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For the estimation procedure, a linear regression model continuously fit the data collected up to that point during the calibration session with temperature as the independent variable and pain ratings as the dependent variable.
Applying the proposed procedure, a linear range of 0.08 10 and 0.10 10 μg g−1 was obtained for selenium and arsenic, respectively.
Firstly, in order to obtain a diagnosis of the failure causes, several FEM models with six tiles of a 0.83 m wide and 1.25 mm thickness, including methacrylate skylights in one of them, were built and then solved as a three steps procedure: a linear pre-stress analysis, a buckling analysis and a nonlinear analysis.
At each stage of the iterative procedure, a linear system has to be solved and the Arithmetic Mean method is used.
For the IR procedure, a linear accelerator (Varian Clinac 600 CD; Radiation Oncology Systems LLC, San Diego, CA, USA) with a 4 MV nominal photon energy and a dose rate of 2.3 Gy/min was used.
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Under the optimum conditions, the proposed procedure has a linear range between 0.05 and 2.0 μg ml−1, with a detection limit of 0.02 μg ml−1 for ethamsylate.
This procedure yields a linear parameter-varying structure for the controller that allows higher-gain and hence higher-performance controllers as the states move closer to the origin.
The optimized procedure showed a linear response from 1 to 100 μg L−1 (S=53.7+2.61C, in which S is the net fluorescence and C is iodide concentration in μg L−1).
The preconcentration procedure showed a linear response within the studied concentration range from 3 to 500 μg l−1 of Ni in the feed solution.
This procedure produced a linear standard curve, which was then used to calculate sample cystatin C concentration from sample optical density.
In particular, the procedure is a linear transformation that maps each array's PM intensity distribution, Ij, onto the average PM distribution of all arrays, Iref.
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