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Free oscillations

There are several other comparable rheological experimental methods involving linear viscoelastic behavior. Among them are creep tests (constant stress), dynamic mechanical fatigue tests (forced periodic oscillation), and torsion pendulum tests (free oscillation). Viscoelastic data obtained from any of these techniques must be consistent data from the others. [Pg.42]

The amplitude drops to zero when the sample is moved from the point of first contact on a distance of the half of the full amplitude of the free-oscillating probe. From this point, a further motion of the sample will cause the cantilever bending upward, similar to what occurred in the contact mode. If the sample motion is reversed the amplitude increases as shown by a dashed curve in Figure 20.2c. [Pg.560]

Decreased deformation of a material specimen vs. time when the specimen is subjected to a free oscillation. [Pg.171]

System s polymer film properties and free oscillation as a fluidized array resists biofouling and iron clogging... [Pg.356]

Exercise. The constants ct and c2 in (2.10) depend on the random term at twice the frequency of the free oscillator. Express them in the spectral density of . [Pg.401]

Figure 9-8. Types of torsion pendulum, (a) Free oscillation apparatus with inertia member supported by test piece (b) free oscillation apparatus with inertial member supported by a fine wire. In both types of apparatus, a lamp and scale is used in conjunction with the mirror to observe the oscillations. The broken lines indicate compensation devices to produce a constant amplitude apparatus... Figure 9-8. Types of torsion pendulum, (a) Free oscillation apparatus with inertia member supported by test piece (b) free oscillation apparatus with inertial member supported by a fine wire. In both types of apparatus, a lamp and scale is used in conjunction with the mirror to observe the oscillations. The broken lines indicate compensation devices to produce a constant amplitude apparatus...
The above equation is an integrodifferential equation that has an unusual structure. Here (co2)1 2 is the frequency of the free oscillator and y is the damping constant. The fourth term on the left-hand side of Eq. (226) has the form of the memory kernel, and its strength is controlled by the dimensionless coupling constant X which contains the contribution from the vertex function. [Pg.132]

Expanding r(r t) in terms of vibrational states [Pg.90]

The extension to more than one dimension is rather straightforward within the time-dependent approach (Heller 1978a, 1981a,b). For simplicity we restrict the discussion to two degrees of freedom and consider the dissociation of the linear triatomic molecule ABC into A and BC(n) as outlined in Section 2.5 where n is the vibrational quantum number of the free oscillator. The Jacobi coordinates R and r are defined in Figure 2.1, Equation (2.39) gives the Hamiltonian, and the transition dipole function is assumed to be constant. The parent molecule in the ground electronic state is represented by two uncoupled harmonic oscillators with frequencies ur and ur, respectively. [Pg.115]

In the resonance region the system oscillates with the external frequency X and with an increased amplitude (entrainment region). Far away from resonance, the internal free oscillations are present. This behaviour is completely absent in systems, where no self-sustained oscillations can exist. A typical example of such a system is a nonlinear conservative system. The resonance diagram has been drawn in Figure 2 for both, the small and the large ampli tude oscillation. [Pg.222]

Figure 8. Regions of different behavior of the externally driven limit cycle of Model 2 (see Figures 5-7) (I) free oscillation (limit cycle with (II) quasi-peri-odic oscillation (III) entrainment (limit cycle with X) (IV) unstable region — onset of traveling waves. Figure 8. Regions of different behavior of the externally driven limit cycle of Model 2 (see Figures 5-7) (I) free oscillation (limit cycle with (II) quasi-peri-odic oscillation (III) entrainment (limit cycle with X) (IV) unstable region — onset of traveling waves.
Seiche sea level oscillations. The level of any basin, being turned out of its equilibrium state by a certain force, returns to its initial position performing decaying oscillations with respect to one or several horizontal lines (nodal lines) until their energy is expended for bottom and coastal friction. These free oscillations are known as seiches (uninodal or multinodal depending on... [Pg.153]

Tidal sea level oscillations. In the Black Sea, tides are formed under the action of the tidal forces in the basin proper, which is limited in size therefore, the tides are small. Over the entire sea area, tides feature a semidiurnal or irregular semidiurnal character. The prevalence of this type of tides is related to the closeness of the semidiurnal period to that of the first mode of free oscillations in the Black Sea (uninodal seishe). [Pg.155]

Woodhouse J. H., Giardine D., and Li X. D. (1986) Evidence for inner core anisotropy from free oscillations. Geophys. Res. Lett. 13, 1549-1552. [Pg.1243]

To find convenient expressions for the storage modulus and the loss tangent for a viscoelastic material under free oscillation in torsion, it is necessary to return to the equation of motion given by... [Pg.275]


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See also in sourсe #XX -- [ Pg.6 , Pg.8 ]




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