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This loss in signal is due largely to the range limit of remote axial scanning using SSTF, which was predicted in previous theoretical work [ 13], as well as variation in coupling efficiency into the single-mode fiber, measured to have a root-mean-square variation of about 10% over this voltage range.
The fiber diameter, which is sometimes call fineness, is the thickness of the wool fiber measured in microns (one millionth of a meter).
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WC was measured using a nonstretchable fiber measuring tape.
The hips were measured using a standardized non-stretchable fiber measuring tape.
For the shortest fibers, eight images were analyzed with a total number of fibers measured equal to 26.
The term ( beta_{text{f}} ) = the angle of the FRP principal tensile fibers, measured with respect to the member longitudinal axis.
Table 1 Chemical compositions of the two fibers measured by EDS Type of fiber Content of element (atom%) C O Fe Eu Eu-shell/Fe-core 84.18 15.04 0.25 0.53 Fe-shell/Eu-core 93.91 5.88 0.2 0.02.
By contrast, these values are considerably higher than V0 of human skinned fibers measured at 12 15°C (slow-twitch fibers: 0.26 1.45 L0 s−1; fast-twitch fibers: 1.12 4.33 L0 s−1 [44] [46]), probably due to the high temperature sensitivity of V0 [44] [44].
Mean lengths (+/ - SEM) of 55 dorsal stress fibers measured from both samples are shown.
Mean length (+/ - SD) of 55 dorsal stress fibers measured from control and ML-7 treated cells.
Figure 1c sketches the waveguiding properties of our fibers measured by microphotoluminescence (μ-PL) experiments.
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