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λ i k ( a, t, x ) represents the interaction coefficients ( i, k = 1, 2, …, n, k ≠ i ).
In this paper, we consider the nonlinear Schrödinger equation with variable coefficients i u t + α ( t ) u x x + β ( t ) | u | 2 u = 0, (1).
The procedure is based on two coefficients: (i) a relation between the average error levels and the total CPU time of the analysis process and (ii) a semi-quantitative relation between the volumes of successive solid modelling phases.
From DFT we obtain all microscopic parameters in the pre-factor and activation energy of impurity diffusion coefficients: (i) the correlation factor through a five frequency model, (ii) the impurity jump frequency within the framework of transition state theory and (iii) the free energies of vacancy formation and vacancy solute binding.
Reactivity coefficients, i.e. Doppler, coolant and moderator, show negative values.
They suggest this can be done "by a judicious choice of the coefficients" (i.e. the λ values).
Similar(19)
where the coefficients, a i, b i, c i, and d i, are the spline coefficients with i=1,2,3,..,n-1.
Take fast Fourier transform (FFT) on the LF-MDCT coefficients x(i), i = 1 ,…, M, and the reconstructed HF-MDCT coefficients x ^ (i), i=M+1 ,…, 2M, respectively.
Identification scheme is also developed to determine the proportional coefficient, i.e. the indentation force coefficient.
e,i: Coefficient of gas interchange between bubble and emulsion phases, overall mass transfer coefficient i th compartment (s-1).
The concept of fracture propagation coefficient, i.e., the ratio of energy supplied by injection to fracture energy, is defined.
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