The instrument has been modeled in sample modulation mode and experimental results obtained for different materials were compared with simulation data.
To achieve our goal, the approach defines a set of mutation rules that should be applied to the inputs of the controller, a tailored version of a classification of the different controller failure modes, and an experimental setup and testing procedure that is specific to self-adaptive systems.
For an excellent overview of ISFET operation, sensing modes, and important experimental design factors, the reader is referred to a review by P. Bergveld.
Second, numerical simulation results for a single mode equation and experimental results for the beam are given.
The concatenated strong fiber Bragg grating and a weak long period grating are presented for simultaneous temperature and solution concentration measurement in the methods of both detailed coupled-mode theory and experimental analysis, and find two ways which include dual wavelength method and dual parameter method to solve the cross sensitivity problem to ensure higher accuracy and sensitivity.
The methods to eliminate or reduce the high-risk failure modes are proposed and experimental investigations are conducted to validate the proposed solutions.
The design and material parameters that allow to create these localized acoustic modes is discussed, and experimental results of the measured acoustic transmission in PS samples fabricated by electrochemical etching are presented.
There is solid empirical [ 25, 34- 36] as well as theoretical [ 19- 21, 37- 39] support for frequent presence of both modes in eukaryotes, and experimental studies have shown that it is relatively easy in mutational terms to move between a hyperbolic mode and a sigmoidal one [ 25, 34].
A comparison with predictions from some selected mixed-mode cohesive laws and experimental data available in the literature is also included to further validate the proposed mixed-mode law.
The paper discusses an optimum algorithm, in which the contact stiffness coefficients are taken as design variables, aiming at minimizing the sum of squares of eigenfrequency differences between finite element modes and their corresponding experimental modes, based on mode shape identification.
