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SMT-Feb2015

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34 SMT Magazine • February 2015 dipoles with energy –pE in the driving them in the region of stronger field E. It is important that the energy gain due to formation of a polarized metal needle does not depend on the field sign as illustrated in Figure 3. The dipole vector p is parallel to the field vector E, so the product –pE is negative. Another wording would be to say that like charges repel producing an outward stress. It is relieved by expelling some of these charges outward via creating a metal whisker with the expelled charge sitting at its far end. These nucleation events take place most easily where the metal surface is locally weak. eLeCTrOSTaTIC MeCHaNISM OF NuCLeaTION aNd GrOWTH OF MeTaL WHISKerS continues Feature It is worth mentioning that the existence of strongly anisotropic stretched (needle-shaped) metallic particles is due to their strong polariza- tion gain in the external electric field. In turn, that gain is a consequence of their large dipole moments due to considerable dipole length. As a result, long enough particles become ener- getically favorable in the external field in spite of the fact that their surfaces are much great- er than that of an equivalent volume sphere. The needle-shaped metallic particles dominate when the field is greater than a certain critical value as illustrated in Figure 4. This consider- ation provides a physical mechanism of the very existence of extremely high aspect ratio metal whiskers not collapsing into spherical shapes of equivalent volumes. Their energetically favor- able shapes are dictated by the existing electric fields. According to this understanding, whis- kers would inevitably collapse into spherical- like shapes in the absence of external electric fields. 4. Following the nucleation is the growth stage where whiskers increase their length by accretion of material at their bases. The growth kinetics are different for whisker lengths below and above the characteristic charge patch di- mension L. In particular, growth rates turn out to be extremely low for short (h<

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