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    Lecture 4

    Design of

    Rock-socketed Piles

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    Rock-socketed piles

    PILE

    Rock

    Socket

    Soil

    Rock

    Load

    In most cases, the lower part of the pile is socketed into rock.

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    Performance of rock socket

    Socket friction

    Socket friction increases with socket

    roughness

    Smooth socket friction fully mobilisedat small pile settlement

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    (after Horvath & Kenny, 1979)

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    Performance of rock socket

    Socket friction is related to socket

    roughness

    Horvath et al. (1983) established that

    fs = 0.8 (RF)0.45 qu

    where RF = roughness factor = (r Lt)/(D

    L)

    r = average height of asperities, Lt = total

    distance along the socket wall profile, D =

    socket diameter, L = socket length & qu =

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    Effect of socket diameter Seidel & Harberfield (1995) found that

    as the socket diameter increases, the

    effect of dilation is reduced for a given

    degree of socket roughness. The variations in socket friction can

    be changed by a factor of up to 3, fordiameters varying between 0.5 m and

    2 m.

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    Rock socket frictionUnit shaft friction fs

    Early days (1960s to early 1970s)

    fs = 250 kPa for fragmented shale

    fs = 120 to 180 kPa for weak

    mudstone

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    Rock socket frictionfs is related to qu

    Rosenberg & Journeaux (1976)

    fs = 0.375 (qu)0.515

    Meigh & Wolshi (1979)

    fs = 0.22 (qu)0.6

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    Rock socket friction Williams & Pells (1981)

    fs = qu

    where and are reduction factors

    reflecting rock strength and fracturestate, respectively. See Figures.

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    Williams & Pells (see next figure for value of )

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    (after Williams and Pells)

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    Rock socket friction Horvath et al. (1983)

    fs = 0.2 to 0.3 (qu)0.5

    Rowe & Armitage (1987)

    fs = 0.45 (qu)0.5 for a smooth socket

    fs = 0.60 (qu)0.5 for a rough socket

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    Rock socket friction From a large set of field data

    (including those of Singapore),

    Zhang & Einstein (1998) found that

    fs = 0.4 (qu)0.5 for a smooth socket

    fs = 0.8 (qu)0.5 for a rough socket

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    Rock socket frictionRecommendations for local design

    Preliminary design using Horvath

    fs = 0.2 to 0.3 (qu)0.5

    Detail design using Williams & Pells

    fs = qu(All values need to be confirmed by load tests)

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    Performance of socket base

    For the same rock strength, base

    resistance increases with overburdenpressure

    Shallow embedment: brittle failure Deep embedment: ductile failure (i.e.

    capacity is not a problem, only

    settlement is a concern, see figure)

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    Socket base resistanceUnit base resistance qb

    Early days (60s & 70s)

    Weak shale 3 MPa

    Moderately strong shale 3.9-4.9

    MPa

    Weak mudstone 6.8 MPaModerately strong mudstone 28-58

    MPa

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    Correlation

    between qband RQD

    for a jointed

    rock mass(after

    Peck et al.,

    1974)

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    Socket base resistance Teng (1962)

    qb = 5 to 8 qu

    Coates (1967)

    qb = 3 qu

    Tomlinson

    qb = 1 to 6 qu

    (depending on rock fracture state)

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    Socket base resistanceRecommended approach for design

    Rowe and Armitage (1987)

    qb = 1 qu under working stress to

    ensure no yielding of rock

    qb = 2.5 qu under ultimate condition

    [Values subject to capacity andsettlement verification from load tests]

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    Socket base resistance Based on a large number of field data

    (including that of Singapore)

    Zhang & Einstein (1998) found that

    qb = 3.0 to 6.6 (qu)0.5

    (with a mean coefficient of 4.8)

    [Note qb is related to square root ofqu]

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    Zhang & Einstein (1998)

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    Conservative ratio of qb upon qu

    (after HK GEO)

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    (after HK GEO)

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    Unconfined compressive strength

    REMINDER

    Use quc (unconfined compressive

    strength of concrete) if the rock is

    stronger than concrete.Poser: In view of the above, is it

    necessary to socket pile into hard rock?{Answer can be yes or no!}

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    Settlement of rock-socketed piles

    For socketed piles with long

    embedment length, capacity isnormally governed by concrete

    strength. Settlement of pile needs to be

    evaluated especially in suspected soft

    toe cases.

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    Rock socket Under working load, the load-

    settlement response of a socketedpiles is fairly linear in most cases.

    Elastic theory can be employed toevaluate the pile settlement

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    0 4 8 12 16 20

    Load (MN)

    0

    4

    8

    12

    16

    Settlem

    ent(mm)

    Load-settlement response is reasonably linear up to working load of 10 MN

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    Rock socket modulus Er Tomlinson

    Er= j Mr quc (see tables)

    Rowe and Armitage

    Er= 215 (qu)0.5

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    Mass factor j (after Tomlinson and BS8004)

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    Modulus ratio Mr (after BS8006)

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    Settlement of rock socket RECOMMENDED APPROACH

    Rowe & Armitage (1987)

    Assumptions:

    Soil above rock socket has nosignificant contribution in resistance

    Elastic solutions are developedassuming a fully bonded socket using a

    FEM.

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    (after

    Rowe &Armitage,

    1987)

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    Rowe and Armitage Assumptions (continued)

    The dimensionless settlement I defined

    by I = Ed D/Qt

    where is the socket settlement, Ed isthe design socket shaft modulus, D is

    socket diameter and Qt is the working

    load. Design charts are developed for various

    pile geometry and socket/concrete

    modulus ratios

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    Rowe and ArmitageDESIGN CONCEPT

    Satisfying a user-specified design

    settlement

    Ensuring an adequate factor of safetyagainst failure

    Limit state design concept: partial safety

    factors applied to deformation andstrength parameters

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    Rowe and ArmitageDESIGN PROCEDURES

    Step 1: Given

    design settlement d

    socket diameter D applied working load Qt

    Concrete modulus Ep [Factored] Unconfined compressive strength of

    rock qu

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    Rowe and Armitage Step 2 (a): Determine

    fs = 0.45 (qu)0.5

    Er= 215 (qu)0.5

    Determine Eb

    if qu

    at pile base is different

    Step 2(b):Apply partial factor of safety

    Design unit shaft resistance d = f fs

    Design rock mass modulus Ed = fE Er

    Partial factors f and fE are taken as 0.7 or 0.5(for probability of 30% and 11% exceeding d )

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    Rowe and Armitage Step 3: Determine Ep/Ed and Eb/Er

    Step 4(a): Determine maximum

    socket length assuming no base

    resistance(L/D)max = Qt/( D

    2 d)

    Step 4(b): Determine thedimensionless settlement I

    I = Ed

    D/Qt

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    Rowe and Armitage Step 5(a): Determine (L/D)d and

    (Qb/Qt)d from the intersection of thefactored design line for (L/D)max with

    the contour for Id using design chartsallowing for slip

    Step 5(b): If there is an intersection,

    calculation is okay & proceed to step

    6.

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    Qb =100%,

    I.e.

    Full base

    resistance

    Qb = 0%, I.e. Full shaft resistance

    Intersection

    refers to

    estimated

    Qb(after

    Rowe &

    Armitage,1987)

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    Rowe and Armitage Step 5(C): Determine the value of (L/D)d

    for given Id If there is a value of (L/D)d can be found,

    determine (Qb/Qt)d for the (L/D)d and proceed

    to step 6 If there is no value, redesign is necessary, go

    back to step 1.

    Refer to paper for details for design involvinga recessed pile

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    Determine the

    value of (L/D)dfor given Id

    Elasticsocket

    (no slip)

    (after Rowe &

    Armitage, 1987)

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    If there is a value of (L/D)d can be found,

    determine (Qb/Qt)d for the (L/D)d

    (after Rowe & Armitage, 1987)

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    Rowe and Armitage Step 6: Check for base condition

    qt = Qt/( D2/4)

    Under working load

    qb = (Qb/Qt)d qt and need to be < qu Under worst condition

    qbu

    = qt

    - 4(L/D)d

    (0.3 fs

    ) and < 2.5 qu

    assuming only 0.3 fs can be mobilised

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    Summary

    of designcurves

    (1) Full slipEb/Er = 0.5

    (after

    Rowe &

    Armitage,

    1987)

    Fig. 6.1

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    Summary

    of designcurves

    (2) Full slipEb/Er = 1.0

    (after

    Rowe &

    Armitage,

    1987)

    Fig. 6.2

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    Summary

    of designcurves

    (3) Full slipEb/Er = 2.0

    (after

    Rowe &

    Armitage,

    1987)

    Fig. 6.3

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    Summary

    of designcurves

    (4) Elasticsocket

    (No slip)

    (after

    Rowe &

    Armitage,

    1987)

    Fig. 6.4

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    Summaryof design

    curves

    (5) Elastic

    socket:

    baseresistance

    (after

    Rowe &Armitage,

    1987)

    Fig. 6.5

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    Axially loaded rock-socketed piles

    Examples 4.1 [from Rowe & Armitage Page 138 Case

    (i)]

    Given:

    Design settlement d = 8.5 mmPile diameter D = 0.71 m

    Design working load Qt = 4.45 MN

    Modulus of pile material Ep = 37,000 MPa

    Unconfined compressive strength of rock qu = 6.75 MPa

    [Rock at pile base is more fractured and Eb = 0.75 Er]

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    CalculationStep 2(a): Unit shaft friction fs = 0.45 (qu)

    0.5 = 1.17 MPa

    Youngs modulus of rock Ef= 215 (qu)0.5 = 560 MPa

    Step 2(b): Take partial factor of safety f = fE = 0.7[Probability of 30% not exceeding d]Design unit shaft friction d = f fs =0.82 MPaDesign rock mass modulus Ed = fE Er= 390 MPa

    Step 3: Ep/Ed = 95 (therefore use Ep/Ed = 100 chart)Eb/Er= 0.75 (interpolation between Eb/Er =1 [Fig. 6.2]

    and = 0.5 [Fig. 6.1])

    Step 4(a):Assume no base resistance, maximum socket length

    (L/D)max = Qt / (D2 d ) = 3.4

    Step 4(b): Dimensionless settlement I = Ed D/ Qt = 0.53

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    Calculation (cont.)Step 5(a):

    By drawing a line from (Qb/Qt)d = 100 % to (L/D) = 3.4in Fig. 6.2(d) (i.e. for Eb/Er= 1) show that (Qb/Qt)d =63 % and the corresponding design socketlength/diameter ratio (L/D)d = 1.3 for Id = 0.53.

    Similarly for Eb/Er= 0.5 from Fig. 6.1(d),(Qb/Qt)d = 27 % and (L/D)d = 2.5

    By interpolation, (Qb/Qt) = 45% and (L/D)d = 1.9

    Hence design socket length = 1.9 D = 1.35 mand proceed to Step (6)

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    Calculation (cont.)Step (6) Unit loading pressure

    qt = Qt / (D2

    /4 ) = 11.2 MPa Under working condition, allowable base pressure

    qb = (Qb/Qt)d qt = 5.1 MPa < qu OKAY

    Under worst condition where only 0.3 fs can bemobilised qbu = qt 4(L/D)d (0.3 fs)

    = 8.5 MPa < 2.5 qu OKAY

    Design completed and required socket length is

    1.35 m.

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    Example 4.2Given:

    d = 5 mm, D = 1 m, Qt = 7.8 MN,Ep = 34,000 MPa, qu = 20 MPa, Eb = Er

    Calculations:

    Step 2(a) & (b): d = f fs = 0.7 x 0.45 qu = 1.4 MPa

    Ed = fE Er= 0.7 x 215 qu = 673 MPa

    Step 3: Ep/E

    d= 34,000 / 673 = 50

    Step 4: (L/D)max = Qt / (D2 d ) = 1.77

    I = Ed D/ Qt = 0.43

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    Calculation (cont.)Step 5(a): Fig. 6.2(c) No intersection!

    Step 5(b): Fig. 6.4(a)

    for I = 0.43 & Ep/Ed = 50

    (L/D) required 1.2

    Fig. 6.5(a)for (L/D) = 1.2 & Ep/Ed = 50

    (Qb/Qt) = 30%

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    Calculation (cont.)Step 6: qt = Qt / (D

    2 /4 ) = 9.93 MPa

    Under working conditionqb = (Qb/Qt)d qt = 0.3 x 9.93 MPa = 2.98 < qu

    (20MPa) OKAY

    Under worst working conditionqbu = qt 4(L/D)d (0.3 fs)

    = 9.93 4(1.2) (0.3 x 0.45 qu)

    = 7.03 MPa < 2.5 qu OKAY

    Required socket length = 1.2 x 1 = 1.2 m

    and there is no slip in the socket.

    References for

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    References for

    Design of rock- socketed piles

    Related publications by C F Leung1. Leung C F and Radhakrishnan R (1985). Observations of an

    instrumented pile-raft foundation in weak rock, Proc. 11th Int.Conf. on Soil Mech. and Fdn. Engr., San Francisco, pp. 1429-1432.

    2. Leung C F, Radhakrishnan R and Wong Y K (1988).

    Observations of an instrumented pile-raft foundation in weakrock, Proc. Instn. Civ. Engrs., Part 1, Vol. 84, pp. 693-711.

    3. Leung C F and Radhakrishnan R (1990). Geotechnicalproperties of weathered sedimentary rocks, GeotechnicalEngineering, Vol. 21, pp. 29-48.

    4. Leung C F, Radhakrishnan R and Tan S A (1991).Performance of precast driven piles in marine clay, J. ofGeotech. Engr., ASCE, Vol. 117, pp. 637-657.

    5. Leung C F (1996). Case studies of rock-socketed piles,Geotechnical Engineering, Vol. 27, pp. 51-67.

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    Related publications by C F Leung (cont.)

    6. Leung C F and Tan G P (1996). Load carrying capacity of spunpiles, Proc. 12th Southeast Asian Geotech. Conf., Kuala Lumpur,Vol. 1, pp. 423-428.

    7. Leung C F and Chow Y K (1998). Settlement of rock-socketedpiles, Proc. 5th Int. Conf. on Tall Buildings, Hong Kong, Vol. 2, pp.884-889.

    8. Radhakrishnan R, Leung C F and Subrahmanyam R (1985).Load tests on instrumented large diameter bored piles in weak

    rock, Proc. 8th Southeast Asian Geotech. Conf., Kuala Lumpur,Vol. 1, pp. 2.50 2.53.

    9. Radhakrishnan R and Leung C F (1989). Load transfer behaviourof rock-socketed piles, J. of Geotech. Engr., ASCE, Vol. 115, pp.755-768.

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    Other publications

    1. BSI (1986). British Standard Code of Practice for Foundations(BS8004:1986), British Standards Institution, London, UK.

    2. Cole K W and Stroud M A (1977). Rock socket piles at

    Coventry Point, Market Way, Coventry" Piles in Weak Rock,Instn. of Civil Engrs., UK, pp. 47-62.

    3. GEO (1996). Pile Design and Construction, GEO PublicationNo. 1/96, Geotechnical Engr. Office, Hong Kong.

    4. Horvath R G and Kenny T C (1979). Shaft resistance of rock-

    socketed drilled piers, Symp. on Deep Foundations, ASCE,pp. 182-214.

    5. Horvath R G, Kenny T C and Kozicki P (1983). Methods ofimproving the performance of drilled piers in weak rock, Can.Geotech. J., Vol. 20, pp. 758-772.

    6. ISRM (1985). Suggested method for determining point loadstrength, Int. J. of Rock Mech. and Mining Sci., Vol. 22, pp.51-60.

    7. Irfan T Y and Powell G E (1991). Foundation Design ofCaissons on Granitic and Volcanic Rocks, GEO Report No. 8,

    Geotech. Control Office, Hong Kong.

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    Other publications (cont.)

    8. Lam T S K, Yau J H W and Premchitt J (1991). Side resistance ofa rock-socketed caisson, Hong Kong Engineer, Vol. 19, No. 2,pp. 17-28.

    9. Meigh A C and Wolski W (1979). Design parameters for weakrock, Proc. 7th European Conf. On Soil Mech. and Fdn. Engr.,Brighton, Vol. 5, pp. 59-79.

    10. Osterberg J O and Gill S A (1973). Load transfer mechanism forpiers socketed in hard soils on rock, Proc. 9th Canadian Symp. on

    Rock Mech., pp. 235-262.11. Peck R B, Hanson W E and Thornburn T H (1974). Foundation

    Engineering, 2nd Edition, John Wiley and Sons, New York, USA.

    12. Rosenberg R K and Journeaux N L (1976). Friction and endbearing tests on bedrock for high capacity socket design,

    Canadian Geotech. J., Vol. 13, pp. 324-333.13. Rowe R K and Armitage H H (1987a). Theoretical solutions for

    axial deformation of drilled shafts in rock, Canadian Geotech. J.,Vol. 24, pp. 114-125.

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    14. Rowe R K and Armitage H H (1987b). A design method for drilledpiers in soft rock, Canadian Geotech. J., Vol. 24, pp. 126-142.

    15. Seidel J P and Harberfield C M (1994). A new approach to theprediction of drilled pier performance in rock, Proc. Int. Conf. onDesign and Construction of Deep Foundations, Orlando, Vol. 2,pp. 556-570.

    16. Shiu Y K and Chung W K (1994). Case studies in prediction andmodelling of the behaviour of foundation on rock, Proc. 8th Int.

    Congress on Rock Mech., Tokyo, Vol. 3, pp. 1243-124.17. Teng W C (1962). Foundation Design, Prentice-Hall, USA.

    18. Tomlinson M J (1995). Foundation Design and Construction, 6thEdition, Longman, UK.

    19. Williams A F and Pells P J N (1981). Side resistance rock

    sockets in sandstone, mudstone and shale, Can. Geotech. J.,Vol. 18, pp. 502-513.

    20. Zhang L and Einstein H H (1998). End bearing capacity of drilledshafts in rock, J. of Geotech. and Geoenvir. Engr., Vol. 124, pp.574-584.

    Other publications (cont.)