Abstract:The paper proposes an approach to studying the nonlinear vibrations of thin cylindrical shells filled with a fluid and subjected to a combined transverse-longitudinal load. Methods of nonlinear mechanics are used to find and analyze periodic solutions of the system of equations that describes the dynamic behavior of the shell when the natural frequencies of the shell and the frequencies of both periodic forces are in resonance relations Keywords: elastic cylindrical shell, ideal incompressible fluid, combined … Show more
“…Karagiozis et al [110] developed two numer ical models based on Donnell's non linear theory with and with out in plane inertia to study non linear vibrations of clamped fluid filled shells. In a series of papers Koval'chuk and Kruk [111,112], Koval'chuk et al [113] and Kubenko et al [114] discussed the problem of non linear forced vibrations of completely filled simply supported circular cylindrical shells using Donnell's non linear shallow shell theory and the Krylov Bogolyubov Mitro pol'skii averaging technique. Particularly, in Refs.…”
Section: Fluid Structure Interaction For Shells Containing Still Fluidmentioning
International audienceThe present literature review focuses on geometrically non linear free and forced vibrations of shells made of traditional and advanced materials. Flat and imperfect plates and membranes are excluded. Closed shells and curved panels made of isotropic, laminated composite, piezoelectric, functionally graded and hyperelastic materials are reviewed and great attention is given to non linear vibrations of shells subjected to normal and in plane excitations. Theoretical, numerical and experimental studies dealing with particular dynamical problems involving parametric vibrations, stability, dynamic buckling, non stationary vibrations and chaotic vibrations are also addressed. Moreover, several original aspects of non linear vibrations of shells and panels, including (i) fluid structure interactions, (ii) geometric imperfections, (iii) effect of geometry and boundary conditions, (iv) thermal loads, (v) electrical loads and (vi) reduced order models and their accuracy including perturbation techniques, proper orthogonal decomposition, non linear normal modes and meshless methods are reviewed in depth
“…Karagiozis et al [110] developed two numer ical models based on Donnell's non linear theory with and with out in plane inertia to study non linear vibrations of clamped fluid filled shells. In a series of papers Koval'chuk and Kruk [111,112], Koval'chuk et al [113] and Kubenko et al [114] discussed the problem of non linear forced vibrations of completely filled simply supported circular cylindrical shells using Donnell's non linear shallow shell theory and the Krylov Bogolyubov Mitro pol'skii averaging technique. Particularly, in Refs.…”
Section: Fluid Structure Interaction For Shells Containing Still Fluidmentioning
International audienceThe present literature review focuses on geometrically non linear free and forced vibrations of shells made of traditional and advanced materials. Flat and imperfect plates and membranes are excluded. Closed shells and curved panels made of isotropic, laminated composite, piezoelectric, functionally graded and hyperelastic materials are reviewed and great attention is given to non linear vibrations of shells subjected to normal and in plane excitations. Theoretical, numerical and experimental studies dealing with particular dynamical problems involving parametric vibrations, stability, dynamic buckling, non stationary vibrations and chaotic vibrations are also addressed. Moreover, several original aspects of non linear vibrations of shells and panels, including (i) fluid structure interactions, (ii) geometric imperfections, (iii) effect of geometry and boundary conditions, (iv) thermal loads, (v) electrical loads and (vi) reduced order models and their accuracy including perturbation techniques, proper orthogonal decomposition, non linear normal modes and meshless methods are reviewed in depth
“…are subjected to combined vibratory loading of various types. The dynamic behavior of shells filled with a fluid is more intensive under combined two-frequency vibratory loading [10,11] than under single-frequency loading [8,12].Here we will discuss test data on the nonlinear dynamic deformation of a glassfiber-reinforced plastic shell (empty or filled) subjected to longitudinal kinematic two-frequency vibrational excitation. Our primary task is to establish and analyze the relationship between the two excitation frequencies and the natural frequencies of the shell and the amplitude of the kinematic loading that cause the most intensive deformation of the shell and to analyze the effect of the filler and the way the excitation frequency varies on these processes.…”
mentioning
confidence: 99%
“…are subjected to combined vibratory loading of various types. The dynamic behavior of shells filled with a fluid is more intensive under combined two-frequency vibratory loading [10,11] than under single-frequency loading [8,12].…”
Experimental results on the nonlinear dynamic deformation of the elastic wall of a glassfiber-reinforced plastic cylindrical shell (either "dry" or filled) during beating caused by kinematic two-frequency loading are discussed. It is revealed that the nonlinear deformation of a shell undergoing beating, especially at the two close frequencies of the modes n = 3 and n = 5, can be accompanied by the alteration of amplitude and deformation mode between one mode n = 3 and combined mode (n = 3) + (n = 5) and the alternation of one mode n = 3 between a traveling wave and a standing wave Introduction. The deformation of elastic cylindrical shells is strongly dependent on major factors (external periodic loading) and other factors. For example, the presence of a filler (fluid or loose material) in thin-walled cylindrical shells may result in compound multimode or multiwave dynamic deformation under certain conditions (free vibraions or external periodic loads). Many theoretical and experimental studies [2, 3, 6-9, 12-14] address the deformation of shell structures and nonlinear and resonant phenomena caused by the imposition and nonlinear interaction of several flexural vibration modes, which create preconditions for the occurrence of complex deformation modes (such as traveling circumferential waves, chaotic processes, etc.) under single-frequency excitation. It was established that even the mode shape a shell takes under purely harmonic loads can affect its dynamic instability domains (DID) [4]. For example, the principal DID of a cylindrical shell is located lower on the frequency axis and is considerably wider than the DID of a shell with alternating curvature. Such a situation is typical for composite shells [1,8]. Therefore, experimental studies of the vibratory and wave processes in composite shell structures interacting with a fluid are of current importance. As indicated in [5], experimental methods not only give a true picture of the behavior of mechanical structures under varying loads, but also make it possible to identify the limits of validity of theoretical models. This fact was confirmed by holographic interferometry studies of the natural frequencies and modes of isotropic circular cylindrical shells.An important task of solid mechanics is to study the nonlinear vibrations (with large deflections) of thin-walled laminated shells under combined vibratory loading. When in service, real shell structures with fluid used in aircraft and rocket technology, chemical engineering, etc. are subjected to combined vibratory loading of various types. The dynamic behavior of shells filled with a fluid is more intensive under combined two-frequency vibratory loading [10,11] than under single-frequency loading [8,12].Here we will discuss test data on the nonlinear dynamic deformation of a glassfiber-reinforced plastic shell (empty or filled) subjected to longitudinal kinematic two-frequency vibrational excitation. Our primary task is to establish and analyze the relationship between the two excitation frequencies and th...
“…When in service, however, real shell structures used in aircraft and rocket technology, space transportation systems, chemical engineering etc., are subjected to combined vibratory loading. In this connection, some tests were performed to study the dynamic behavior of shells filled with a fluid and subjected to longitudinal-and-transverse and compound two-frequency vibrational excitation [4,10,17,18].Here we will discuss test data on the nonlinear dynamic deformation of the elastic wall of a glassfiber-reinforced plastic shell (empty or filled) subjected to two-frequency vibrational excitation. Our primary task is to find the combination of the two excitation frequencies and the natural frequencies of the "dry" and filled shells and the amplitude of the vibrational load that cause the most intensive deformation of the shell wall and to analyze the associated processes and the effect of the filler on them.…”
mentioning
confidence: 99%
“…When in service, however, real shell structures used in aircraft and rocket technology, space transportation systems, chemical engineering etc., are subjected to combined vibratory loading. In this connection, some tests were performed to study the dynamic behavior of shells filled with a fluid and subjected to longitudinal-and-transverse and compound two-frequency vibrational excitation [4,10,17,18].…”
We discuss test data on the nonlinear dynamic deformation of the elastic wall of a cylindrical glassfiber-reinforced shell (empty or filled) subject to radial two-frequency excitation. It is revealed that such processes can be accompanied (especially at the lowest resonant frequencies) by the cyclic variation in the amplitude and deformation mode between traveling and standing circumferential wave Introduction. An important task of solid mechanics is to study the nonlinear vibrations (with large (of the order of the thickness) deflections) of thin-walled shells made of laminated composites among which glass-reinforced plastics are most popular [16]. Many publications [1-3, 5-9, 11-16, etc.] address the deformation of shell structures and nonlinear and resonant phenomena caused by the superimposed and nonlinearly interacting flexural vibration modes, which create preconditions for the occurrence of complex deformation modes (such as traveling circumferential waves, chaotic processes, etc. under single-frequency excitation). When in service, however, real shell structures used in aircraft and rocket technology, space transportation systems, chemical engineering etc., are subjected to combined vibratory loading. In this connection, some tests were performed to study the dynamic behavior of shells filled with a fluid and subjected to longitudinal-and-transverse and compound two-frequency vibrational excitation [4,10,17,18].Here we will discuss test data on the nonlinear dynamic deformation of the elastic wall of a glassfiber-reinforced plastic shell (empty or filled) subjected to two-frequency vibrational excitation. Our primary task is to find the combination of the two excitation frequencies and the natural frequencies of the "dry" and filled shells and the amplitude of the vibrational load that cause the most intensive deformation of the shell wall and to analyze the associated processes and the effect of the filler on them.1. Test Specimen, Equipment, and Procedure. The test specimen was an elastic glassfiber-reinforced plastic cylindrical sandwich shell with length N sh = 900 mm, inside diameter D sh = 320 mm, and wall thickness d sh = 0.68 mm. The shell was fixed vertically, with its lower end inserted into the ring groove filled with epoxy resin in a disk and the upper end free. The disk was fixed to a foundation. A VEDS-100 electrodynamic shaker was used to excite transverse vibrations of the shell. The shaker table was in elastic contact with the lateral surface of the shell at a point located at 0.3N sh from the lower end. To produce two-frequency vibrational excitation, we used a generator built in the frame of the shaker and an external Robotron generator (one of them was used for single-frequency excitation). The vibroaccelerations of the shaker table and the shell wall were measured with IS-318 and D-14 transducers operating with the measuring unit of the shaker and an AD-1 microtransducer (with a mass of about 1 g) with a VShV-3 device. The signals (amplitudes, frequencies) from the transducers were a...
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