Sentence examples similar to sections of area from inspiring English sources

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).

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 13 Time-height cross sections of area-mean θ ′ w ′ ¯ (left panels), q ′ w ′ ¯ (middle panels), and u ′ w ′ ¯ (right panels).

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).

Time-height cross sections of area-mean θ ′ w ′ ¯ for cases B1, B3, and B5 are shown in the upper panels of Figure 8.

The eddy momentum flux is sensitive to the initial vertical shear of zonal flow UZ. Figure 5 shows time-height cross sections of area-mean u ′ w ′ ¯ for UZ values 0 and 3 m · s-1 · km-1.

Such strong wind shear forms via convective adjustment (Figure 5) and turbulent mixing (Figure 9). Figure 9 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).

The domain area is 16 times larger than in sections 'Convective adjustment in unstable layer (case A)' and 'Microscale eddies induced by turbulent thermal flux (case B)'. Figure 13 shows time-height cross sections of area-mean θ ′ w ′ ¯, q ′ w ′ ¯, and u ′ w ′ ¯ for large-domain experiments of cases A10 and B3 under the condition U Z  = 0 m · s 1 · km 1.

Thin sections of areas containing midgut were stained with uranyl acetate and lead citrate, and examined in a Hitachi H7650.

This paper studies the vibration characteristics of a rotating tapered cantilever Bernoulli Euler beam with linearly varying rectangular cross-section of area proportional to xn, where n equals to 1 or 2 covers the most practical cases.