Applied Structural and Mechanical Vibrations 2009 Part 15 docx

... eq (15. 16) simplifies to (15. 17) It can be observed that eq (15. 17) is equivalent to eq (15. 12) valid for a voltage amplifier. The differences are that R f and C f now replace R T and ... Fig. 15. 14, since the ground conductor is an integral part of the signal loop and breaking it would interrupt the return path. Fig. 15. 15 Two-wire voltage transmission between transdu...

Ngày tải lên: 10/08/2014, 20:20

... or 180° and real numbers suffice for a complete description. 6.5 Structure and properties of matrices M, K and C: a few considerations A fundamental part of the analysis of MDOF systems and of ... ζ k and the kth frequency ω k can be determined from the kth eigenvecctor and the damping, mass and stiffness matrices. 6.8 Generalized and complex eigenvalue problems: reductio...

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... LLC Applied Structural and Mechanical Vibrations Theory, methods and measuring instrumentation Paolo L.Gatti and Vittorio Ferrari Copyright © 2003 Taylor & Francis Group LLC Applied Structural ... 1959– Applied structural and mechanical vibrations: theory, methods, and measuring instrumentation/Paolo L.Gatti and Vittorio Ferrari. p. cm. Includes bibliographi...

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... recognize eq (4.42) and we understand that the FRF representation gives information on both the magnitude of response and the phase angle of lag between response and excitation. This particular form ... been obtained in Chapter 2 and here it is solved in the undamped and damped cases, considering free vibrations first (homogeneous equation: no forcing external excitation) and th...

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... orders of the perturbation calculation. We then replace K 1 and M 1 by γ K 1 and γ M 1 and express i and p i as (well-behaved and rapidly converging) power series in γ . In the final result ... (or Laplace) transform: h(t) and H( ω ) are a Fourier transform pair and, likewise, h(t) and H(s) are a Laplace transform pair. Unfortunately, both the time-domain and the fr...

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... H( ω ) and hence (7.47) where, for brevity, we write H Re and H Im for the real and imaginary part of H, respectively. In addition, we can express h(t) as (7.48) divide the real and imaginary parts ... Newland, D.E., Mechanical Vibration Analysis and Computation, Longman Scientific and Technical, 1989. Copyright © 2003 Taylor & Francis Group LLC Fig. 7.5 Receptance R22(...

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... clamped and free. Without reference to any particular set of coordinates (rectangular, polar, etc.), we denote by s and n the coordinates in the tangential and normal directions to the contour and ... the differential operators K and M parallels the symmetry of the matrices K and M, the othogononality conditions (6.44) and (6.42b) are the counterpart of eqs (8.128) and the exp...

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... Press, Cambridge, Mass., 1947. 15. Leissa, A.W., Vibration of Plates, NASA SP-160, 1969. 16. Gerardin, M. and Rixen, D., Mechanical Vibrations: Theory and Applications to Structural Dynamics, John ... not difficult and it can be shown that the eigenvalues of the two eigenproblems in which the n×n matrices K and M are obtained by bordering and (of order (n–1)×(n–1)) with the...

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... assumption, the excitation and the response are usually broadband signals (for example, random or impact) and the tests are often performed by using a two channel analyser and a single-input single-output ... f 0 and the phase angle θ . Specifically, from the second of eqs (10.14) it is immediately evident that when we have (10.15a) and, from the first of eq (10.14), (10.15b) Eq...

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... narrow-band and wide-band random processes, these definitions having to do with the form of their spectral densities. Working, in a sense, backwards we can investigate what kind of time histories and ... functions result in narrow-band and wide-band processes. Broadly speaking, a narrow-band process has a spectral density which is very small except within a narrow band of frequencies: i...

Ngày tải lên: 10/08/2014, 20:20