bearing capacity comparison

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Delivered by ICEVirtualLibrary.com to: IP: 212.118.15.110 On: Fri, 10 Jun 2011 06:57:30 White, D. J., Teh, K. L., Leung, C. F. & Chow, Y. K. (2010). Ge ´otechnique 60, No. 2, 147–149 [doi: 10.1680/geot.8.D.024] 147 DISCUSSION A comparison of the bearing capacity of flat and conical circular foundations on sand D. J. WHITE, K. L. TEH, C. F. LEUNG and Y. K. CHOW (2008) Ge ´otechnique 58 , No. 10, pp. 781–792 T. Orr , Trinity College Dublin, Ireland The authors have presented an interesting paper concern- ing a fundamental problem for geotechnical engineers: the bearing capacity of circular foundations on sand. In this paper the authors have included an equation for the factor N ª in the bearing capacity equation for circular foundations on the ground surface, which has been determined from the results of centrifuge tests. The authors’ paper is particularly relevant at this time as the new European Standard for Geotechnical Design, EN 1997-1: Eurocode 7 Geotechnical Design (CEN, 2004) is due to be implemented in March 2010 by the national standards organisations in the member countries of the Comite ´ Europe ´en de Normalisation (CEN). EN 1997-1 provides the principles for geotechnical design as code text and some calculation models in informative annexes, that is not as mandatory code text. One of these calculation models is an analytical method for calculating the bearing capacity of a spread foundation. As no exact solution exists for N ª ,a number of equations have been proposed for N ª since the bearing capacity equation was first introduced by Terzaghi (1943). The equation in EN 1997-1 for N ª for a strip foundation with a rough base is N ª ¼ 2( N q 1) tan ö9 (7) where N q ¼ e ðtanö9 tan 2 (45 þ ö9=2) (8) This equation for N ª was obtained by Vesic (1973) and is based on the equation for N q in EN 1997-1, which was originally derived by Prandtl (1920). This later equation is an exact solution. From the results of centrifuge model tests the authors provide the following equation for N ª for a circular founda- tion with a flat rough base N ª ¼ 0 : 0286e 0 : 2109ö9 (2) It should be noted that this equation for N ª is for a circular foundation and hence differs from the N ª equations reported by most other authors, which are for strip foundations. An additional shape factor, s ª is traditionally applied to N ª to account for the foundation shape. A number of papers about the bearing capacity of spread foundations on sand have been published in Ge ´otechnique over the years, for example Meyerhof (1951), De Beer (1970), Cassidy and Houlsby (2002) and Lyamin et al. (2007). Some of the equations that have been proposed for N ª and that differ from the EN 1997-1 equation, include N ª ¼ 1 : 5( N q 1) tan ö9 by Brinch Hansen (1970) (9) N ª ¼ ( N q 1)tan(1 : 4ö9) by Meyerhof (1963) (10) Martin (2005) used the method of characteristics to obtain what he stated appear to be exact solutions for N ª for various design situations. Salgado (2008) proposed the fol- lowing equation that provides a good fit to Martin’s results N ª ¼ ( N q 1)tan (1 : 32ö9) (11) According to Smoltczyk (U. Smoltczyk (2008), personal communication), equation (7) was adopted for N ª in EN 1997-1 because it had been used in DIN 4017 as an updating of earlier approximations, such as Brinch Hansen’s (1970) equation, on the basis of large-scale tests on sand carried out by DEGBO in Berlin (Muhs, 1971). The authors’ equation for N ª for a circular foundation can be converted to an equation for N ª for a strip foundation by applying the following shape factor correction proposed by Lyamin et al. (2007) s ª ¼ 0 : 0336ö9(1 þ 0 : 002ö9) (12) so that N ª (strip) ¼ 0 : 0286e0 : 2109ö9=(0 : 0336ö9(1 þ 0 : 002ö9)) (13) The N ª values for a strip foundation for ö9 ranging from 208 to 408 obtained using the authors’ converted equation (13) together with those obtained using the EN 1997-1 equation and the Meyerhof, Brinch Hansen and Salgado equations are tabulated in Table 3 and plotted in Fig. 11 for comparison. The N ª values in Table 3 and Fig. 11 show that, for a strip foundation for 20 8 < ö9< 40 8 (a) the EN 1997-1 N ª values exceed all the other predicted N ª values and hence, as previously shown by Orr (2008), are unconservative. For example, the EN 1997-1 N ª value exceeds the authors’ value by 41% for ö9 ¼ 20 8 , reducing to 27% for ö9 ¼ 40 8 (b) the authors’ values are very similar to Meyerhof’s values (c) Salgado’s values based on Martin are similar to Brinch Hansen’s values and are more conservative than the authors’ values for ö9. 30 8 . In the case of a circular foundation, the authors’ N ª values are compared with the EN 1997-1 values obtained by multi- plying equation (7) by the EN 1997-1 shape factor for a circular foundation, which is s ª ¼ 0 . 7. These N ª values are also given in Table 3 and plotted in Fig. 12. Fig. 12 shows that for 20 8 < ö9< 40 8 , the EN 1997-1 N ª values for a circular foundation exceed the authors’ values for ö9, 27 . 5 8 , for example by 42% for ö9 ¼ 20 8 , but are less than the authors’ values for ö9. 27 . 5 8 , for example by 44% for ö9 ¼ 40 8 . These differences for circular foundations are not as significant as those for strip foundations because for ö9. 27 . 5 8 they are conservative, while for values of ö9, 27 . 5 8 , although they are unconservative, they are not normally relevant for foundations on sand. The comparison between the authors’ and EN 1997-1 N ª values for both circular and strip foundations shows that significant differences can occur and that the EN 1997-1

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Page 1: Bearing Capacity Comparison

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White, D. J., Teh, K. L., Leung, C. F. & Chow, Y. K. (2010). Geotechnique 60, No. 2, 147–149 [doi: 10.1680/geot.8.D.024]

147

DISCUSSION

A comparison of the bearing capacity of flat and conical circularfoundations on sand

D. J. WHITE, K. L. TEH, C. F. LEUNG and Y. K. CHOW (2008) Geotechnique 58 , No. 10 , pp. 781 – 792

T. Orr, Trinity College Dublin, IrelandThe authors have presented an interesting paper concern-

ing a fundamental problem for geotechnical engineers: thebearing capacity of circular foundations on sand. In thispaper the authors have included an equation for the factorNª in the bearing capacity equation for circular foundationson the ground surface, which has been determined from theresults of centrifuge tests.

The authors’ paper is particularly relevant at this time asthe new European Standard for Geotechnical Design, EN1997-1: Eurocode 7 Geotechnical Design (CEN, 2004) isdue to be implemented in March 2010 by the nationalstandards organisations in the member countries of theComite Europeen de Normalisation (CEN). EN 1997-1provides the principles for geotechnical design as code textand some calculation models in informative annexes, that isnot as mandatory code text. One of these calculation modelsis an analytical method for calculating the bearing capacityof a spread foundation. As no exact solution exists for Nª, anumber of equations have been proposed for Nª since thebearing capacity equation was first introduced by Terzaghi(1943). The equation in EN 1997-1 for Nª for a stripfoundation with a rough base is

Nª ¼ 2 (Nq � 1) tan �9 (7)

where

Nq ¼ e�tan�9tan2 (45 þ �9=2) (8)

This equation for Nª was obtained by Vesic (1973) and isbased on the equation for Nq in EN 1997-1, which wasoriginally derived by Prandtl (1920). This later equation isan exact solution.

From the results of centrifuge model tests the authorsprovide the following equation for Nª for a circular founda-tion with a flat rough base

Nª ¼ 0:0286e0:2109�9 (2)

It should be noted that this equation for Nª is for a circularfoundation and hence differs from the Nª equations reportedby most other authors, which are for strip foundations. Anadditional shape factor, sª is traditionally applied to Nª toaccount for the foundation shape. A number of papers aboutthe bearing capacity of spread foundations on sand havebeen published in Geotechnique over the years, for exampleMeyerhof (1951), De Beer (1970), Cassidy and Houlsby(2002) and Lyamin et al. (2007). Some of the equations thathave been proposed for Nª and that differ from the EN1997-1 equation, include

Nª ¼ 1:5 (Nq � 1) tan �9 by Brinch Hansen (1970) (9)

Nª ¼ (Nq � 1)tan(1:4�9) by Meyerhof (1963) (10)

Martin (2005) used the method of characteristics to obtainwhat he stated appear to be exact solutions for Nª for

various design situations. Salgado (2008) proposed the fol-lowing equation that provides a good fit to Martin’s results

Nª ¼ (Nq � 1)tan (1:32�9) (11)

According to Smoltczyk (U. Smoltczyk (2008), personalcommunication), equation (7) was adopted for Nª in EN1997-1 because it had been used in DIN 4017 as anupdating of earlier approximations, such as Brinch Hansen’s(1970) equation, on the basis of large-scale tests on sandcarried out by DEGBO in Berlin (Muhs, 1971).

The authors’ equation for Nª for a circular foundation canbe converted to an equation for Nª for a strip foundation byapplying the following shape factor correction proposed byLyamin et al. (2007)

sª ¼ 0:0336�9(1 þ 0:002�9) (12)

so that

Nª(strip) ¼ 0:0286e0:2109�9=(0:0336�9(1 þ 0:002�9))

(13)

The Nª values for a strip foundation for �9 ranging from 208to 408 obtained using the authors’ converted equation (13)together with those obtained using the EN 1997-1 equationand the Meyerhof, Brinch Hansen and Salgado equations aretabulated in Table 3 and plotted in Fig. 11 for comparison.The Nª values in Table 3 and Fig. 11 show that, for a stripfoundation for 208 < �9 < 408

(a) the EN 1997-1 Nª values exceed all the other predictedNª values and hence, as previously shown by Orr(2008), are unconservative. For example, the EN 1997-1Nª value exceeds the authors’ value by 41% for�9 ¼ 208, reducing to 27% for �9 ¼ 408

(b) the authors’ values are very similar to Meyerhof’svalues

(c) Salgado’s values based on Martin are similar to BrinchHansen’s values and are more conservative than theauthors’ values for �9 . 308.

In the case of a circular foundation, the authors’ Nª valuesare compared with the EN 1997-1 values obtained by multi-plying equation (7) by the EN 1997-1 shape factor for acircular foundation, which is sª ¼ 0.7. These Nª values arealso given in Table 3 and plotted in Fig. 12. Fig. 12 showsthat for 208 < �9 < 408, the EN 1997-1 Nª values for acircular foundation exceed the authors’ values for�9 , 27.58, for example by 42% for �9 ¼ 208, but are lessthan the authors’ values for �9 . 27.58, for example by 44%for �9 ¼ 408. These differences for circular foundations arenot as significant as those for strip foundations because for�9 . 27.58 they are conservative, while for values of�9 , 27.58, although they are unconservative, they are notnormally relevant for foundations on sand.

The comparison between the authors’ and EN 1997-1 Nª

values for both circular and strip foundations shows thatsignificant differences can occur and that the EN 1997-1

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equation may be significantly unconservative, particularlyfor strip foundations and for low �9 values. Cassidy andHoulsby (2002), based on numerical modelling of circularfoundations, came to a similar conclusion for �9values , 308. Hence, when national standards organisationsare deciding whether or not to adopt the EN 1997-1 calcula-tion model for bearing resistance in their national annexesand when geotechnical engineers are designing foundation toEN 1997-1, they should be aware of the differences betweenthe various predicted and measured Nª values. The authors’paper is a helpful and timely contribution in this regard.

REFERENCESBrinch Hansen, J. (1970). A revised and extended formula for

bearing capacity. Bulletin No. 28, Danish Geotechnical Institute,Lyngby.

Cassidy, M. J. & Houlsby, G. T. (2002). Vertical bearing capacityfactors for conical footings on sand. Geotechnique 52, No. 9,687–692.

Comite Europeen de Normalisation (2004). EN 1997-1: Eurocode 7geotechnical design. Part 1 : general rules. CEN, Brussels.

De Beer, E. E. (1970). Experimental determination of the shapefactors and the bearing capacity factors of sand. Geotechnique20, No. 4, 387–411.

Lyamin, A. V., Salgado, R., Sloan, S. W. & Prezzi, M. (2007). Two-and three- dimensional bearing capacity of footings in sand.Geotechnique 57, No. 8, 647–662.

Martin, C. M. (2005). Exact bearing capacity calculations using themethod of characteristics. Proc. 112th Int. Conf. IACMAG, Turin4, 441–450.

Meyerhof, G. G. (1951). The ultimate bearing capacity of founda-tions. Geotechnique 2, No. 4, 301–332.

Meyerhof, G. G. (1963). Some recent research on bearing capacityof foundations, Can. Geotech. J. 1, No. 1, 16–26.

Muhs, H. (1971). Die experimentelle Untersuchung der Grenztrag-fahigkeit nichtbindiger Boden bei lotrechter Belasatung. DEG-BO-Mitteilungen, Vol. 27, DEGBO, Berlin.

Orr, T. L. L. (2008). Eurocode 7 and geotechnical models. Von derForschung zur Praxis, Symposoium anlassich des 80. Geburt-stags von Prof. U. Smoltczyk, (ed. P. A. Vermeer), pp. 187–207.Institut fur Geotechnik der Universitat Stuttgart.

Prandtl, L. (1920). Uber die Harte plastischer Korper. Nachrichtender koniglichen der Gesselschaft der Wissenschaft Gottingen,Math-Phys. Kl., No. 12, 74–85.

Salgado, R. (2008). The engineering of foundations. London:McGraw Hill.

Terzaghi, K. (1943). Theoretical soil mechanics. Wiley, New York.Vesic, A. S. (1973). Analysis of ultimate loads of shallow founda-

tions. J. Soil Mech. Found. Div., ASCE 99, No. SM1, 45–73.

Authors’ replyWe thank the discusser for his interest in our paper. Thediscussion is concerned with the expression for the bearingcapacity factor Nª for rough circular footings that weprovided (equation (2) in both the original paper and thediscussion). It highlights the difference between this andother published solutions including in particular the equiva-lent expression adopted in Eurocode 7, which is based on ashape factor applied to an empirical expression for Nª for astrip footing. Our original paper was concerned only withcircular foundations, but the discussion considers both planestrain (strip footing) and circular geometry. In this responsewe have therefore adopted the notation Nª-strip and Nª-circle todifferentiate between these cases, which are linked by theshape factor, sª ¼ Nª-circle/Nª-strip (with similar notation ap-plying for Nq and Nc).

Table 3. Nª values for strip and circular foundations

�9: 8 Nq Nª – strip foundation Ng – circular foundation

White et al. EN 1997-1 BrinchHansen

Salgado Meyerhof White et al.(circular)

Eurocode 7(circular)

20 6.40 2.78 3.93 2.95 2.68 2.87 1.94 2.7522.5 8.23 4.16 5.99 4.49 4.12 4.43 3.29 4.1925 10.66 6.32 9.01 6.76 6.27 6.77 5.57 6.3127.5 13.94 9.69 13.47 10.10 9.50 10.29 9.44 9.4330 18.40 14.98 20.09 15.07 14.40 15.67 16.00 14.0732.5 24.58 23.31 30.05 22.54 21.92 24.00 27.11 21.0435 33.30 36.50 45.23 33.92 33.68 37.15 45.93 31.6637.5 45.81 57.45 68.77 51.58 52.47 58.40 77.82 48.1440 64.20 90.83 106.05 79.54 83.26 93.69 131.85 74.24

Effective angle of shearing resistance, φ�

0

20

40

60

80

100

20 25 30 35 40

EN 1997-1

Salgado

Brinch Hansen

Meyerhof

White .et al

Fig. 11. Nª values against �9 for a strip foundation

0

20

40

60

80

100

120

20 25 30 35 40

Effective angle of shearing resistance, φ�

EN 1997-1

White .et al

Fig. 12. Nª values against �9 for a circular foundation

148 DISCUSSION

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First a small clarification – the discusser perhaps impliesthat equation (2) was derived from centrifuge model testsbut in fact it was fitted to theoretical lower bound plasticitysolutions calculated using Martin’s analysis of bearing capa-city (ABC) program (Martin 2003; 2004). The benefit offitting an expression to these results is that it allows ourprocedure for capturing the stress-dependency of frictionangle to be performed iteratively without the need for a lookup table linking friction angle to Nª-circle. The discrepancybetween the theoretical values and our fitted expression isless than 5% over the range of friction angle 258 , � , 458.

The status of the Nª-circle values on which our equation (2)is based is that they are lower bound plasticity solutions forwhich the consistent upper bound provides equal resistance(C. M. Martin (2009), personal communication). In order forthe solutions to be established as formally exact, it must bedemonstrated that the lower bound stress field can beextended without violating the yield criterion. This has notyet been done, but Lyamin et al. (2007) have producedextensible lower bound solutions by way of finite elementlimit analysis for a 24-sided polygon (nominally a circle)that are within a few percent of the ABC solutions, so it ishighly likely that the ABC solutions will be extensible. Forpractical purposes the Nª-circle values on which equation (2)is based are definitive. The values of Nª-strip calculated byABC are formally exact. The consistent upper bound me-chanism provides the same resistance and the lower boundstress field is extensible (Martin, 2005).

There are idealisations associated with exact bearingcapacity factors derived from plasticity theory. The soil isassumed to obey normality and progressive failure is ne-glected. Closed-form expressions for Nq-strip and Nc-strip basedon these idealisations have long been established as exact(Shield, 1954), are generally accepted in practice, and areprovided in the Eurocode. Therefore, for consistency weshould also use expressions for Nª-strip and Nª-circle (andindeed Nq-circle and Nc-circle) that have the same basis. Wherea closed-form equation does not exist, an expression such asequation (2), which is fitted to theoretical solutions, mustsuffice. Similar expressions to equation (2) for other valuesof footing roughness and for plane strain (strip footing)conditions rather than circular geometry can easily bederived using ABC. The outdated empirical expressions suchas those listed by the discusser should be expunged fromdesign codes, text books and lecture notes now that moreaccurate relationships can be devised to replace them.

In practice, rather than using the individual bearing capa-city factors, a more rigorous approach is to discard the(conservative) assumption of superposition and use a pro-gram such as ABC directly. In this way the effects of thesoil strength, self-weight and surcharge are combined in thecalculation of a single lower bound stress field and theresulting bearing capacity, rather than three terms – imply-ing three different superimposed stress fields – being addedtogether.

The remaining uncertainty, which was the principal focusof our paper, is the determination of appropriate inputparameters – in particular the operative friction angle. Thediscusser highlights that our equation (2) indicates a valueof Nª-circle that is 44% higher than the Eurocode value(sªNª-strip) for � ¼ 408. An alternative view of this discre-pancy is to note that for Nª-circle , 75, equation (2) predictsa friction angle that is 7% lower than the Eurocode value(37.58 against 408). In this range, a 18 adjustment of � (i.e.,2.5%) changes Nª-circle by more than 20%.

By viewing the discrepancy in terms of friction angle it is

easier to reconcile the Eurocode expression with our morerigorous approach. The discusser states that the Eurocodeexpression for Nª-strip and the shape factor sª were validatedfrom large-scale model tests. In these tests, the link between� and Nª-circle (or sªNª-strip) was presumably assessed bycomparing the measured Nª-circle with the friction anglemeasured in a soil element test – which is unaffected byprogressive failure. As our paper highlights, progressive fail-ure means that the operative friction angle beneath a founda-tion at failure is lower than the peak friction angle of anyindividual soil element. An operative friction angle of 37.58in a large footing test compared with 408 for the same soilin an element test is perfectly plausible given the observa-tions in our paper, and could explain the divergence inFig. 12.

This observation does not provide an argument in supportof the empirical Eurocode basis for Nª-circle instead of atheoretically rigorous one, because it applies equally toNq-strip and Nc-strip (for which the theoretically exact solutionsare firmly established). Instead, it highlights that designersmust consider carefully the influence of progressive failureon the operative friction angle that is used to calculatebearing capacity factors.

It appears that the current set of bearing capacity factorsin the Eurocode is a conflicting mixture of theoretical rigourbased on idealised soil behaviour where closed-form expres-sion are available (e.g. Nq-strip and Nc-strip), and empiricismwhere they are not – perhaps inadvertently incorporating anadjustment of � for progressive failure. We suggest that theexpressions currently given for Nª-strip and the shape factorsshould be revised to be consistent with theory. A simpleimprovement would be to adopt the empirical expression forNª-strip given by Brinch Hansen (1970), which is identicalwith the current Eurocode expression but with an initialfactor of 1.5 rather than 2 (see the discusser’s equation (9)).Brinch Hansen’s expression provides values that lie within5% of the exact solutions. Our equation (2) could be used todefine Nª-circle directly, rather than by way of a shape factor.Equally importantly, it is necessary to develop guidance onthe appropriate friction angle to input, accounting particu-larly for progressive failure.

We would encourage readers to download and make useof Martin’s ABC software, which he has generously madeavailable through his website (http://www-civil.eng.ox.ac.uk/people/cmm/software/abc/).

REFERENCESBrinch Hansen, J. (1970). A revised and extended formula for

bearing capacity, Bulletin No. 28, Danish Geotechnical Institute,Lyngby

Lyamin, A. V., Salgado, R, Sloan, S. W. & Prezzi, M. (2007). Twoand three-dimensional bearing capacity of footings on sand.Geotechnique 57, No, 8, 647–662.

Martin, C. M. (2003). New software for rigorous bearing capacitycalculations. Proceedings of international symposium on founda-tion: innovation, observation, design and practice, Dundee, pp.581–592.

Martin, C. M. (2004). User guide for ABC: Analysis of BearingCapacity. Version 1.0, Report No. 2261/03. Oxford: OxfordUniversity Engineering Laboratory (OUEL).

Martin, C. M. (2005). Exact bearing capacity calculations using themethod of characteristics. Proc. 11th Int. Conf. of IACMAG,Turin 4, 441–450.

Shield, R. T. (1954). Plastic potential theory and Prandtl bearingcapacity solution. J. Appl. Mech. 21, 193–194.

DISCUSSION 149