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The models were capable of describing the experimental data adequately and the parameters were physically acceptable.
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The parameters are physically meaningful variables, and their variation is taken to indicate physical changes responsible for the observed perturbations dB.
The model parameters are physically meaningful and can readily be estimated from measurement data.
The modified Kunii Levenspiel model is well suited for use in scale-up calculations for an industrial reactor as all the parameters are physically reasonable and can be predicted for larger reactors.
The introduction of these parameters is physically necessary because the logs do not allow dimensions to be defined.
The crucial importance of NTF/NTD for multi‐way data analysis applications results from the very large volume of real‐world data to be analyzed under constraints of sparseness and non‐negativity of factors to be estimated, when only non‐negative parameters are physically interpretable.
This corresponds to Hirshfeld's 'rigid-bond' test (Hirshfeld, 1976 ▶) for testing whether anisotropic displacement parameters are physically reasonable (Sheldrick, 1997 ▶) and is in general appropriate for bonded and 1,3-separated pairs of atoms and should hold true for most covalently bonded systems.
Both models were able to describe the experimental observations and the estimated values for kinetic parameters were in physically meaningful order of magnitude.
Instead, we examine to what degree the simple model did represent the unweighted original data, a good representation being essential to the argument that the parameters derived are physically meaningful.
In the first step, sets of feasible attachment locations for the absorbers are identified, and in the second step, the required absorber parameters that are physically realizable are obtained, under the constraints of a tolerable vibration amplitude for the absorber masses.
As we can see from Equations 10 and 11, in either of the works [1] and [3], the parameters which are physically meaningful (i.e., the length of the baseline) in the presented phase-to-height mapping model are hardly analyzed due to the difficulty of isolating these parameters from the calibrated coefficients.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com