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In an ideal field design, the electrode spacing is smaller than the thickness of the features of interest, with the array length substantially greater than the well separation.
According to [15], GFDM is a FBM scheme that uses a non-orthogonal design where the sub-channel spacing is smaller than the sub-channel Nyquist band.
When the twin spacing is smaller than a critical value (such as d < 1.88 nm), there is no ample room between TBs, and dislocation dissociation is highly restricted.
When the dimensionless wellbore spacing is smaller than 0.4, then the region in between the wells will have less aperture variations which results in a lower (sigma _{Theta }).
The most important limitation is their resolution; too closely spaced harmonics cannot be distinguished if the spacing is smaller than the inverse of the observation period.
The SHE is enhanced by the resonant tunneling through the QD when the level spacing is smaller than the level broadening.
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The path spacing is small and the path is dense.
This indicates that the difference will be large when the fracture spacing is small.
This dependence can be divided into the linear part (when the finger spacing is large) and non-linear part (when the finger spacing is small).
The simulation results revealed that the outer fractures contribute more to gas production when fracture spacing is small due to the effect of fracture interference.
However, similar to[17], we assume that subcarrier spacing is small enough so that the bandwidth variables can be approximated as to be continuous in this article.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com