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The height cross section of the SWCNT functionalized with PS/PC and cyt c (Fig. 4Ac) shows that the diameter of the structures is 3.5 nm which is significantly larger than bare SWCNT.
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b Height vs. time of UAV 12. c Time-height cross section of radar echo power (in dB, arbitrary scale) in range imaging mode, after doing the Capon processing, at vertical incidence from 16 30 LT to 18 00 LT on June 9 in the height range 1.27 6.5 km ASL.
Fig. 2 Typical height cross-sections of the ordered antidot arrays, before and after thin film deposition, as extracted from AFM images.
The range-height cross sections of the water vapor and aerosol within a 400 m range can be obtained for 25 min.
Figure 2 Latitude-height cross sections of the total number/occurrence frequency (1/1,000) of sporadic E layers (upper/lower row).
Figure 4 shows time-height cross sections of area-mean θ ′ w ′ ¯ and q ′ w ′ ¯ in cases A02 to A20.
Figure 4 Time-height cross sections of area-mean θ ′ w ′ ¯ (upper panels) and q ′ w ′ ¯ (lower panels).
Time-height cross sections of area-mean θ ′ w ′ ¯ for cases B1, B3, and B5 are shown in the upper panels of Figure 8.
Figure 9 shows time-height cross sections of area-mean u ′ w ′ ¯ for UZ values of 0 and 3 m · s 1 · km 1.
Figure 5 Time-height cross sections of area-mean u ′ w ′ ¯ in U Z = 0 and 3 (m · s -1 · km -1 ; upper and lower panels, respectively).
Figure 13 Time-height cross sections of area-mean θ ′ w ′ ¯ (left panels), q ′ w ′ ¯ (middle panels), and u ′ w ′ ¯ (right panels).
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