 
          2848
        
        
          Proceedings of the 18
        
        
          th
        
        
          International Conference on Soil Mechanics and Geotechnical Engineering, Paris 2013
        
        
          Figure 2: Model for the soil pile interaction in the peudoestatic model.
        
        
          To increase the application time of loading, a high strength
        
        
          resilient material is required to be placed on the head of the pile
        
        
          in the area of impact. Assuming that the load is obtained by a
        
        
          falling mass of approximately 10% of the ultimate capacity of
        
        
          the pile (Fu) and also considering the charging triangular
        
        
          diagram of Figure 3, then:
        
        
          
            g
          
        
        
          
            h
          
        
        
          
            F
          
        
        
          
            gh
          
        
        
          
            g
          
        
        
          
            F
          
        
        
          
            F
          
        
        
          
            gh m t
          
        
        
          
            u
          
        
        
          
            u
          
        
        
          
            u
          
        
        
          21.0
        
        
          2 1.0
        
        
          2
        
        
          50
        
        
          
        
        
          
        
        
          
        
        
          (3)
        
        
          Where
        
        
          
            h
          
        
        
          is the falling height of the mass
        
        
          
            m
          
        
        
          . This cinematic
        
        
          equilibrium equation is an approximation since restitution
        
        
          forces has been overridden.
        
        
          The maximum forces that can be exerted on the pile tip
        
        
          (F
        
        
          max
        
        
          ) due to the falling mass on a cushion material of elastic
        
        
          constant
        
        
          
            k
          
        
        
          
            e
          
        
        
          can be calculated as:
        
        
          max
        
        
          max
        
        
          2
        
        
          1
        
        
          
            z F hgm
          
        
        
          
        
        
          (4)
        
        
          Where z
        
        
          max
        
        
          is the maximum deformation of the cushion
        
        
          material z
        
        
          max
        
        
          = F
        
        
          max
        
        
          /k
        
        
          e
        
        
          . Then, replacing in equation (4),
        
        
          
            e
          
        
        
          
            khgm F
          
        
        
          2
        
        
          max
        
        
          
        
        
          (5)
        
        
          Being the natural frequency of the mass-cushion system:
        
        
          
            e
          
        
        
          
            k
          
        
        
          
            m T
          
        
        
          
        
        
          2
        
        
          
        
        
          (6)
        
        
          Since t
        
        
          50
        
        
          is half of the natural frequency and assuming a
        
        
          triangular shape of the wave (see Figure 3):
        
        
          
            e
          
        
        
          
            e
          
        
        
          
            k
          
        
        
          
            m
          
        
        
          
            t
          
        
        
          
            k
          
        
        
          
            m
          
        
        
          
        
        
          
        
        
          3
        
        
          2
        
        
          50
        
        
           
        
        
          (7)
        
        
          Figure 3: Simplified model of the stress pulse.
        
        
          Equations (5) to (7) allows to evaluate the magnitude of
        
        
          the mass and the falling height to obtain a maximum force F
        
        
          max
        
        
          according to the elastic constant
        
        
          
            k
          
        
        
          
            e
          
        
        
          of the cushion material.
        
        
          From Figure 2, the equilibrium equation can be derived
        
        
          as:
        
        
          (8)
        
        
          
            aMM F F F
          
        
        
          
            p
          
        
        
          
            s
          
        
        
          
            k c d
          
        
        
          )
        
        
          (
        
        
             
        
        
          Where
        
        
          
            M
          
        
        
          
            s
          
        
        
          and
        
        
          
            M
          
        
        
          
            p
          
        
        
          are the mass of the pile and the soil
        
        
          respectively and
        
        
          
            a
          
        
        
          is the acceleration of the movement.
        
        
          Equation (8) can be rewritten in terms the resistant forces as a
        
        
          function of the dynamic parameter
        
        
          
            F
          
        
        
          
            c
          
        
        
          
            = c v
          
        
        
          , and
        
        
          
            F
          
        
        
          
            k
          
        
        
          
            = k u
          
        
        
          , being
        
        
          
            u
          
        
        
          and
        
        
          
            v
          
        
        
          the displacement and velocity of displacement
        
        
          respectively:
        
        
          (9)
        
        
          
            aMM uk vc F
          
        
        
          
            p
          
        
        
          
            s
          
        
        
          
            d
          
        
        
          )
        
        
          (
        
        
             
        
        
          Dynamic Force
        
        
          Equation (9) allows determine dynamic influence on the
        
        
          measured force at the point of where the velocity becomes zero
        
        
          and thereafter correcting the measured force by the dynamic
        
        
          effect.
        
        
          Fd
        
        
          Mp
        
        
          2 TESTING PROCEDURE.
        
        
          Figure 4 and 5 sketch the testing setup and electronic devices
        
        
          used for the pseudoestatic load test. This loading design
        
        
          generates a time-controlled load which will depend on the
        
        
          magnitude and height of the falling mass, and geometry and
        
        
          elastic properties of the elastomeric cushion included between
        
        
          the mass and head of the pile. The force pulse is captured by a
        
        
          load cell placed below the cushion. The displacement of the pile
        
        
          is obtained from the double integration of the signals captured
        
        
          by two accelerometer placed on the shaft and below one
        
        
          diameter from top of the pile. The weight of the mass to be used
        
        
          ranges between 5% and 10% of the servicebility capacity of the
        
        
          pile. The test requires the continuous increment of the height of
        
        
          drop of the mass. The output of the conditioners is then
        
        
          digitized by the dynamic analyzer and conveniently stored for
        
        
          subsequent laboratory analysis. In addition to the equipment
        
        
          shown, a proximeter is placed to capture displacements and
        
        
          permanent settlement of the pile. The maximum testing load is
        
        
          obtained when a permanent displacement is generated or until
        
        
          the 50% of the service load is reached.
        
        
          Figure 4. Testing setup for the pseudoestatic load test.
        
        
          Figure 5. Testing electronic devices used for the pseudoestatic load test.
        
        
          The impact mass can be made at the site usually employing a
        
        
          concrete slab or a steel casing filled with concrete depending on
        
        
          its size. For the purpose of centering the load, steel bars are used
        
        
          as guides for obvious safety reasons and ensuring the impact of
        
        
          the mass be centered avoiding the generation of moments. For
        
        
          the purpose of preventing the damage of the pile by the
        
        
          application of impact on the mass, the shaft is increased (1.5 to
        
        
          2 times the diameter) by means of a steel case of the same
        
        
          diameter of the shaft. In all cases, the accelerometers must be
        
        
          positioned below this extension or in a window made on it. The
        
        
          Spring
        
        
          +
        
        
          Force
        
        
          Ms
        
        
          Damping
        
        
          Force
        
        
          F
        
        
          c
        
        
          F
        
        
          
            k
          
        
        
          
            c
          
        
        
          
            k
          
        
        
          Amplitude (KN)
        
        
          T
        
        
          t
        
        
          50
        
        
          Time
        
        
          Falling Weight
        
        
          Cushion
        
        
          Pile
        
        
          Steel
        
        
          Load Cell
        
        
          Case
        
        
          Accelerometer
        
        
          Load cell
        
        
          Signal Conditioner
        
        
          Signal Recorder
        
        
          
        
        
          Signals from
        
        
          Signals from load cell
        
        
          Pile
        
        
          Signal Processor