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contributor authorJ. A. Owczarek
date accessioned2017-05-08T23:40:59Z
date available2017-05-08T23:40:59Z
date copyrightSeptember, 1993
date issued1993
identifier issn1528-9044
identifier otherJEPAE4-26139#240_1.pdf
identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/111752
description abstractIn this part of the paper the drop test method is used to show that RTV dispersions are in fact plastic “false body” materials, and to determine the magnitudes of the residual yield stresses after shearing for different RTV dispersion lots. With the aid of the equation for the wall shear stress derived in Part I of this paper [1], a correlation equation between the residual yield stress and the deposition variables is obtained, and analysis is made of the drop spreading phenomenon. It is shown that the drop spread, which is responsible for the run-over, or wicking, of external leads of electronic circuits, can be decreased by decreasing the deposition rate of the encapsulant. Finally, a method is developed to determine the required deposition flow rate and deposition time to produce a drop having required final diameter and cured skin thickness.
publisherThe American Society of Mechanical Engineers (ASME)
titleCoating of Electronic Components by the RTV Dispersion—Part II: Determination of the Residual Yield Stress After Deposition, and Method to Produce a Drop of Required Cured Skin Thickness and Diameter
typeJournal Paper
journal volume115
journal issue3
journal titleJournal of Electronic Packaging
identifier doi10.1115/1.2909324
journal fristpage240
journal lastpage248
identifier eissn1043-7398
keywordsCoating processes
keywordsCoatings
keywordsDrops
keywordsElectronic components
keywordsSkin
keywordsThickness
keywordsYield stress
keywordsEquations
keywordsShearing
keywordsCircuits
keywordsShear (Mechanics)
keywordsStress AND Flow (Dynamics)
treeJournal of Electronic Packaging:;1993:;volume( 115 ):;issue: 003
contenttypeFulltext


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