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We define that the bias of the estimated directions of the arrival of the sources is calculated by (15).
The acoustic radiation of the aerodynamic sources is calculated in a second step by solving an appropriate system of acoustic equations.
Then the efficiency of active control by point sources is calculated as a function of both frequency and position and comparisons are made between finite and infinite length primary sources.
The likelihood, which represents the error rates caused by multiple sources, is calculated by the formula P(D| g = G) = ∏ i = 1 n P (D i | g = G ) for multiple independent samples D i, where i = 1, 2, …, n, and n is the number of reads.
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The radiation impedances of some commonly used sound sources are calculated.
The risk weight proportions of the risk sources are calculated by Analytic Hierarchy Process (AHP).
The typical performances of such sources are calculated by using a recently developed model.
Energies deposited by alpha particles from these sources were calculated using the SRIM range-energy code.
In the first one, the amplitudes of the individual point sources were calculated by means of the in-duct Green's function.
The heat load and the temperature distribution of the magnet is analyzed by a finite element method, and the upper limits of several heat leak sources are calculated.
Therefore, the distance between the upper and lower point sources and the distance between the left and right point sources were calculated for both fluoroscopic and nuclear images.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com