Sentence examples for damp time from inspiring English sources

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The influence of different damping time on the weld strength of various materials is investigated.

The improved expression includes the effects on the collision damping time of the particle material coefficient of restitution and of non-equilibrium particle velocity distributions.

We perform optimum vibration damping time design and demonstrate that by optimizing the thickness and the properties of the coating layers, substantial improvements can be achieved in the vibration damping characteristics of viscoelastic beams and plates.

In the nonlinear theory, the linear electron Landau damping effects on ion acoustic solitary wave have been investigated in an electron-ion plasma neglecting the particle trapping effect under the assumption that the particle trapping time is much larger than the Landau damping time [1, 13].

In this paper we focus on particle flows in which the particles have no liquid films and report on an improved expression we have developed for the collision damping time of particle velocity fluctuations used in the BGK approximation.

In order to simulate the power swing, displacement angle of source A is considered as: delta (t)={delta}_0+kcdot {e}^{-t/tau}cdot sin left(2pi cdot {f}_{slip}cdot tright) (2 where k = 5 is constant scaling coefficient, τ = 0.3 is the damping time constant and f slip  = 1Hz is the slip frequency.

Maintenance of the pressure at 1.01325 bar was carried out on the basis of Langevin piston Nose-Hoover[42], [43] method with a barostat oscillation time of 100 fs, a barostat damping time of 50 fs and a barostat noise temperature of 310 K. 50 ps of equilibration period were performed for each system after minimization and annealing steps.

For all equilibrium simulation, constant temperature (T = 300 K) was enforced using Langevin dynamics with a damping coefficient of 5 ps−1, constant pressure (p=1 atm) was enforced through the Nosé-Hoover Langevin piston method with a decay period of 100 fs and a damping time constant of 50 fs.

The sensitivity study is presented in Fig. 4. The relation between parameters of the initial and the reduced models is represented in Fig. 5. Damping time of the oscillations is most sensitive to parameters k14 p 1, k18, k20 p, k21 p 1, k22, k26, C0.

The wiggler will influence many aspects of beam dynamics: linear motion, dynamic aperture, emittance, damping times, etc.

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