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Using Equations 22 and 23, it may be observed that symmetric and antisymmetric wave modes in general laminates cannot be decoupled.
A coaxial erbium doped fiber (EDF) designed to show inherent gain flattening for one of its propagating modes in general supports two or more modes with different gains.
A new, fast, and accurate numerical algorithm to assess stability against ideal ballooning modes in general three-dimensional magnetic configurations of interest to controlled thermonuclear fusion is described.
Results show that the LDF model is valid for water-sorbing heat exchanger and the moisture uptake experiences four different modes in general, including non-isothermal adsorption, near-isothermal adsorption, capillary condensation and cooling-based condensation.
In fact, if the underlying lattice is translational invariant, one obtains that two different modes, in general of the form e i k x, are orthogonal, e.g. ⟨ ϕ k 1 ( x ), ϕ k 2 ( x ) ⟩ = ∫ e i ( k 1 - k 2 ) x d x = δ ( k 1 - k 2 ).
An examination of the wave-train closure principle shows that, although the frequency equations obtained by using the principle are identical to those derived from the wave evolution results, the principle does not describe the realistic process of the formulation of vibration modes in general.
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Also, the higher visual security of frequency mode as compared to spatial store mode in general is confirmed numerically.
Multiple boreholes heat exchangers (BHEs) are widely used in ground source heat pump systems (GSHPS) and are operated in intermittent mode in general.
It has been found that near the gamma point (center of the Brillouin zone), the dispersion relationship for the TM mode is independent of the propagation direction, while the TE mode in general depends on the electromagnetic waves propagation direction.
However, in a PnC, these modes will in general be coupled depending on the symmetry of the particular PnC.
These residues lie at the hinge axes of rotational motion identified by the residue mobility profiles in Fig. 2. The correlation coefficients of the residue fluctuation vectors between p1-p6WT and LP1′Fp1-p6D30N/N88D in both modes are in general higher than they are between p1-p6WT and p1-p6D30N/N88D.
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