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The N2 adsorption isotherms for MWCNT/Mg-MOF-74 composites, measured at 298 K, are displayed in Fig. 6a.
The loss tangents of all the PEI/2 wt.% MWNT/BSTZ composites measured at 1 MHz were less than 0.05.
The dark and photocurrent characteristics (current vs. time) of the ZnO NWs and ZnO NW CdO composites measured at 0 V are given in Fig. 8.
The CO2 adsorption isotherms for MWCNT/Mg-MOF-74 and MWCNT/MIL-100 MWCNT/MIL-100 Femeasured at 273, 298, and 313 K, are exhibited in Figs. 4 and 5.
Open image in new window Fig. 12 CO2 uptake (cubic bars) and adsorption breakpoint (cylindrical bars) enhancements for a MWCNT/Mg-MOF-74 and b MWCNT/MIL-100(Fe) composites measured at 297 K. Figure 12b shows the improvement in both adsorption capacity and breakpoint due to adding MWCNT to the pristine MIL-100 Fe). MIL-100 Fe
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Figure 3 shows the absorbance values (Abs) and the absorption coefficients (α = (Abs × ln 10)/l, where l = 7.95 mm is the length of the composite) measured at a maximum radiation intensity of 1 μW/cm2.
High density polyethylene (HDPE) was used as a matrix polymer and steady-state shear viscosities of various compositions of HDPE/hollow sphere polymeric composites were measured at various temperatures.
The dielectric constant of sintered composites was measured at 1 MHz.
The direct current (DC) volume electrical conductivity of the composites was measured at room temperature using homemade resistivity setup with the help of Keithley 2400 sourcemeter and 2182 nanovoltmeter.
Figure 4a presents the discharge capacity of pristine H and composites HA and HN measured at current densities of 44, 110, 220, 660, and 1320 mA g−1 in a voltage range of 4.8 2.0 V.
The dielectric constants (εr) and loss tangents (tanδ) of the PEI/MWNT and PEI/MWNT/BSTZ composites were measured at 1 MHz using an LCR meter HP 4294 (Agilent Technologies Inc., Santa Clara, CA, USA). Figure 1 shows the FTIR spectra in the range of 500 to 4,000 cm-1 of the MWNTs and the acid-treated MWNTs.
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