The thermal parameters such as glass transition [Tg] and crystallization [Tc] temperatures of the prepared glass were obtained from the DTA trace as shown in Figure 3.
Following Thatcher and England (1998), we considered the problem in a 2-D plane perpendicular to the fault trace, as shown in Fig. 1.
In order to increase the convenience and reality of the simulation, the simulation is separated into two modes: local simulation and recorded trace as shown in Figure 5.
The profile line was constructed perpendicular to the Yammouneh Fault trace line, such that the boreholes were distributed in equal number on both sides of the fault trace, as shown in Fig. 3.
We then used our two-step scratching method (as shown in Figure 1c,d) to fabricate 3D nanodot arrays on PC surfaces.Firstly, to fabricate nanodots with a size of 500 nm, we chose two-step scratching traces (as shown in Figure 1c) using scratching angles of 90° and 0° for ripple formation with a period of 500 nm.
Therefore, in this study we introduce another parameter which is the rate of variation of the SC which is the maximum rate of change of the geomagnetic field during the higher-frequency region of the SC, and without having discontinuities in the trace as shown in Fig. 3.
The SS electrode exhibited relatively planar surfaces with parallel polishing traces, as shown in Figure 2(a).
This pulse duration is confirmed by comparing experimental (black) and calculated (red) interferometric autocorrelation traces, as shown in Fig. 2(d).
This 2D-conductance map has been obtained by collecting the conductance histogram in color code of 250 consecutive breaking traces as those shown in Figure 2a.
First, the interfacial length between oil and CO2 was evaluated by tracing the interface as shown in the figure.
