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pdfcrowd.com ope n in br ows er PRO v ersion Are you a developer? Try out the HTML to PDF API Sear ch... Tweet 0  0 Submit  You are her e: Home / Bearing Capacity Theor ies  / Prandtl’s Theory on Bearing Capacity Analysis | Failure Mechanism Prandtl’s Theory on Bearing Capacity Analysis | Failure Mechanism Prandtl 1920 developed an equation based on h is study of penetration of long hard metal punc her into softer materials for compu ting the ultimate bearing capacity. He made the following assumptions for the derivation. The material is sof ter , homogeneous and isotropic. The material is weightless and possesse s only f riction and cohesion. Recent Projcts: Snake Game Using C Sound Operated On-Off Switch Micropho ne Amplifier Using Op-amp 741 Thermal Touch Switch using op-amp 741 Voltag e into Frequency Con verter Telephone Diary using C++ Employee Management System Using HOME ELECTRONICS PROJECTS CIVIL PROJECTS COMPUTER PROJECTS MECHANICAL PROJECTS CONTACT US!  AB OUT US! 5 Like Share Mechanisms CD-ROM Linear Motion Mechanism Mechanism Soi l Analy sis Methods et e

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    You are here: Home / Bearing Capacity Theories / Prandtls Theory on Bearing Capacity Analysis | Failure

    Mechanism

    Prandtls Theory on BearingCapacity Analysis | FailureMechanism

    Prandtl 1920 developed an equation based on his study of penetration of long hard metal puncher intosofter materials for computing the ultimate bearing capacity. He made the following assumptions forthe derivation.

    The material is softer,

    homogeneous and isotropic.

    The material is weightless and

    possesses only friction and

    cohesion.

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    The problem is two dimensional

    The base of the puncher is smooth.

    The material behaves as a rigid

    body.

    The volume change will be Zero.

    The resulting deformation will be a

    plastic deformation.

    Failure mechanism The mechanisms of failure of soil under plastic equilibrium

    are:

    1. Failure occurs along definite slip surfaces and symmetrical with respect to the

    centerline of the puncher or footing in the case of soil for symmetrical vertical

    loading.

    2. Under ultimate load Qult acting on the footing of width B as shown in Fig(a), a

    triangular wedge of soil abc is formed below the footing and pushed down as a

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    rigid body. The stresses acting on abc will be in active stage.

    3. Due to gradual downward push of the wedge abc, the soil mass on its left and right will be pushed

    outward and upward. The failure takes place along the slip surfaces bcde and acfg. These

    surfaces comprise triangular wedges bde and afg, and sectors bcd and acf.

    4. The mass of soil will be in a plastic state above `the failure surface gfcde and in elastic state

    below the surface.

    5. The failure surfaces can be divided into three Zones I to III as Shown in the Fig.(a). Zone I will be

    in active state, Zone II in radial shear and Zone III in plastic state.

    6. The lower boundaries of zone II are parts of logarithmic spirals with their poles coinciding with

    the corresponding edge of the footing. The straight lines de and fg are tangential to spirals at

    points d and f respectively and meet the horizontal surface at angles of (450 /2)

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