Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Beams free vibrations

Each eigenvalue determines, through Eq. (17.91), a natural frequency of free vibration of the beam, while Eq. (17.89) gives the mode shape function f (x). [Pg.791]

Timoshenko s beam model used by Wang et al. [60] for free vibrations of MWCNTs study it was shown that the frequencies are significantly over predicted by the Euler s beam theory when the aspect ratios are small and when considering high vibration modes. They indicated that the Timoshenko s beam model should be used for a better prediction of the frequencies especially when small aspect ratio and high vibration modes are considered. [Pg.255]

Ansari et al. [78] 2012 Adaptive Inteimo-lecular Reactive Empirical Bond Order (AIREBO) potential (8,8) 8.3-39.1 Vibration characteristics and comparison between different gradient theories as well as different beam assumptions in predicting the free vibrations of SWCNTs... [Pg.258]

Free vibrations of MWCNTs using Timoshenko beam... [Pg.259]

Load response and failure analyses of bars, beams, plates, shells, and mechanical and adhesively bonded Joints are common in structural design, as well as stability and free vibration analyses of bars, plates and shells. These analyses can always be performed with general purpose FE programs. Nevertheless, computer codes developed specifically for these analyses are useful because FE programs are laborious to use. These tools should have the following features ... [Pg.383]

For a column under live load, maximum deformation and internal force of nodal sections are closely related to natural vibration period and vibration mode. Therefore, natural vibration period of a column must be determined for calculating wind load and seismic load of the column (Wei, 1985). Columns used in chemical plants or refinery plants typically have one end fixed and the other free, which may be considered as cantilever beam structures. Tall columns are high-rise flexible buildings with less damping resulting in simplified free vibration (Jeary, 1997). [Pg.101]

Figure 5.6 Free vibration torsion pendulum P, polymer specimen Cl, fixed upper clamp C2, lower clamp fixed to inertia bar W, sliding masses to change moment of inertia M, mirror to reflect light beam... Figure 5.6 Free vibration torsion pendulum P, polymer specimen Cl, fixed upper clamp C2, lower clamp fixed to inertia bar W, sliding masses to change moment of inertia M, mirror to reflect light beam...
Suppose that a microfabricated cantilever beam is to be used as a sensor for detecting the presence of a certain bacterium in a hquid solution see Figure 1.31. Following its fabrication, the beam is first coated with an antibody that is specific to the particular bacterium of interest and its free vibration characteristics are determined. The beam is then dipped into the solution to be tested. If the bacteria of interest are present, they will attach themselves to the surface of the beam, attracted by the antibody. The beam is then removed from the solution and its free vibration characteristics are re-examined. Estimate the influence of an added mass due to the attached bacterium cells, say rib cells each of mass mb, on the fundamental natural frequency of the beam. (The effectiveness of this approach for detection of bacteria has been demonstrated by Ilic et al. (2000).)... [Pg.64]

K. Senthil Kumar, 1. Siva, Jeyaraj, J. Winowlin Jappes, S. Amico, and N. Rajini, Synergy of fiber length and content on free vibration and damping behavior of natural fiber reinforced polyester composite beams. Mater. Des. 56,379 (2014). [Pg.212]

HOSHIYA, M. and SHAH, H.C., Free Vibration of a Beam-Column with Stochastic Properties, Proceedings of the ASCE-EMD Specialty Conference, Purdue University, 1969, pp. 107-111. [Pg.81]

FIG. 7-5. Apparatus of Fujino, Kawai, and Horino for measurement of dynamic Young s modulus of fibers by free vibrations. (A. A ) Chucks (B) sample fibers (C) clamps (D) inertial disc (E) idler pulleys (F) piano wire (C) mirror to reflect light beam (H) weight to adjust static tension. [Pg.163]

E.A. Armanios, A.M. Badir, Free vibration analysis of anisotropic thin-walled closed-section beams. AlAA J. 33(10), 1905-1910 (1995)... [Pg.207]

The tensile strength and stress of the IPMC are measured in the same manner as those of the IP. The bending stiffness of a fully hydrated IPMC sample is estimated using the free oscillation attenuation method. By bending the sample to the appropriate initial displacement, the free vibration response can be recorded. The natural frequency of the cantilever, is obtained from the fast Fourier transform of the free vibration response curve. The stiffness of the IPMC, Egg, is determined using Eq. 4, which is based on the thin cantilever beam theory of material mechanics ... [Pg.137]

Free Vibrations of Hinged Beam of Rectangular Cross Section... [Pg.1604]

In order to examine the influence of shear deformation on the free vibrations of beams in the... [Pg.1604]

Nonlinear Dynamic Seismic Anaiysis, Tabie 1 Material properties, geometric, inertia constants, and shear deformation coefficients of the rectangular cross section of application section Free Vibrations of Hinged Beam of Rectangular Cross Section ... [Pg.1605]

Free Vibrations or Beam with Very Flexible Boundary Conditions... [Pg.1605]

In this application the free vibrations of Timoshenko beams with very flexible boundary conditions is examined, since in this case the natural frequencies and the corresponding modeshapes are highly sensitive to the effects of shear deformation and rotary inertia (Aristizabal-Ochoa 2004). Thus, the linear free vibration analysis of piimed-free beams of length L = 5.0 m of various cross sections is examined (p = 2.40 tn/m, E = 25.42 GPa, G = 11.05 GPa). In Table 3 the geometric and inertia constants as well as the shear correction factors of the examined cross sections are presented (re = 1/a). The differential equations for the linear free vibrations of this special case can be obtained by Eq. 14 for zero axial stress resultant and external force as... [Pg.1605]

Nonlinear Dynamic Seismic Analysis, Fig. 3 Free vibration period ratios TITq at various amplitude ratios Wmax/r for beam slenderness //r = 50 of the simply... [Pg.1606]

Forced Vibrations or Beam of Hollow Rectangular Cross Section Under Biaxial Bending In order to examine the influence of shear deformation on the free vibrations of beams in the geometrically nonlinear range, a clamped beam... [Pg.1606]

Nonlinear Dynamic Seismic Analysis, Table 3 Geranetric constants of the pinned-free beam of application section Free Vibrations or Beam with Veay Flexible Boundary Conditirais ... [Pg.1606]

Free Vibrations of Beam of Thin-Walled l-Section Without STMDE... [Pg.1615]

Fig. 11 Time history of the twisting moment at the left end of the beam of application section Free Vibrations of Beam of Thin-Walled I-Section Without STMDE, for the case of initial twisting rotations dxa x)... Fig. 11 Time history of the twisting moment at the left end of the beam of application section Free Vibrations of Beam of Thin-Walled I-Section Without STMDE, for the case of initial twisting rotations dxa x)...
Fig. 16 Axial load F -torsional fundamental natural frequency cOf relation of Eq. 50 (Mohri et al. 2004) along with pairs of values (cty, N) obtained for application section Free Vibrations of Beam of Thin-walled I-Section with STMDE (AEM)... Fig. 16 Axial load F -torsional fundamental natural frequency cOf relation of Eq. 50 (Mohri et al. 2004) along with pairs of values (cty, N) obtained for application section Free Vibrations of Beam of Thin-walled I-Section with STMDE (AEM)...

See other pages where Beams free vibrations is mentioned: [Pg.112]    [Pg.789]    [Pg.255]    [Pg.256]    [Pg.33]    [Pg.1605]    [Pg.1606]    [Pg.1606]    [Pg.1615]    [Pg.1617]    [Pg.1620]    [Pg.1620]    [Pg.1621]    [Pg.1622]    [Pg.1624]    [Pg.1634]   
See also in sourсe #XX -- [ Pg.789 , Pg.796 ]




SEARCH



Free vibrations

© 2024 chempedia.info