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Large pressure differentials between the salt and rock layers make it difficult to keep the drill within the pressure window when passing from one to the other.
Narrow pressure window can be drilled safely.
The least mud pressure window is found in both azimuths 0° and 180° and the highest mud pressure window is found in both azimuths 90° and 270°.
At azimuth 0° and 180° the mud pressure window is similar and between 40.59 and 67.91 MPa.
The main object of stochastic analysis as applied in this study was geared towards defining the safe mud pressure window under a given set of conditions.
Figure 5b shows the safe mud pressure window predicted by Mogi Coulomb criterion that is a little wider than that predicted by Mohr Coulomb criterion.
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Original high pressure windows and sample cell have been developed to ensure both pressure resistance and transparency for the optical laser and Raman scattering beams.
Consequently, these membranes must be operated within narrow temperature and pressure windows, and must be free to expand upon absorption of hydrogen.
The drop shape could be monitored through two high-pressure windows fixed at both sides of the cell.
Diffusion coefficients of carbon dioxide and methane were measured by measuring the rate of gas absorption in a high-pressure windowed cell.
The nucleation and evolution of InN nanowires in a self-catalyzed growth process have been investigated to probe the microscopic growth mechanism of the self-catalysis and a model is proposed for high pressure growth window at ~760 Torr.
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