Polymeric
dispersants that adsorb onto various types of fine particles
have been designed through complex formation between cationic polyethyleneimine
(PEI) and anionic oleic acid (OA) to improve particle surface compatibility
with nonaqueous solvents. Complex formation involves the OA-assisted
dissolution of PEI in a nonaqueous solvent (toluene) by ultrasonication. While PEI itself is immiscible in
toluene, various molecular weights (MWs) of PEI (M
w = 600, 1800, and 10 000) visibly dissolved when,
in the presence of more than 5-mol % PEI (based on the ethyleneimine
(EI) unit of PEI), a complex formed between the carboxyl group of
OA and the amines of PEI in toluene. Si3N4 and
one of the typical multicomponent compositions for Si3N4 ceramic fabrication, Si3N4–Y2O3–MgO, were chosen to demonstrate the usage
of PEI–OA complexes for improving nonaqueous slurry
stability. While nontreated Si3N4 particles
rapidly formed dense slurry aggregates followed by solidification
in toluene, PEI associated with 30 mol % OA effectively adsorbed on
Si3N4 fine particles and drastically improved
the flow properties with ∼1.8 mg/m2 treatment. Surprisingly,
the flow properties were maintained even for dried and redispersed
slurries. The effect of the MW of PEI–OA and its additive
content on the stability of Si3N4/toluene slurries
has been clarified, and their applicability toward Si3N4–Y2O3–MgO multicomponent
systems is discussed.
To collect the signals of magnetic nanoparticles (MNPs) at a distance from a magnetic nanoparticle tomography, a strong ac magnetic field should be generated by applying a high current to the excitation coil. To this end, sinusoidal excitation using a linear amplifier-type ac power source has been applied to the tomography. Although this source can provide a high-quality sinusoidal voltage, its low power efficiency is not suitable for generating the required high current. To overcome this limitation, we use an H-bridge voltage source inverter to achieve high efficiency by generating a square-wave voltage. However, the third harmonic component in the square wave, undermines the acquisition of MNP signals. Thus, we suppress the third harmonic by shifting the switching phase of the inverter transistors. As a result, the third harmonic in the excitation current is reduced to less than one-tenth of that obtained after conventional suppression. We verify the distribution of MNP signals at depths up to 50 mm using the proposed excitation approach. The results demonstrate the effectiveness of the proposed approach based on square-wave inverter excitation for magnetic nanoparticle tomography.
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