While the shield wire is still in the same position (not drawn in Fig. 1b), the line is divided into three equal sections and phase conductors are alternated with each other.
We can make this idea more intuitive by looking at random graphs, section "Random graphs and phase transitions".
These correspond to the random graph with few edges and the highly connected graph in section "Random graphs and phase transitions".
As shown in the previous section, the amplitude and phase of the optical noise signal generally depend on —as well as on system parameters such as and, the length of the water column between target and receiver measured along the laser beam propagation direction.
The exact solutions of the nozzle wave equation (Section 3), for the four families of ducts, are plotted (Section 4) as amplitude and phase versus distance, for several combinations of frequency and low Mach number.
The image of the illumination function depicts a cross section of the amplitude and phase within the focal plane of the beam and, thus, determines the final spot profile at the sample surface.
As demonstrated in the previous section, both the magnitude and phase of the complex image function U x,y) = |U x,y) |exp[ iΦ x,y)] can be uniquely determined using SLIM (using Eqs. (3) and (5)).
The performance of three materials was evaluated by means of several analysis methods including: kinetic analysis (corrosion rate), SEM (microcosmic morphology of surface and cross-section),EDS (distribution of elements of cross-section) and XRD (phases formed on the surface layer).
Fig. 6 Observed and calculated pseudo-sections of apparent resistivity and phase for TM and TE modes.
Fig. 5 The observed and computed pseudo-sections for apparent resistivity and phase data in TE and TM modes.
