAN IA02 IA3135'.737 1.773 1.9051.974N'345 2.118 L$12 L362

2:Im n

3:I 4:Im n

5:1m n

1%9 1216 1.610 1.478 1,961 1.775 2.334 2.0901A19 1547 2.007 1.091 2A37 2269 X$97 2.6691.9S6 1.915 2A31 2.342 2.9Q LN6 3811 3~LNI 2AI 2.901 2.841 3824 3AN 1.191 3.9902.7Q 2.77$ 3A31 3.399 1.164 4A64 4.950 4704

TaMe$.c'lyH O.OOOJD = J.OO.

Qopo OA:I 1:Ih' h

20'ASS 0.7N 0.9'12 LSI02S'L797 'IAOI

IAIDO

1.04230'L9N 1117 1A2 1&735' A02 IA17 1&9 IA69417 1.140 IA17 1859 1.7SS

2:1m h

3illn h

4:Im n

5:Im n

1AO 1AI71 IA40 1.307 2A3 1.776 2.7N ZOP I1A24 IAS 2.193 1.7$7 L770 Z211 3A6 Z651IAS IA30 L574 Z 1$7 3&1 Zd93 3.934 3A'$92.1701.9$0 2.990 Z$92 3A03 MQ 4897 3.9272505 L332 3A51 3.071 4A25 Z Sl 5344 444$

TaMeO.c'/yH= O.OOOlD= J.2O.

Qopo OA:I I:1m n m h

20'.172 0.9N ILQ I.N425' A05 1&2 1809 1A330'IA$ 6 18101.7N 1.66930'.935 IA30 2AN7 2A074; X245 2.174 2A29 L390

2:Im n

3:Im n

4:Im n

Silm n

TaMe1.c'/yH= O.OOOJD= J.OO

Qopo 05:I lilm n m n

20'A91 IA9 1861 1%325'426 1A37 1.910 1.7N2.187 LOIS $207 2.10135'507 2A36 2.704 X$41N'A40 2.915 3.17$ 3AS6

2:1m n

3:Im n

41m n

5:Im n

1.752 IAOI L011 1.705 L337 1.993 2AOS L2N2.143 1.903 2A67 2.179 X$67 LQ4 3302 2.902ZSN L342 2.964 2A96 3A43 3.120 3.967 3A773ANI 2832 351S 3'AI2 3.771 4.707 4AS3874 3A9 4136 3.91S 4803 4807 5543 5.171

GROUND ENGINEERING MAY 1989

1509 I~ IAd 1.193 2.230 1.799 2A43 2.107%22 1895 $222 I897 2.705 2.2S7 3211 Zd902.1dl 1.9SO 2A45 2.342 3AI 2419 3A9 3,3242535 L344 3.114 LN9 3.79S 3.413 4811 4,0252.9Q 2.791 3A42 3AOS 4A42 4.090 5&3 4406

40'andr„to values of 0, 0.3and 0.6, thevariationin factor of safety lay between 0and 1.63%(average 0.4%).In everyinstance the value of Fobtained with 30shces was the lower. We subsequentlyused 30 slices for aU our analyses, so thatin that respect our results wiU yieldmarginally conservative values ofF.

ComI$ arlsoawith yrevious resultsO'onnor 4MitcheU compared theirresults with Bhahop 8 Morgenstern's forc'/yH = 0.06andD = 1.00,andwehavedone the same. The results ot thiscomparison are ahownin TaMe J,expressed as percentage differencesfrom the original

Bishop'sMorgensternm

and n values. O'onnor 8c Mitchell's resultsshow slightly ckeer agreement withBishop 8c Morgenstern's than do ours, withtheir values ofm andnbeing on average0.38%higher, while our results average0.78%higher. The use ot such values inEq.(1)wiU result in a correspondingpercentage increase inF compared withthe other worker's results. Theseditferences are sufficiently small to be ofno practical importance.

It is also possible to compare, indirectly,our results with those ofTaylor (I846)s.Chandler (1884) used Taylor'0 work toconstruct aslope height versus inclinationrelationship tor aslope having the soilproperties c'0kPa, (ti' 34', f„0.16and y = 33kw/ms, obtaining therelationship ahowninRfg.2. Ourextension ot the Bishop 4 Morgenaternresults enable this relationship, whichinvolves slope incinathna in the range 1:1to 0.6:1,tobe checked. It is seen that thecaicuINed points agree extremely weUwiththe relationship obtained from

Taylor'ada'reseatioa

ofresultsIn the tables that foUow (Tablee2te JO),we present reauha ofour computations, towhich we have added for the user'a

Page 3: Further extensions to the Bishop & Morgenstern slope

convenience the results obtained byBishop &Morgenstern and O'onnor &Mitchell We are thus able to give thestabiTity coefficient for slopes in the range0.5:1(P= 64') to 1:5(P= 11.3'),for valuesofc'/yH = 0to0.15,and/' 20'to40'.

As Bishop &Morgenstern pointed out

(p 136),for the special case where c' 0the failure surface is a plane parallel to theslope surface (the Minite slope'ase) and

F = tang'(1 —r„sec'P)/tang ...(2)

Thus m and n (TaMe 3)may be easilyevaluated as m = tan 46'/tanP, andn = m sec'Itl.

The previous authors presented theirresults in both tabulations and in chartform. We believe that the tabulations areused far more frequently than the charts,and therefore only include the tabulations.A particular benefit of the charts is that it ispossible to show (for given values of/, 46',c'/yH and D) contours ofvalues ofr„(r+which yield the same value ofF for valuesofD = 1.00and 1.25;and also for D = 1.25and 1.50.The value of r„used for designcan then be compared with thecorresponding value ofr, to provide animmediate indication whether or not thereis a more critical deeper slip surface. Thisis not so conveniently achieved withtables, but a partial solution, followedhere, is outlined in the following section.

Use of tablesThe tables give values of m and n to beinserted in the equationF=m —nr„ (1)to obtain the factor of safety, F, of the slopefor given values of c'/yH, P', r„and slopeinclination/, all ofwhich are defmed inFldf.2. A method for obtaining a value ofr„within the slope for use in Eq.1 is given byBishop &Morgenstern(1960).

For values ofn appearing in the tables initalics there is the possibility of a deeper,more critical failure surface if the designvalue ofr„isequal to or less than 0.5.Theuser should then check this possibility,using the table giving the next highestvalue of D for the same value of c'/yH. It isalso possible that a deeper critical surfacemay exist where the design r„is greaterthan 0.5.No indication of this is given in thetables, so the user should also check thispossibility at higher values of D. Thisproblem does not occur when c' 0(TaMe 2);nor, as is often the case, when astronger stratum lies at or close to the baseof the slope.

TaMe$.c'/yH= O.OZ$;D= 1.OO.

03:1m n

1:1m n

2:1m n

3:1m n

4:1m n

5:1m n

20'5o

30'5'0'3145

O.NO 1.088 0.837 1.610 1.1N 2.141 1.443 2.664 1.801 3.173 Z 1300.950 1.013 1245 1.053 1.872 1.386 2.502 1.8153.12d Z2$9 3.742 2.71$1.064 1238 1.416 1296 2.142 1.N6 2.884 2201 3.623 2.7$S 4.357 3.3311.190 1.485 1.605 1564 2.443 2.030 3.306 24$9 4.177 3.331 5.024 4.N11.332 1.762 1.798 1.824 2.772 2.386 3.775 3.14$ 4.785 3.94$ 5.77d 4.7$9

TaMe O. c'lyH = O.OZ$;D = 1.2$

05:Im n

1:1m n

2:1m n

3:1m n

4:1m n

5:1m n

20'5o

30'5'IP

TaMe lO. c'/yH = O.O?$;D = J.$0.

05:Im n

1:1m n

2:1 3:1m n

4:1m n

5:1m n

20'50

30'5'0'.637

1.305 1.706 1.349 1.918 1.514 2.199 1.728 2.548 1.985 2.931 2.2721.977 1.663 2.052 1.708 2.308 1.914 2.660 2.2N 3.083 2.530 3.552 2.9152.340 2.041 2.426 2.1N 2.735 2.3SS 3.158 2.714 3.d59 3.128 4.218 3.5852.741 2.459 2.841 2.537 3211 2.854 3.708 3.285 4.302 3.786 4.961 4.3433.193 2.931 3.310 3.031 3.742 3.397 4.332 3.926 5.026 4327 5.788 5.185

TaMe II.c'lyH= O.IOOID = l.OO.

Slope 0.5:1 1:1 2:1m n m n m n

3:1m n

4:1m n

5:1m n

20'50

30'5'0'.993

0.797 1.263 0.871 1.841 1.M3 2.421 L472 2.982 1.8153.549 2.1$71.106 1.025 1.422 1.078 2.102 L430 2.785 LS4$ 3.358 Z303 4.131 2.7431222 '1.259 1.592 1.306 2.378 1.714 3.183 Z2$8 3.973 ZS30 4.751 3.3721.347 1.508 1.781 1.57d 2.692 2.086 3.612 2.71$ 4.516 3.3$9 5.426 4.8$91.4N 1.7N 1.995 1.879 3.025 2.445 4.103 3.230 5.144 4.N1 6.187 4.831

TaMe 12.c'/yH = O.MO; D = 1.2$.Slope 0.5:1 1:1

m n m n

2:1m n

3:1m n

4:1m n

5:1m n

20'50

30'5'0'.489

1.036 1.529 1.095 13174 1.301 2.283 1.558 2.751 ES43 3.2531.735 1.313 1.799 1.394 2.197 1.642 2.681 1.972 3.233 2.330 3.8331.997 1.602 2.091 1.718 2540 2.0N 3.112 2.415 3.753 2.8$8 4.4512280 1.908 2.414 2.076 2.922 2.415 3.5N 2.914 4.333 3.458 5.1412597 2.253 2.763 2.453 3.345 2.855 4.119 3.457 4.987 4.142 5.921

2 1$82.7SS3.3724.0724.872

TaMe13. c'lyH = O.lOOID = 1.$0.

Slope 0.5:1m n

1:1m n

2:1m n

3:1m n

4:1m n m

5:1

20'5o

30'5'0'.778

1.314 1.863 1.371 2.079 1.528 2.387 1.742 2.768 2.014 3.1582.119 l.d74 2211 1.732 2.477 1.942 2.852 2.215 3.297 2.542 3.7962.489 2.063 2.586 2.122 2.908 2.385 3.349 2.728 3.881 3.143 4.4682.N2 2A84 3.0N 2.553 3.385 2.884 3.900 3.3N 4.520 3.NO 5.2113.347 2.957 3.469 3.04d 3.924 3.441 4.524 3.941 5.247 4.542 6.040

2.2852.9273.6144.3725.2N 37

GROUND ENGINEERING . MAY 1989

1.336 1.023 1.387 I.N7 1.688 1.285 2.071 1.543 2.492 1.S1$ 2.954 2.1731.575 1.284 1.656 1.386 2.N4 1.641 2.4d9 1.957 2.972 Z31$ 3.523 2.7301.NO 1.560 1.943 1.701 2.352 2.015 2.NO 2.385 3.499 2.857 4.149 X3$72.109 1.865 2.245 2.025 2.728 2.385 3.357 2.870 4.079 3.4S7 4.831 4.0432.424 2.210 2.5N 2.403 3.154 2.841 3.889 3.428 4.729 4.128 S.N3 4.830

Page 4: Further extensions to the Bishop & Morgenstern slope

TaMe14. c'/yH= 0.12S;D = 1.00.

Slope

20'5030'5'0'.5:1

1:1m n m n

2:1m n

3:1m n

4:1m n

5:1m n

1.121 O.N8 1.425 0.881 2.042 1.148 2.689 1.$41 3.263 1.784 3.868 2.1241.254 1.051 1.596 1.112 2.323 1.447 3.062 L9N 3.737 2.271 4.446 27211.37d 1.267 1.769 1.337 2.618 1.777 3.457 2.298 4253 2.S10 5.073 3.3681.505 1.530 1.956 1.586 2.929 2.115 3.880 2.7054.823 3.407 5.767 4.0481.612 1.743 2.171 1.891 3.272 2.483 4.356 3.1S3 5.457 4.NB 6.551 4.893

Table 1$.c'/yH = 0.12$;D = 1.2$.Slope

2(P25o

30'5'0'$

:I 1:1m n m n

2ilm n

3:1m n

4:1m n

5:1m n

1.642 1.057 1.671 1.102 2.054 1.324 2.492 1.$79 2.983 1.8d1 3.496 2.1671.8N 1.326 1.941 1.402 2.377 1.671 2.894 1.993 3.481 2.379 4.078 2.7$32.156 1.626 2.234 1.727 2.727 2.042 3.324 2.431 4.009 2.91d 4.712 3.40$2.447 1.948 2.557 2.085 3.110 2.452 3.801 2.928 4.586 3.$N 5.414 4.12S2.767 2.295 2.922 2.490 3.542 2.913 4.338 3.494 5.237 4.161 6.207 4.94$

TaMe16. c'/yH = 0.12$;D = 1.$0.

Slope

20'$0

30'5'0'$

:1 1:1ni n m n

2:1m n

3ilnl h

4ilm n

5:1m n

1.920 1.322 2.015 1.385 2.234 1.545 2.565 1.749 2.963 2.N4 3.400 2.287

2.261 1.683 2.3N 1.754 2.638 1.972 3.028 2.229 3.5N 2.550 4.019 2.9132.631 2.073 2.745 2.145 3.072 2.425 3.529 2.749 4.083 3.149 4.692 3.5983.039 2.504 3.160 2.577 3.549 2.923 4.084 3.324 4.727 3.813 5.436 4.3623.497 2.982 3.628 3.065 4.N9 3.485 4.712 3.980 5.456 4.566 6.278 5.226

TaMe 17.c'/yH= 0.1$0;D= 1.00.

Slope 0.5rl 1:1m h nl h

2:1m n

3:1m n

4:1m n

5:1nl h

20'5o

30'5'0'.248

0.813 'I.585 0.886 2.261 1.170 2.895 1.448 3.579 LNd 4230 2.159

1.386 1.034 1.761 1.126 2.536 L4d2 3.259 1.S14 4.052 22N 4.817 Zld51525 1.260 1.944 1.370 2.836 1.791 3.657 2.2454567 2.S11 5.451 3.4161.660 1.539 2.134 1.619 3.1dl 2.1$3 4.098 2.721 5.137 3.4N 6.143 4.1171.NS 1.832 2.346 1.901 3.512 2.535 4.597 3.2$8 5.782 4.NB 6.913 4.8N

TaMe 16.c'/yH = 0.1SO;D = 1.2$.Slope 0.5:1

m n

1:1m n

2:1nl h

3:1nl h

4:1m n

5:1m n

20'50

30'5'0'aMe10.

c'/yH= 0.1$0; D = 1.$0.

0.5:1m n

1:1 2:1m n m n

3:1m n

4:1m n

5:1m n

1.796 1.079 1.813 1.107 2.229 1.334 2.701 LBN 3.225 1.873 3.780 2.182

2.042 1.344 2.083 1.409 2.560 1.692 3.107 2.0153.724 2.384 4.363 2.7692.309 1.639 2.377 1.734 2.909 2.065 3.542 2.464 4.262 2.941 5.995 X406

2.NS 1.971 2.700 2.094 3295 2.475 4.018 2.946 4.846 3.$34 5.697 4.129

2.934 2.335 3.066 2.449 3.728 2.938 4.556 3.509 5.498 4.1956.490 4.947

Linear interpolation may be used, withoutsignincant loss of accuracy, forcalculations involving intermediate valuesofc'/yH, IJ) 'nd cotti.

Worked exampleThe example chosen is that used byBishop &Morgenstern (1960),an earthslope for which the relevant designparameters are P' 30', c'/yH = 0.035,r„=0.5,and which has a slope inclinationcottJ = 4:l.

Referring to TaMe 3(c'/yH = 0.025;D = 1.00),it is seen that the value ofn,2.622, is shown in italics. Since the designvalue of r„(0.5)lies just within the range 0.5to 0, there will be a deeper more criticalfailure surface. Thus it is necessary to turnto TaMe 4(c'/yH = 0.025, D = 1.25).Thisgives m = 2.953,n = 2.806, which whensubstituted into Eq. 1, along with r„=0.5,yields F = 1.550.

Similarly, from TaMe S(c'/yH = 0.050,D = 1.00)a deeper more critical failuresurface is again indicated. Thus Table 6(c'/yH = 0.050,D = 1.25)givesm = 3.221,n = 2.819,and Eq. 1 yields F = 1.812.

Interpolating linearly for c'/yH = 0.035givesF = 1.550+ 0.4 x 0.262

= 1.65.

AcknowledgementsWe are grateful to the Institution of CivilEngineers and the Canadian GeotechnicalJournal for aQowing us to reprint theresults previously obtained by Bishop &Morgenstern and O'onnor &Mitchell.

References1.Bishop, AW and Morgenstern, NR (1960).Stabilitycoefficients for earth slopes. Gdotechnigue 10, 129-150.2. O'onnor, MJ and Mtchell, RJ (1977).An extensionof the Bishop &Morgenstern slope stabiTity charts.Canadian Georechnical Journal 14, 144-151.3.Bishop, AW (1955).The use of the slip circle in thestability analysis of slopes. Gdotechnigue 5, 7-17.4.Spencer, E (1967).A method ofanalysis ofthestabiTity ofa~cuts assuming parallel intersliceforces. Gdotschnique 17, 11-26.S.Taylor, DW (1948).Fundamentals of soil mechanics.New York, Wiley. (pp4S6-462).6.Chandler, RJ (1984).Recent European experience oflandslides in overconsoiidated days and soft rocks.Proc 4th lnt Symposium on Landslides, 1,61-6l.

38

20'5o

30'5'0'.061

1.335 2.1642.402 1.691 2.5202.772 2.N2 2.9023.181 2.514 3.3193.643 3.0N 3.788

1.391 2.394 1.550 2.748 1.756 3.174 2.020 3.641 2.3081.768 2.798 1.978 3.212 2.237 3.711 2.561 4.259 2.9242.168 3.236 2.441 3.718 2.758 4.293 3.156 4.931 3.6042.6N 3.715 2.940 4.269 3.333 4.938 3.819 5.675 4.3643.0N 4.255 3.503 4.896 3.983 5.667 4.569 6.517 5.228

GROUND ENGINEERING MAY 1989