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The gas production rate decreases until the start of reinjection.
After the period, the relative σ decreases until predawn.
It is shown that scatter decreases until reaching a steady state value for long crack growth.
Results have shown that thermal conductivity decrease when density decreases until an optimum.
As a result, gas rate rapidly decreases until the well stops production.
Increasing β from c∗, ρ M still decreases until reaching a turning point 2β=2c∗≃0.
Moreover, peak 2 continuously decreases until it disappears while its resonant wavelength decreases throughout.
With the increasing scale parameter, spectral homogeneity of segments decreases until they match the objects in the real world.
For the constant total flow rate, that maximum decreases until a minimum, and then increases with production time.
Subsequently this discharge variability decreases until reaching its minimum in October at the end of the dry season.
Further, the value of η e increases as f ″ ( 0 ) decreases, until the limit point is approached, η e = ∞.
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