Abstract:Abstract:The static problem for elastic shallow cables suspended at points at different levels under general vertical loads is addressed. The cases of both suspended and taut cables are considered. The funicular equation and the compatibility condition, well known in literature, are here shortly re-derived, and the commonly accepted simplified hypotheses are recalled. Furthermore, with the aim of obtaining simple asymptotic expressions with a desired degree of accuracy, a perturbation method is designed, using… Show more
“…Finally, it should be noted here that in our multi-parameter perturbation method, the parameters are not dependent on each other, thus leading to a large number of independent perturbation equations. However, in the literature, there exists an alternative and much more efficient method [ 38 , 39 , 40 , 41 , 42 ], in which all the parameters (irrespective of their number) are perturbed together along straight lines in the parameter space, thus formally re-conducting the multi-parameter case to that of a single parameter. At the end of the procedure, however, the parameters can be varied independently, since the exploring straight line can be freely chosen.…”
In this study, we use a multi-parameter perturbation method to solve the problem of a functionally graded piezoelectric cantilever beam under combined loads, in which three piezoelectric coefficients are selected as the perturbation parameters. First, we derive the two basic equations concerning the Airy stress function and electric potential function. By expanding the unknown Airy stress function and electric potential function with respect to three perturbation parameters, the two basic equations were decoupled, thus obtaining the corresponding multi-parameter perturbation solution under boundary conditions. From the solution obtained, we can see clearly how the piezoelectric effects influence the behavior of the functionally graded piezoelectric cantilever beam. Based on a numerical example, the variations of the elastic stresses and displacements as well as the electric displacements of the cantilever beam under different gradient exponents were shown. The results indicate that if the pure functionally graded cantilever beam without a piezoelectric effect is regarded as an unperturbed system, the functionally graded piezoelectric cantilever beam can be looked upon as a perturbed system, thus opening the possibilities for perturbation solving. Besides, the proposed multi-parameter perturbation method provides a new idea for solving similar nonlinear differential equations.
“…Finally, it should be noted here that in our multi-parameter perturbation method, the parameters are not dependent on each other, thus leading to a large number of independent perturbation equations. However, in the literature, there exists an alternative and much more efficient method [ 38 , 39 , 40 , 41 , 42 ], in which all the parameters (irrespective of their number) are perturbed together along straight lines in the parameter space, thus formally re-conducting the multi-parameter case to that of a single parameter. At the end of the procedure, however, the parameters can be varied independently, since the exploring straight line can be freely chosen.…”
In this study, we use a multi-parameter perturbation method to solve the problem of a functionally graded piezoelectric cantilever beam under combined loads, in which three piezoelectric coefficients are selected as the perturbation parameters. First, we derive the two basic equations concerning the Airy stress function and electric potential function. By expanding the unknown Airy stress function and electric potential function with respect to three perturbation parameters, the two basic equations were decoupled, thus obtaining the corresponding multi-parameter perturbation solution under boundary conditions. From the solution obtained, we can see clearly how the piezoelectric effects influence the behavior of the functionally graded piezoelectric cantilever beam. Based on a numerical example, the variations of the elastic stresses and displacements as well as the electric displacements of the cantilever beam under different gradient exponents were shown. The results indicate that if the pure functionally graded cantilever beam without a piezoelectric effect is regarded as an unperturbed system, the functionally graded piezoelectric cantilever beam can be looked upon as a perturbed system, thus opening the possibilities for perturbation solving. Besides, the proposed multi-parameter perturbation method provides a new idea for solving similar nonlinear differential equations.
“…Perturbation methods are powerful asymptotic techniques that are widely used in a large variety of scientific research fields, ranging from direct problems concerning linear and nonlinear dynamics, stability and bifurcation [42][43][44][45] to inverse problems dealing with modal identification, optimal spectral design, damping and damage detection [46][47][48][49][50][51]. Perturbation methods are also classical and well-established strategies to study different problems in cable mechanics, including static behaviors [52,53], linear and nonlinear dynamic phenomena [2,3,[54][55][56][57], aerodynamic instabilities [58][59][60], active vibration control [61,62].…”
Section: Perturbation Solution Of the Direct Problemmentioning
“…Under self-weight, the cable hangs on points and in the vertical plane, spanned by the unit vectors (a , a ), and occupies the equilibrium configuration shown in thin line in Figure 1. Possible evaluation of the equilibrium configuration via perturbation methods is discussed in [15,16]. An orthogonal uniform wind U = a is assumed to flow, which causes the cable to reach an unknown current configuration, shown in thick line in Figure 1.…”
The aeroelastic stability of horizontal, suspended, shallow, iced cables is studied via a continuum model. Both external and internal damping, consistent with the Rayleigh model, are taken into account. The quasi-static theory of the aerodynamic forces is applied. An in-plane nonlinear model of galloping is formulated, displaying the importance of internal damping, both on the critical velocity and on the limit-cycle amplitude. A perturbation procedure is developed for nonlinear analysis in nonresonant conditions (monomodal galloping). The modification of the galloping mode due to quadratic nonlinearities is studied, and its real or complex character is discussed.
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