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In general, with the increasing flow rate, the percentage removal and slope of breakthrough curves increased.
From this figure, it can be observed that the slope of breakthrough curves decreased by increasing the bed height.
The slope of breakthrough curve decreased with increasing bed height, which resulted in a broadened mass transfer zone.
Results showed that by increasing the bed height, the breakthrough and exhaustion times increased and the slope of breakthrough curves decreased.
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The slope of the breakthrough curve decreased with increasing bed height which resulted in a broadened mass transfer zone.
Again the variation in the slope of the breakthrough curve and adsorption capacity may be explained on the basis of mass transfer fundamentals.
With the manufacturer protocol for cleaning, the slopes of the measured breakthrough curves of the radial flow XT140 capsule were found to be better reproducible as compared to the XT5 capsule (see Fig. 8a).
The simulated breakthrough curve closely matches the breakthrough point and the initial slope of the measured data.
A simple quantitative relationship SBTC≈SP(Z)/2−1 is built based on a multi-rate mass transfer analysis, where SBTC is the slope of the power-law portion of tracer breakthrough curve, and SP(Z) denotes the slope of the power-law portion of the distribution of P(Z) which can be measured, e.g., in core logs.
This was a moment of breakthrough.
We saw a number of breakthrough performances.
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