2007
DOI: 10.1016/j.ijpharm.2006.11.005
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Triboelectrification of pharmaceutical powders by particle impact

Abstract: Pharmaceutical powders are very prone to electrostatic charging by colliding and sliding contacts with walls and other particles. In pharmaceutical formulation processes, particle charging is often a nuisance and can cause problems in the manufacture of products, such as affecting powder flow, and reducing fill and dose uniformity. For a fundamental understanding of the powder triboelectrification, it is essential to study charge transfer due to a single contact of a particle with a target plane under well-def… Show more

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Cited by 104 publications
(63 citation statements)
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“…These phenomena agree with the experimental observation and theoretical analysis by Matsuyama et al (2003), in which the non-uniform charge distribution on the surfaces of particles can influence the charge accumulation process and lead to different charging coefficients. The values of transferred charges on particles in the current study are in the range of 10 -13 to 10 -11 C, which is comparable to the typical charge on pharmaceutical particles induced by impact charging (Watanabe et al, 2007). Under realistic conditions, the charge should be distributed on the surface of a particle and may be under relaxation and dissipation, especially for conductors.…”
Section: Discussionsupporting
confidence: 58%
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“…These phenomena agree with the experimental observation and theoretical analysis by Matsuyama et al (2003), in which the non-uniform charge distribution on the surfaces of particles can influence the charge accumulation process and lead to different charging coefficients. The values of transferred charges on particles in the current study are in the range of 10 -13 to 10 -11 C, which is comparable to the typical charge on pharmaceutical particles induced by impact charging (Watanabe et al, 2007). Under realistic conditions, the charge should be distributed on the surface of a particle and may be under relaxation and dissipation, especially for conductors.…”
Section: Discussionsupporting
confidence: 58%
“…where S is the maximum contact area during the collision, k is the charging constant (Matsusaka et al, 2000;Watanabe et al, 2007) and is of the order of 10 -4 C·m -2 ·V -1 . After each collision, the charge on materials i and j will hence become q i -Δq and q j +Δq, respectively.…”
Section: Is the Contact Potential Difference (Cpd) Between The Surfaces;mentioning
confidence: 99%
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“…where S m is the maximum contact area during the collision, k s is the charging constant during contact electrification and is of the order of 10 -4 C·m -2 ·V -1 [32][33][34]. During a collision, the charge will be transferred from material i to material j.…”
Section: The Contact Electrification Modelmentioning
confidence: 99%