Abstract

AbstractThe propagation characteristics of F‐(flexural) wave and the reflection from vertical cracks in pipe‐piles subjected to an eccentric vertical excitation were numerically investigated using elastodynamic finite integration technique (EFIT). The accuracy of the self‐written code was validated by comparing computed results against the measured data. The snapshots of circumferential, radial and vertical velocities in intact and cracked pipe‐piles, as well as the velocity histories of the pile‐top were presented. It is found that not only L‐(longitudinal) wave (corresponding to axisymmetric mode) but also F‐wave (corresponding to non‐axisymmetric mode) can be excited in pipe‐piles subjected to an eccentric vertical excitation. F‐wave causes motion in all directions, while L‐wave only causes vertical motion. The three‐dimensional (3‐D) interference is weak at 90° away from the excitation position for circumferential velocity response, while at 45° or 135° for radial velocity response. The reflected F‐wave (RFW) from the pipe‐toe has multiple peaks due to the dispersion effect of F‐wave. Reflection occurs when F‐wave encounters vertical cracks, while L‐wave is not sensitive to vertical cracks. The intensity of RFW from vertical cracks varies with excitation‐and‐sensor modes. For shallow vertical cracks, the RFW strength varies with the sensor positions; while the intensity of the RFW caused by deep vertical cracks varies little with the sensor positions. With the increase of crack length, the strength of the first arrival RFW due to the vertical crack has no obvious change; however, the strength of RFW from the pile‐toe decreases.

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