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Main damping factor

For agiven set of m possible damper locations, find the positions of dampers and the value of their main damping factors. which minimize the objective function (1) and fulfill the explicit constraints of Equation (2) and other implicit constraints mentioned above. [Pg.53]

Here, the objective function is the maximum value of the modulus of the transfer function of horizontal displacement for the top floor, evaluated at the fundamental natural frequency of the frame with dampers. This function is the appropriate element of vector H(A) = —H(A)Mr defined above. The values of weight coefficients are equal to zero except for one of them, which is equal to 1. The modulus of transfer function of different kinds was widely used in the objective function considered by Take waki (2009). Itis assumedthat the value of the main damping factor is c 3 = 8.675 MNs/m and that the total capacity ofthe dampers is (7 = 69.4 MNs/m. Thismeans... [Pg.66]

The two main conditions on the damping factor y is that it should be large enough to remove as many integrals as possible while small enough to retain the accuracy of the calculation. The optimum value for y is yet to be determined. [Pg.9]

The temperature dependence of the individual linewidth, eq. (21), is rather complicated. At very low temperatures the Langevin function in this equation becomes saturated for the majority of the nanoparticles, so that the main mechanism of this dependence is the thermal modulation of the magnetic anisotropy energy. Indeed, one can see from figure 8 (bottom) that the Ar temperature dependence provides a good estimate of the experimental low-temperature linewidth. As the damping factor linearly depends on the linewidth, it follows the same temperature dependence [11],... [Pg.46]

Dynamic mechanical properties exhibit side chain or branch motions short main chain segment motions, main chain segmental motions, recrystallization, and melting. These transitions are observed as inflections in the storage modulus curve with temperature, peaks in either the loss modulus or damping factor (tan( )) curves. Figure 3.11 shows the dynamic mechanical spectroscopy (DMS) of a ZN-VLDPE at 1 Hz in tensile mode. The glass transition temperature (maxima of the loss modulus... [Pg.78]

The REVERB model for main loop operation is shown in Figure 3.9-2. The parametric input include cavity volumes, window areas, density, and damping factors. The circulator is modeled as two acoustic power sources, one at the circulator inlet and one at the outlet assuming 90 percent of the power is released downstream and 10 percent upstream. [Pg.218]

K, The position of main HgTe-line for p-type is 118 cm-i at 30 fC and is the same as for n-type sample while the oscillator strengths of these lines for n- and p-type samples are drastically different 62500 cm-2 for w-type and 39000 cm-2 for p-type, respectively. The damping factor is nearly two times larger for p-type Hgo,s Cdo,i Te because the line shape is much asymmetric and wider in comparison with the w-type Hgo s Cdo,2 Te. [Pg.473]

The EXAFS amplitude falls off as 1 /R. This reflects the decrease in photoelectron amplitude per unit area as one moves further from the photoelectron source (i.e., from the absorbing atom). The main consequence of this damping is that the EXAFS information is limited to atoms in the near vicinity of the absorber. There are three additional damping terms in Equation (2). The 5 q term is introduced to allow for inelastic loss processes and is typically not refined in EXAFS analyses. The first exponential term is a damping factor that arises from the mean free path of the photoelectron (A(k)). This serves to limit further the distance range that can be sampled by EXAFS. The second exponential term is the so-called Debye-Waller factor. This damping reflects the fact that if there is more than one absorber-scatterer distance, each distance will contribute EXAFS oscillations of a... [Pg.165]

Dynamic vibration absorption handles vibrational energy and reduces the vibration of the main vibrating system by a dynamic vibration absorption device with a mass (w), spring constant (k), and viscosity damping coefficient (c). As dynamic vibration absorption is effective only under optimum conditions, it is necessary to optimize the dynamic vibration system prior to use by analyzing the mode of ftie vibration of the source. The optimization can be achieved by controlling die characteristic frequency, damping factor, mass, and installation location (see Fig. 3). [Pg.334]

A viscous damping term was added that depended on a stadium function /, which smoothly increased from 0 to 1 with increasing distance from the center of the simulation cell, and y is a friction coefficient. The goal was to adsorb sound waves and emitted dislocations and prevent them from reflecting back into the main region. The central conclusion of the work challenged the traditional concept that crack tip velocity was the single most important factor... [Pg.386]

The antomatic voltage regnlation is stabilised by the use of derivative feedback. The source of the feedback is the output of the power amplifier. The output from the derivative, or damping, circuit is deducted from the reference voltage at the summing junction. The damping is mainly determined by the factor Kf. The two time constants Tf and Tf2 result from the components in the feedback measurement and smoothing circuits. [Pg.84]


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