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    CALCULO DE LOS ESFUERZOS ALEJADOS DE LOS LÍMITESDE LA EXCAVACION

    Observando la figura siguiente, podemos expresar las ecuaciones finales de la

    solución bidimensional de la distribución de esfuerzos alrededor de una abertura

    en un cuerpo elástico usando en este caso un sistema de coordenadas polares en

    la cual los esfuerzos son definidos en técnicas de tracciones, actuando sobre las

    caras de un elemento ubicado por un radio r y un ángulo polar θ.

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    ESFUERZOS ALEJADOS DE LOS LÍMITES DE LA EXCAVACIÓN

    Componentes de los esfe!"os en el pnto #!$   θ %&

    Esfuerzo radial: σ r 1

    2 P

     z[ (1+k )(1− a

    2

    r2 )+(1−k )(1−  4 a

    2

    r2  +

    3a4

    r4 )cos2θ]

    Esfuerzo tangencial: σ θ 1

    2 P z[ (1+k )(1+ a

    2

    r2 )−(1−k )(1+ 3a

    4

    r4 )cos2θ]

    Esfuerzo de corte: τ rθ 1

    2 P

     z[−(1−k )(1+2a

    2

    r2 −

    3a4

    r4 )sen2θ]

    Esfe!"os p!'n('p)les en el pnto #!$   θ %&

    Esfuerzo principal máximo: σ  !1

    2 "  σ  r # σ θ $ #

    τr θ

    ¿¿

    14(σ r−σ θ )2+¿

    √ ¿

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    )exp"GSI −1009−3 D $

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    −203 $

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    mi+'&!4 "enfocándose al peor de los casos$.

    *)ll)ndo los p)!2met!os del m)('"o !o(oso&

    m b!4.exp"45−10028−4 (0) $+,&5.

    )exp"45−1009−3(0) $,++.

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