Sentence examples for modes of equation from inspiring English sources

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The two modes of Equation (10) manifest themselves as two resonances in the spectroscopy data.

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By incorporating the description of radiation modes, this equation of natural mode expansions is used to study the coupling among vibration modal amplitudes due to the modal cross-impedances and the convergence of near and farfield solutions.

The different energy levels of atoms are identified with the simple vibrational modes of the wave equation.

The coupling between in-plane, D +, and out-of-plane, D z, modes gives rise to the hybrid mode, which the analysis of Equation (18) shows that this hybrid mode is always unstable.

Assuming deflection with multiple modes of vibration, the governing equation is reduced to a set of nonlinear ordinary differential equations by the Bubnov Galerkin procedure.

This formalism has been applied to the study of the scale scale interaction and information transfer between the first two modes of the truncated Burgers equation.

Our results also indicate that, in the limit of vanishing Mach number, there exist stable discrete modes in addition to the discrete modes of the Orr-Sommerfeld equation.

The primary branch modes are good approximations, in terms of both structure and frequency, to corresponding modes of the continuous governing equations, and offer some improvements over a quadrilateral C-grid scheme.

Considering the orthogonality of the main vibration mode, the equation of motion can be obtained as m_{ii} ddot{q}_{i} + 2m_{ii} omega_{ii} xi_{i} dot{q}_{i} + m_{ii} omega_{ii}^{2} q_{i} = Q_{i} left( t right)quad left( {i = 1,2,3, ldots,n} right), (17 where m ii, ω ii, ( xi_{i} ) and Q i (t) are the ith modal mass, angular frequency, damping ratio and generalized force, respectively.

Asymptotic approximations show that the lowest modes of the prolate spheroidal wave equation are concentrated with an O(1/√c) length scale where c is the "bandwidth" parameter of the prolate differential equation.

This resulted in expressions for perceived velocity, v' (the value of m at the mode of the posterior; Equation 3) and perceived ISD, l' (i.e., v't; Equation 1).

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