Nature of contact between polymer and mold in injection molding. Part I: Influence of a non-perfect thermal contact

2000 ◽  
Vol 40 (7) ◽  
pp. 1682-1691 ◽  
Author(s):  
D. Delaunay ◽  
P. Le Bot ◽  
R. Fulchiron ◽  
J. F. Luye ◽  
G. Regnier
1979 ◽  
Vol 101 (1) ◽  
pp. 20-27
Author(s):  
P. J. Closmann ◽  
E. R. Jones ◽  
E. A. Vogel

The effect of heat conduction on temperature along the wall of a well casing has been determined by solution of the equations of heat conduction. The casing was assumed to pass vertically through a planar heat source of constant temperature. The casing and formation were assumed to be in perfect thermal contact. Numerical results were obtained for two sizes of steel casing and one size of aluminum casing. At any given distance from the heat source, the casing temperature differs most at early times from the formation temperature computed in the absence of casing. This difference decreases rapidly with time. Furthermore, the maximum difference occurs at greater distances from the heat source as time increases. In general, after about three months of heating, errors in measured temperatures due to conduction along the casing wall are negligible.


2004 ◽  
Vol 24 (14-15) ◽  
pp. 2029-2040 ◽  
Author(s):  
A Bendada ◽  
A Derdouri ◽  
M Lamontagne ◽  
Y Simard

1981 ◽  
Vol 48 (4) ◽  
pp. 871-875 ◽  
Author(s):  
Maria Comninou ◽  
J. R. Barber ◽  
John Dundurs

An elastic half plane is indented by a perfectly conducting rigid flat punch, which is maintained at a different temperature from the half plane. It is found that, depending on the magnitude and direction of the total heat flux, one of the following states occurs: separation at the punch corners, perfect thermal contact throughout the punch face, or an imperfect contact region at the center with adjacent perfect contact regions.


1990 ◽  
Vol 30 (24) ◽  
pp. 1599-1606 ◽  
Author(s):  
Chi J. Yu ◽  
J. E. Sunderland ◽  
C. Poli

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