5 Slope Stability

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    Chapter 5

    Slope Stability

    FKAAS, UTHM

    Dr. CM Chan

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    5.1 Natural and artificial slopes

    (Whitlow 2001)

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    5.2 Soil moements ! Slope insta"ilit#

    Falls

    Topples

    Slides- rotational, compound, translational

    Lateral spreads

    Flows

    Complex or compound failure

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    5.2.1 $#pes of soil moements

    (Whitlow 2001)

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    5.% Causes of insta"ilit#

    Main categories-te causes of slope insta!ilit"#

    $ %round conditions- weatered, fissures, etc&

    $ %eomorpological processes- tectonic

    acti'ities, wa'e erosion, etc&

    $ ("sical processes- rainfall, tidal effects,etc&

    $ Man-madeprocesses- exca'ation, drawdown

    of water le'el )reser'oirs*, mining, +uarr"ing,

    etc&

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    Commoncauses of slope insta!ilit"#

    $ eateringeffect

    $ Canges of slope geometr"

    $ ecrease in effecti'e stressof soil mass

    $ .xcess loading)e+ui'alent to increase in

    eigt of slope*

    $ (oor design and/or construction- e&g&exca'ation near toe of existing slope

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    5.& Slope sta"ilit# anal#sis

    Metods of anal"sis#

    $ 0nfinite slope metod- plane translational

    slide

    $ .ffecti'e and total stress approac )usuall"

    u1 2o*

    $ Fellenius or Swedis or ordinar" slice

    metod

    $ Metod of slices )effecti'e stress*- 3isop4s

    metod, 3isop4s modified metod

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    $ Ta"lor4s metod- undrained anal"sis

    $ 3isop-Morgenstern4s metod

    $ 5an!u4s metod- non-circular slip surfaces

    $ edge metod- single plane

    Focus:

    $ Fellenius or Swedish or ordinary slice method

    $ Taylors method- undrained analysis

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    5.5 'actor of safet# ('S)

    6elies on sound engineering 7udgement,

    consideration of 'arious contri!uting factors and

    appropriate metod of anal"sis&

    Factors to !e considered#

    $ Conse+uencesof failure

    $ Confidencein te a'aila!le information and

    data

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    Higfactor of safet" )FS*#$ ris8 of loss of li'es and ad7acent structures-

    ultimate limit state

    $ possi!ilit" tat slope could !e prone tpdeformations wic could affect ad7acent

    structures, e'en if it as sufficient sta!ilit"-

    ser'ice limit state

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    Lowerfactor of safet" )FS*#

    $ period of exposure to factors causing

    insta!ilit" is sort- e&g& temporar" wor8s

    $ do notaffect li'es or structures

    $ localised- simple remedial measures )wen

    re+uired*

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    9arious factors to !e considered in coosinga

    suita!le FS#

    $ (ast or local experience- presence or pre-

    existing slip planes, future canges to soil

    profile, water ta!le le'els, etc&

    $ Complexit" of ground conditions

    $ ata from site in'estigationreports

    $ Confidence in design parameters)searstrengt, pore pressures, etc&*

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    5. $a#lors method

    6efers to Ta"lor4s cur'es )Ta"lor4s # undrained

    anal"sis sta!ilit" cart*&

    Ta"lor ):;, depends on slope inclination

    angle, ?, and dept factor, , @ is dept of stiff

    stratum&

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    Ta"lor4s undrained anal"sis sta!ilit" cart&

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    F 1 te lowest FS o!tained from a circular arc

    anal"sisof a omogeneousslope wit undrainedsear strengt, cu, !ul8 unit weigt, , and eigt,

    H u1 2o&

    >s depends on te slope angle )or*, and

    dept factor , were H )or @* 1 dept to stiff

    stratum&

    See Taylors curves (Fig. 12.10, pg.

    !1"#arnes$.

    %&ample 12.' (#arnes$

    30

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    Hard la"er

    .xample#

    3ased on te a!o'e figure, @ 1 :B&2 m&

    1 :B/:2 1 :&B

    From Ta"lor4s cart, wit 1 :&B and ? 1 B2, terefore > 1 2&:B&>s 1 cu/ FH

    FS 1 )

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    5.* +rdinar# slice ! Swedish ! 'ellenius

    method

    Assumption# te inter-slice forcesare e+ualand

    opposite- teir resultants are @ero&

    .: 1 .B and E: 1 EB&

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    6esol'ing te forces acting normalto te !ase

    of eac slice# ) *cos - ul

    *here,

    u ) whw

    hw) height to the water ta+le a+ove the

    +ase o the slice or related to the

    nearest euipotential line i a low netis drawn

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    For a omogeneousslope wit c and constantalong te slip surface#

    F 1 cLA3 tan)cos - ul*

    sin*here,

    $ *, and u are determined or each slice

    and ta+ulated.$ can +e positive or negative.

    -

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    Te formula can !e rewritten as#

    F 1 Gc4L )cos - rusec* tan4

    sin

    3" ta8ing ! 1 Lcos,

    u 1 ru

    Lcos

    u 1 ru sec

    L

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    For a stead" state seepage troug slopes, te

    pore pressure must !e ta8en into account-effecti'esear strengt parameters are used&

    0f pore pressure is assumed to !e @ero#

    F 1 GcL costan

    sin

    %&amples .2a and .2+ (otes +y F /ing$

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    .xample =&Ba (otes +y F /ing$

    ivenTe slope and soil properties, as sown in

    Fig& =&:IFind FS 'ia te Fellenius metod of slices for te

    trial circle sown

    :2;&Io

    J

    :2 m

    6 1 : m

    B&I m

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    (rocedure#

    :& Te slope was plotted to a con'enient scale&

    B& For te assumed failure circle and te slices

    selected, te widt of eac slice is measured as

    B&I m&

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    e&g& Te calculations for slice :are as follow#

    : 1 )area* x )* 1 !/B

    1 )B&I x : 1 :cos: 1 =

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    Ta!le =&Ba