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According to Steinau et al. [31], who recommended four to six hourly control measurements in cases of impending IAH in children, IAP is measured at least six hourly by about 50% of participants claiming to perform measurements.
According to Steinau et al. [ 31], who recommended four to six hourly control measurements in cases of impending IAH in children, IAP is measured at least six hourly by about 50% of participants claiming to perform measurements.
However, with the detection limit reported therein, this system is limited to measurements in cases of significant mercury exposure.
However, these models are based on continuum or scattering theory, and therefore cannot explain the broadband measurements in cases where scattering and non-scattering losses co-exist.
We have used the mean of the three measurements in cases, where elemental composition data were needed, and the three results separately, where X-ray spectra were needed.
The splitting of lens nuclei resulted in two complementary specimens, thus providing an avenue for additional measurements in cases of specimen damage or artifacts of preparation.
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Observed differences result from simplifications of mathematical model, inaccuracy of the kinetic and vapour-liquid equilibrium description for highly nonideal, multicomponent system and from precision of experimental measurements in case of transient state.
From X-ray diffraction measurements, in case of Si or B4C target used as a sputter target, the grain size was drastically decreased from 30 to 10 nm as the evaporation rate of the sputter source was increased.
This figure shows measurements in case of fluorescent light with increasing frequency over time.
This figure shows measurements in case when motion occurs, the fluorescent light has changing frequency, and other light sources are switched on and off, at the same time.
Fig. 3 Example of a typical autospectrum pointing to a 1 maximum RF based on 1000 measurements in case of a Straumann test implant.
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