Sentence examples for layered case and from inspiring English sources

Comparing the layering and slab effects in slip inversions, the relative importance of the layering displacements is, naturally, larger for the purely layered case, and the relative importance of the interface displacements is larger in the slab case (Fig. 4).

However, the maximum slip only changes slightly: It increases from 38.5 m in the homogeneous to 39.6 m in the layered case and decreases to 37.3 m when slabs are introduced.

When the heterogeneous models are employed in inversions, the maximum slip increases from 38.5 m in the homogeneous to 39.6 m in the layered case and decreases to 37.3 m when slabs are introduced, and potency changes accordingly.

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.

To confirm the presence of microscale eddies in the large model domain, domain size (5 × 5 km) in sections 'Convective adjustment in unstable layer (case A)' and 'Microscale eddies induced by turbulent thermal flux (case B)' is extended by a factor of four (to 20 × 20 km) in the large-domain experiment (section 'Sensitivity of microscale eddies to model domain size').

For Hall, an average of 1465.9 packets are dropped in the source in the application layer adaptation case, and 1140.5 packets in the combined application plus MAC layer adaptation case.

The 0.035 M (pH ≈ 4.5) solutions of T and C applied 3 times revealed the best potential to act as single treatments while more aggressive treatments showed to have negative outcomes: formation of a superficial dense layer (T case) and excessive dissolution of calcite gains (C case).

As a result the associated states essentially follow the dispersion of the valence band in the one-layer case, see Fig. 4(b) and (c).

For the simulated two-layer case, the dimensions of the bottom and top layers were 10 × 10 × 8 cm and 10 × 10 × 1 cm, respectively, with the same node distance as for the homogeneous case.

The continuous layer case is studied using several different beam theories.

From a two-layer reference solution, an explicit solution for the multi-layer case is derived.