The sources contributing to the absolute uncertainty of the average dosimetry were a) antenna modeling; 0.1 dB (experimentally verified); b) deviation of incident field exposure with respect to the target field including transfer calibration, sensor linearity, feedback control, and reflections from furniture, 0.7 dB; and c) average anatomy, dielectric parameters, and discretizations.
We then generated random Kh values of normal distribution based on the mean and standard deviation of the field measurements in the five layers, as well as using modified means and standard deviations.
The average mean deviation of all field plots was -16.02 dB (p < 0.005) ; range -8.58 to -24.73 dB.
All but one oxidative potential measurement were above the LOD (> 725/m), calculated as three times the standard deviation of the field blank readings.
The results from a representative experiment are shown and expressed as the mean number of migrated cells/field ± standard deviation of six fields of view/condition.
The data are presented as means ± standard deviation of 4 fields from each well of triplicate samples.
The average field strength and standard deviation of the incident field at each cow location is based upon ~80 measurements.
Deviations of the field from the vertical did not exceed 2°.
Besides, the present results indicate that the sound pulse decay inside a not very reverberant classroom consists of an initial fast decay, leading to deviations of the field survey results from those predicted by the exponential decay under the uniform sound energy decay assumption.
The approximately linear lag time scaling of the mean square phase fluctuations 〈Δ φ τ, t′)〉 measured at different phases of the pulsation cycle clearly shows that the deviations of the field autocorrelation function from the expected ballistic behavior observed in vivo [ 4, 13, 14] does not arise from time-averaging of g(1)(τ, t) over integration times longer than the pulse cycle time 1/ f0.
