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It is found that the average mixing efficiency of nutrient source and bacteria liquid reaches 98%, and the maximum power density reaches 118.34 mW/m3, 28.9% higher than that of MFC without mixer.
As s increases, the mixing layer thickness increases, and the mixing efficiency of an entrained fluid decreases.
For the perfectly mixed fluids, M is 1, and for the unmixed fluids, M is 0. A mixing efficiency of 0.9 or above indicates excellent mixing, and a mixing efficiency between 0.8 and 0.9 indicates acceptable mixing.
Applying magnetic field considerably improves the mixing efficiency of the micromixer and reduces the mixing length.
It was numerically revealed that the viscosities and the densities, as well as the initial temperatures and the rheology of mixing fluids have significant effects on the flow regimes and the mixing efficiency of two fluids.
The mixing efficiency of this micromixer is relatively low as the mixing of two fluids is executed by the laminar diffusion process.
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Villermaux Dushman reaction experiments were also conducted for additional verification of CFD results and for mixing efficiency evaluation of the different geometries.
Continuous heat balance calorimetry allows determination of mixing efficiency by measurement of effective excess enthalpy of non-reactive streams.
This visual technique allowed the quantification of mixing efficiency, as well as identification of issues such as flow recycling, stagnant zones, and other inconsistencies in the mixing dynamics.
It is observed that the fluid is trapped within the vortex core at higher Reynolds number, leading to a reduction in mixing efficiency and appearance of a maxima.
Then, the computed 3D laminar flow patterns and several mixing performance criteria (power consumption, pumping capability, intensity of segregation, mixing time, mixing efficiency and specific energy) of the impellers are investigated.
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