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30 the temperature in a flow in the experimental model the primary focus should be to vary flow rate to understand its effect in graphene exfoliation. For this design to supply an inlet velocity of 6 m/s at the venturi tube a pump which can supply a flow of over 6 GPM must be used. This is because the inlet diameter of the venturi is 9 mm and therefore it must see a flow of 6 GPM to produce an inlet velocity of 6 m/s. In order to experimentally study the effect of flowrate on graphene exfoliation it is recommended a prime mover which could change the speed of the pump is being used or else to include a flow adjustment valve in the circuit proposed in Figure 10. 2.5 Conclusion In conclusion, an inexpensive method to exfoliate biocompatible graphene is presented. This paper would act as an effective introduction to the field of biocompatible graphene exfoliation using hydrodynamics. Based on the results, it could be concluded that processing time reduces the number of layers of graphene, yet the level of disorder seems to increase. As it was recorded the I2D/IG and ID/IG ratios to be .307 and .33 respectively at 6 hours. Based on the data of the effects of temperature on graphene exfoliation it could be identified with increase in temperature graphene exfoliation improves as the I2D/IG ratios improved accordingly. This is because with increase in temperature cavitation improves. This paper also provides adequate information to further study the effects of cavitation in graphene exfoliation. This design has proven that cavitation is the governing phenomenon in fluid based mechanochemical graphene exfoliation. This paper has provided an entrance to study graphene exfoliation based on other hydrodynamic principles.PDF Image | Hydrodynamic cavitation exfoliation layered graphene nano
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