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Fig. 9. Sketch demonstrating the dependence of H (top) and (bottom) on lǁ and showing the probable locations of the transparent and opaque regions.
A bleached photographic film is a developed photographic film where all the opaque regions are transformed into transparent by another chemical processing.
It has been suggested that the perception of transparency is triggered by X-junctions formed by junctions of contours of the transparent and opaque regions at the overlapping area [68].
While lens pathology observed in both infantile and mature DS lenses reveal opaque regions that are clinically described as supranuclear, the ages of the corresponding fiber cells comprising these regions are different (Fig 8).
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The area corresponds to the non-propagation (opaque) region for the fast (Alfven-type) branch.
The region where, is an opaque region, where the wave becomes evanescent, and the region where is transparent for waves.
The sample goes through immiscible (opaque) region to transparent region (seemingly miscible) and back to immiscible (opaque) again as temperature increases through 300 °C region.
The ratios of the opaque region to the whole area in 2009 and 2010 chalky grains were estimated to be 61.1 ± 10.2 and 78.4 ± 13.6%% (n = 50), respectively.
However, due to the tunneling effect part of the wave energy leak out the ionospheric sub-resonators and forms wave field with small, but finite amplitude even in the opaque region.
In a finite pressure plasma with an opaque region near the field-line top, it has a minimum at the equator and two maxima in both hemispheres, a total of three extremes (Fig. 10).
The structure of the wave potential Φ must be most deformed for the fundamental mode, in comparison to the cold plasma case, since the opaque region is largest and "deepest" for it.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com