Sentence examples for mode with c from inspiring English sources

Therefore, the amplitude of longer vertical wavelength mode with c x  = 100 m/s grows up to higher altitudes (see above) and substantially exceeds the amplitude of the mode with c x  = 30 m/s near 100 km (compare Figures 6 and 7).

Figures 6b,c and 7b,c show that at t = 5 h, wave amplitudes mach to the exponential growth up to altitudes 50 to 60 km for AGW mode with c x  = 30 m/s and up to 70 to 80 km for c x  = 100 m/s.

Calculations show that F mz does not almost change up to altitudes 50 to 60 km for AGW mode with c x  = 30 m/s and up to 70 to 80 km for c x  = 100 m/s, then decreases due to wave dissipation.

This may explain why wave mode with c x  = 100 m/s produces larger dynamical effects and stronger wave-induced jet at high altitudes than the mode with smaller c x. Increased mean flows combined with superimposed wave structures (see Figure 7c) may produce narrow layers with large vertical wind shears.

In (b) the yellow box shows the dominant (smaller) bubble size mode while the magenta box shows the larger bubble size mode with (c) showing the respective bubble diameters in the distributions measured by Klug and Cashman (1994) on gray and white pumice from the 1980 Mount St. Helens eruption.

Open image in new window Fig. 4 Variation of ( B/D ) and ( phi_{m} ) with respect to cold ion concentration for slow mode with a ( H = 1 ) and b ( H = 3 ), and for fast mode with c ( H = 1 ) and d ( H = 3 ), where ( sigma_{c} = 0.05 ), ( sigma_{h} = 0.2 ).

All the compounds were analyzed using AutoDock 4.225 to confirm the binding mode with the C-C loop of EDA.

Fig. 1 a Schematic representation of surface charge measurement configuration and equivalent circuit of sample connected the electrometer with feedback amplifier in Coulomb mode, with the three capacitors C s, C IN, and A C f in parallel.

In Figure 5, these oscillations are larger for solid lines showing that partial reflections could be larger for wave modes with larger c x and longer λ z.

To explore the stability and binding mode of Irigenin with C-C loop of EDA, energy minimized Irigenin-EDA complex was subjected to molecular dynamics simulation for 100 ns run under GROMOS 43a1 force field.

Docking studies were performed to identify the binding mode of 3d with c-Met kinase domain in comparison to moderate and weak derivatives.