Results 241 to 250 of about 169,867,477 (285)
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Vibration coupling in continuous belt and band systems
Journal of Sound and Vibration, 1985Small transverse oscillation of an endless band supported by wheels couples the response of the free spans of the band to oscillation of the wheels. The coupling arises from the finite curvature of the free spans of the band when its bending stiffness is finite.
C.D. Mote, W.Z. Wu
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Impact damper for axial vibration of a continuous system
Proceedings of the Institution of Mechanical Engineers, Part C: Journal of Mechanical Engineering Science, 2015Application of Impact damper for reduction of vibration amplitude through momentum transfer is now well established. However, no literature is available for the effect of an impact damper on axial vibration of a rod as a continuous system. The equation for axial vibratory displacement of the rod, fixed at one end and a lumped mass at the other end, is ...
SB Sanap, SY Bhave, PJ Awasare
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Vibration of a continuous system with clearance and motion constraints
International Journal of Non-Linear Mechanics, 2000zbMATH Open Web Interface contents unavailable due to conflicting licenses.
Metallidis, P., Natsiavas, S.
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Principal Trajectories of Forced Vibrations for Discrete and Continuous Systems
Meccanica, 2000The author shows some relations between linear normal modes and principal directions. He considers a linear \(n\)-degree-of-freedom forced system \(M\ddot{\mathbf x}+K\mathbf x=\mathbf p(\omega t)\), where \(\mathbf x(t)\in R^n\), \(M\) and \(K\) are constant mass and stiffness \(n\times n\)-matrices respectively, and \(\mathbf p(\omega t)\) is a ...
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Random Vibrations of Discrete and Continuous Systems
1988The topic of random vibrations of discrete and continuous systems is treated in four papers as follows. 1. Correlation and Spectral Analysis A Brief Outline 2. Measurement of Characteristics of Stationary Random Processes 3.
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Random Vibrations of Linear Continuous Systems
1984In this and the following chapters, we shall consider forced vibrations of linear systems subjected to random loadings. These problems have been thoroughly investigated for systems with a finite number of degrees of freedom; all the necessary information and illustrative examples were given in Sections 2.1 and 2.2.
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Vibration Analysis of Continuous Systems by Dynamic Discretization
Journal of Mechanical Design, 1980An equivalent mass matrix may be defined, for a segment of a continuous system, as one which retains precisely the dynamic properties of the original segment in discretized form. Dynamic Discretization, which makes use of a particular form of Stodola iteration, progressively generates the equivalent mass matrix in ascending powers of frequency squared,
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