Abstract:The effect of cubic material nonlinearity on the propagation in a pipe of the lowest axially symmetric torsional wave mode has been investigated in this paper. Two cases, one that the material of the whole pipe is nonlinear, and the second that a small segment of the pipe is nonlinear, have been considered. For the first case, a first and a third harmonic have been obtained by the perturbation method. Analytical expressions for the two cumulative harmonics have been derived. The second case leads to a scatteri… Show more
“…The secondary field generated from the region of nonlinearity contained first-, second-, and third-harmonic components. The second-harmonic component was found to be a result of the quadratic nonlinearity while the first-and third-harmonic components were generated by the effects of cubic nonlinearity [3], which parallels the finding of Wang and Achenbach [2]. This paper considers the interaction of an incident longitudinal wave with a spherical region of constant quadratic and cubic elastic nonlinearity.…”
Section: Introductionsupporting
confidence: 67%
“…Recently, a number of investigators have considered the interaction of an elastic wave with a localized region of elastic nonlinearity [1,2,3]. Tang et al modeled the interaction of an incident longitudinal wave with a region with spatially-dependent quadratic nonlinearity, which was contained in a linear elastic host medium [1].…”
Section: Introductionmentioning
confidence: 99%
“…Wang and Achenbach modeled the interaction of an incident torsional guided wave on a local annular region of cubic nonlinearity [2]. Solutions based on reciprocity found backward and forward propagating waves from the region of nonlinearity, which contained first-and third-harmonic components [2]. Kube then considered the interaction of an incident longitudinal or shear wave with a region of spatially-dependent and generally anisotropic quadratic and cubic nonlinearity encompassed in an otherwise linear host medium [3].…”
In this paper, the interaction of an incident finite amplitude longitudinal wave with a localized region of nonlinearity is considered. This interaction produces a secondary field represented by a superposition of first-, second-, and third-harmonic components. The secondary field is solely a result of the quadratic and cubic elastic nonlinearity present within the region of the inclusion. The second-harmonic scattering amplitude depends on the quadratic nonlinearity parameter β , while the firstand third-harmonic amplitudes depend on the cubic nonlinearity parameter γ. The special cases of forward and backward scattering amplitudes were analyzed. For each harmonic, the forward-scattering amplitude is always greater than or equal to the backward scattering amplitude in which the equality is only realized in the Rayleigh scattering limit. Lastly, the amplitudes of the scattered harmonic waves are compared to predicted harmonic amplitudes derived from a plane wave model.
“…The secondary field generated from the region of nonlinearity contained first-, second-, and third-harmonic components. The second-harmonic component was found to be a result of the quadratic nonlinearity while the first-and third-harmonic components were generated by the effects of cubic nonlinearity [3], which parallels the finding of Wang and Achenbach [2]. This paper considers the interaction of an incident longitudinal wave with a spherical region of constant quadratic and cubic elastic nonlinearity.…”
Section: Introductionsupporting
confidence: 67%
“…Recently, a number of investigators have considered the interaction of an elastic wave with a localized region of elastic nonlinearity [1,2,3]. Tang et al modeled the interaction of an incident longitudinal wave with a region with spatially-dependent quadratic nonlinearity, which was contained in a linear elastic host medium [1].…”
Section: Introductionmentioning
confidence: 99%
“…Wang and Achenbach modeled the interaction of an incident torsional guided wave on a local annular region of cubic nonlinearity [2]. Solutions based on reciprocity found backward and forward propagating waves from the region of nonlinearity, which contained first-and third-harmonic components [2]. Kube then considered the interaction of an incident longitudinal or shear wave with a region of spatially-dependent and generally anisotropic quadratic and cubic nonlinearity encompassed in an otherwise linear host medium [3].…”
In this paper, the interaction of an incident finite amplitude longitudinal wave with a localized region of nonlinearity is considered. This interaction produces a secondary field represented by a superposition of first-, second-, and third-harmonic components. The secondary field is solely a result of the quadratic and cubic elastic nonlinearity present within the region of the inclusion. The second-harmonic scattering amplitude depends on the quadratic nonlinearity parameter β , while the firstand third-harmonic amplitudes depend on the cubic nonlinearity parameter γ. The special cases of forward and backward scattering amplitudes were analyzed. For each harmonic, the forward-scattering amplitude is always greater than or equal to the backward scattering amplitude in which the equality is only realized in the Rayleigh scattering limit. Lastly, the amplitudes of the scattered harmonic waves are compared to predicted harmonic amplitudes derived from a plane wave model.
“…The problem stated in Fig. 1 can be solved by using the reciprocity theorem in an elegant manner [2,3]. The virtual wave can be selected as the free Lamb wave propagating in the plate without material nonlinearity, which is denoted by the state B.…”
Higher harmonics are sensitive to micro-defects, which can be utilized in the development of nonlinear ultrasonic techniques (NLUTs). Thus, the higher harmonic generation by material nonlinearity has attracted considerable attention. However, few works have been done on the elastic wave propagation in a finite structure with a localized region of material nonlinearity. The propagation of the SH wave in a plate with a localized region of quadratic material nonlinearity is investigated in this paper. The nonlinear governing equations are reduced to a set of linear equations at different orders by using the perturbation method. The incident plane SH wave satisfies the zero-order equations. The elastic waves generated by the nonlinear material region can be obtained by solving the first-order equations, whose inhomogeneous terms can be regarded as the equivalent body forces and surface tractions. In the first-order approximation, only the Lamb wave can be generated by the interaction of the SH wave with a region of quadratic material nonlinearity. In this paper, the analytical solution for the generated backward Lamb wave is obtained, whose amplitude varies with a material-dependent constant linearly and with the length of the nonlinear region in the form of a sine function.
“…Recently, a number of investigators have turned to exploiting the effects of cubic material nonlinearity in an effort to measure material degradation of solids using nonlinear ultrasonics. [1][2][3][4] While attention has been primarily given to third-harmonic generation, Wang and Achenbach 3,4 unveiled a significant increase to the fundamental harmonic amplitude because of the combinations of quadratic and cubic nonlinearity. The possibility of extracting material nonlinearity information from the fundamental wave for applications in nondestructive evaluation (NDE) is especially promising.…”
This letter considers the combined effects of quadratic and cubic nonlinearity on plane wave propagation in generally anisotropic elastic solids. Displacement solutions are derived that represent the fundamental, second-, and third-harmonic waves. In arriving at the solutions, the quadratic and cubic nonlinearity parameters for generally anisotropic materials are defined. The effects of quadratic and cubic nonlinearity are shown to influence the amplitude and phase of the fundamental wave. In addition, the phase of the third-harmonic depends on a simple combination of the quadratic and cubic nonlinearity parameters. Nonlinearity parameters are given explicitly for materials having isotropic and cubic symmetry. Lastly, acoustic nonlinearity surfaces are introduced, which illustrate the nonlinearity parameters as a function of various propagation directions in anisotropic materials.
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