Determination of the size distribution of non-spherical nanoparticles by electric birefringence-based methods

被引:49
|
作者
Arenas-Guerrero, Paloma [1 ]
Delgado, Angel V. [1 ]
Donovan, Kevin J. [2 ]
Scott, Kenneth [2 ]
Bellini, Tommaso [3 ]
Mantegazza, Francesco [4 ]
Jimenez, Maria L. [1 ]
机构
[1] Univ Granada, Dept Appl Phys, E-18071 Granada, Spain
[2] Queen Mary Univ London, Sch Phys & Astron, London E1 4NS, England
[3] Univ Milan, Dept Med Biotechnol & Translat Med, I-20090 Milan, Italy
[4] Univ Milano Bicocca, Dept Med & Chirurg, I-20854 Vedano Al Lambro, MB, Italy
来源
SCIENTIFIC REPORTS | 2018年 / 8卷
关键词
DYNAMIC LIGHT-SCATTERING; STRETCHED-EXPONENTIAL RELAXATION; CARBON NANOTUBES; GOLD NANORODS; SUSPENSIONS; DISPERSION; PARTICLES; SINGLE; PHASE;
D O I
10.1038/s41598-018-27840-0
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
The in situ determination of the size distribution of dispersed non-spherical nanoparticles is an essential characterization tool for the investigation and use of colloidal suspensions. In this work, we test a size characterization method based on the measurement of the transient behaviour of the birefringence induced in the dispersions by pulsed electric fields. The specific shape of such relaxations depends on the distribution of the rotational diffusion coefficient of the suspended particles. We analyse the measured transient birefringence with three approaches: the stretched-exponential, Watson-Jennings, and multiexponential methods. These are applied to six different types of rod-like and planar particles: PTFE rods, goethite needles, single- and double-walled carbon nanotubes, sodium montmorillonite particles and gibbsite platelets. The results are compared to electron microscopy and dynamic light scattering measurements. The methods here considered provide good or excellent results in all cases, proving that the analysis of the transient birefringence is a powerful tool to obtain complete size distributions of non-spherical particles in suspension.
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页数:10
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