Asymptotic Description of Flutter Amplitude Saturation by Nonlinear Friction Forces

Figure 41: Phase’s space diagram for a test at an angular velocity of 19.36 rpmm Figure 42 shows phase’s plane diagram corresponding to a test at an angular velocity of 14.86

We observe that for certain ξ 1 , ξ 2 > 0, when 0 < ξ < ξ 1 all initial conditions go to the equilibrium with larger norm (the non-healed state), when ξ 2 < ξ < 2 all

Since all free critical points c ξ are symmetric and, by Lemma 6.2, have symmetric orbits, to find all possible stable dynamics of the maps O n,α (z) other than the

3 ξ cDPS , in the ξ sDPS ranges indicated in the panels, for four-jet events in data, selected in the phase space defined in the legend, compared to the result of fitting a

Water gas phase abundance in the TW Hya disk model (from top left to bottom right): standard model (model 1), with 1/1000 of the low ISM metallicity (model 3), C/O ratio of 1.86

Figure 4-8 – Gaussian noise added to the closed loop within the dspace environment 57 Figure 4-9 - Process used to obtain cleaner frequency responses from measured data 58 Figure

Different proxies for growth options ratio to the firm’s total value (GOR) (either MBAR (the market to book assets ratio), Q (Tobin’s Q), or RDsales (the ratio of R&D expenses

In this subsection we present an experiment oriented to check the order of accuracy of the nonlinear cubic splines close to critical points at smooth zones of the function. In order