Beam on Elastic Foundations

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    Loadings on locks

    1. Water level = max

    2. Water level= min

    3. Empty lock - repairs

    N N

    N N

    N N

    T TT T

    T T

    T T

    M M

    M M

    M M

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    N N

    T TM MPa

    S

    gr

    p

    N* N*

    M* M*

    Equivalent loadings on the floor

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    Beams on elastic foundations

    Foundation slab&

    Foundation terrain

    Plane strain conditionst=ct

    q=ct

    All the sections - same displacements analyze on a 1 m slice

    Plane strainconditions

    B= (theoretic)

    B> 3 x Lg (practice)

    ( end sections)

    Soil reactions

    NN

    M

    M

    Lg

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    Methods to calculate BoEF

    Mathematical equations(soil structure interaction)

    Behavior of the soil

    Deformed average fiber of the slab

    = + ()

    = k

    = + 1 + 22 + 33 + +

    Winkler

    Gurbonov-Posadov

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    Winkler Model

    =

    =

    The reacting forces of the foundation are proportional at every point to the deflection of thebeam at that point

    Introduced by E. Winkler in 1867 The application of this modelon soil foundations should be regarded only as a practical

    approximation

    includes the flexural rigidity of thebeam and also the elasticity of thesupporting medium

    = 4

    Characteristic of the system

    N

    mfoundation modulus

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    Stiffness of the beam

    Characterizes the relative stiffness of the beam on elastic foundation

    < 0.5 ( 4 )

    > 5 ()

    0.5 4 < < 5 ()

    Short beam

    Medium beam

    Long beam

    The beam deformation can beneglected beam absolutely rigid computed using statics

    Loads applied at one end have afinite and not negligible effect onthe other end no approximationsare possible

    The effect of a Load applied at oneend can be neglected at the otherend computations are greatlysimplified

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    Mathematical expressions for y M T

    = 1() +1

    2()

    1

    3()

    1

    ()

    1

    3(( )) +

    1

    (( )) +

    1

    (( ))

    = 1 1 2() 1

    3() 4() 1 2(( )) + 1

    3(( )) + 1

    3(( ))

    = 1 +1

    2 +

    3() +

    () +1(( ))

    1

    2(( )) -

    1

    2(( ))

    = 1 +

    2 +

    3() 4() 4(( )) 1(( )) -

    1(( ))

    1 = cosh() cos()

    2() =1

    2 cosh sin + sinh() cos()

    3 =1

    2 sinh() sin()

    () = 12 cosh sin sinh() cos()

    = = 2

    2 =

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    Winkler model advantages and disadvantages

    Disadvantages:

    k has no physical sense. it is determined from in situ tests. a wide variety of formulas for k different values for the same E and

    you cant determine k from those formulas.

    k depends on : physical properties of the foundation

    the shape and the length of the loading plate

    the concentrated force value the model doesnt consider the lateral loadings

    for an uniform loading (weight) there is no moment or shear force diagrams (false)

    Advantages:

    for sand foundations correct results (if k is determined accurately)

    very easy and simple model

    For floor locks Winkler model can beused for thin compressible

    foundations (

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    Winkler Example

    k=50000 K=kPaLg=15mhg=2m

    a = 1.5 mc = 3 mconcrete beam

    P=500 kNM = 150 kNmq = 10 kN/m

    s = - 20 kN/m

    Ansys beam54 elements

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    Gurbonov Posadov Method

    it is based on Boussinesq/ Flamandmodels (elastic half-space/ half-plane model)

    the soil is replaced by a solid body with the following characteristics:

    extends laterally and down elastic linear deformable homogeneous and isotropic

    Disadvantages:

    overestimate the settlements

    settlements at the ends tend to infinite

    overestimates the moments

    the model doesnt consider the lateral loadings

    Boussinesq spatial problem

    Flamand - plane problem

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    Gurbonov Posadov Method

    = + ()

    = + 1 + 22 + 33 + + Exponential series

    polynomial equation (n degree)

    , 1, 2, - unknowns

    n = 10 (practical reasons)

    In order to calculate y, M, T G.P. realized tables for unitary loadings

    The tables are realized for half of the slab foundation (because the loadingsare symmetrical).

    This half is divided in 10 parts where the efforts, moments and shear forceare calculated.

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    N NT TM MPa

    S

    gr

    p

    N* N*

    M* M*

    Equivalent loadings on the floor

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    flexibility index

    t < 1 short beam (absolutely rigid)1

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    Gurbonov Posadov Example

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    Conclusions

    Winkler model is a very simple model but it should be regarded as a practical

    approximation when it is used on soil foundations.

    For a uniform loading (weight) the Winkler model doesntcompute shear force

    diagrams or moment diagrams which in reality is false.

    Gurbonov Posadov model take into consideration the displacement of the soil

    outside the beam.

    For predimensioning purposes of a lock floor we can use Gurbonov Posadov

    Method.

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    Thank you for your attention!