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Microscopically, increasing the flow rate, the film diffusion resistance decreases.
Hence, the degradation of two-phase heat transfer due to mass diffusion resistance is not captured.
Side reactions caused by diffusion resistance are minimized, and moreover, the involatile byproducts, if any, do not produce additional diffusion resistance.
Thus, direct calculation of gaseous phase diffusion resistance was possible.
The zeolite shell thickness was optimized to prevent poisoning and minimize diffusion resistance.
This was because of the highly dispersed Fe2O3 and low diffusion resistance of its open structure.
While the adsorption is controlled by mass diffusion resistance when (tth/tm)~O(1) or less.
The smaller charge transfer and electrolyte diffusion resistance are mainly demonstrated to be responsible.
Therefore, the Li ion diffusion resistance is increased and the Coulombic efficiency is reduced gradually.
This observation suggests that the diffusion resistance of CO2 through the solid Li2CO3 surface layer is the rate-limiting step.
High charge transfer and diffusion resistance were observed in 0D Co Al-LDHs, whiCo Al-LDHsre led to poor capacitance.
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