“…This involved the addition of a local gas resistance layer at the heat transfer surface, thereby allowing for greater voidage at this point. Baskakov (4) assumed that the thickness of this thermal resistance layer was approximately equal to the particle radius. He further assumed that the resistance of this layer was approximately equal to the temperature difference between the wall and adjacent particles, divided by the value of the specific heat flux between them.…”
Section: Another Modification Of the Packet Model Presented By Micklementioning
“…This involved the addition of a local gas resistance layer at the heat transfer surface, thereby allowing for greater voidage at this point. Baskakov (4) assumed that the thickness of this thermal resistance layer was approximately equal to the particle radius. He further assumed that the resistance of this layer was approximately equal to the temperature difference between the wall and adjacent particles, divided by the value of the specific heat flux between them.…”
Section: Another Modification Of the Packet Model Presented By Micklementioning
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