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Considering that none of the resonances shows line broadening or resonance shifting relative to lipid-free αS, each of these modes is separated by an energy barrier sufficiently large to give rise to the slow kinetics observed.
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The modes are separated into three distinct families and each family is handled separately.
Different modes were separated in time domain and dispersive curve of each mode is calculated by FFT.
For the first approach, in the frequency-wavenumber plane modes are separated and thus can be filtered.
This structure is obtained by transformations of the dependent variables such that weakly interacting modes are separated.
The two TEM00 modes are separated in frequency by one FSR of the high finesse cavity ((mathrm{FSR} = c/(2 L)approx1.5mbox{ GHz})), where (L=97mbox{ mm}) is the cavity length.
The measurement of the antisymmetric modes was separated from the measurement of the symmetric mode by the special configuration of the strain gauge sensor systems.
Thereupon, the aerodynamic and aeroelastic components of the pressure modes were separated, and the pressure modal admittance functions were then identified with the isolated aerodynamic components.
Starting from standard hydrodynamic assumptions, the fluid oscillatory modes are separated to an impulsive mode and convective modes through the introduction of a reference frame co-moving with the base of the tank.
The demands for extremely large models are due to large physical domains or the desire to resolve high-frequency levels, at least as long as the different modes are separated, say to 500 Hz.
The results might be quite different if mobile and outreach modes were separated for the NRHS approach.
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