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TOOLED THICK COMPOSITES by ARVEN H. SAUNDERS III ...

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Boundary Conditions<br />

HR<br />

HR<br />

HR<br />

V<br />

R<br />

CV<br />

V<br />

R<br />

CV<br />

V<br />

R<br />

CV<br />

Boundary Conditions<br />

HR<br />

HR<br />

HR<br />

V<br />

R<br />

CV<br />

V<br />

R<br />

CV<br />

V<br />

R<br />

CV<br />

Figure 3-9. Flow Resistance Network Representing the Laminate.<br />

where Visc(i, j) is the CV resin viscosity, permL(i, j) is CV longitudinal permeability, permT(i, j) is<br />

CV transverse permeability, dx is the typical distance x-wise between the CVs, Abs(Z(i, j) - Z(i, j<br />

+ 1)) is the vertical distance between the CVs, and FlowHgt(i,j) is the common CV height<br />

between CV(i,j) and CV(i+1,j). Note that the HR values incorporate longitudinal permeability and<br />

VR values incorporate transverse permeability. The cross-sectional area (flow channel) through<br />

which resin can flow between 2 adjacent CVs is the flow height * dy. Since resin viscosity may<br />

differ for the 2 CVs involved due to temperature effects, the average viscosity of the 2 CVs is<br />

used for the resin flow between them. The more restrictive minimum permeability between the 2<br />

adjacent CVs value is used.<br />

The resin flow for the contact areas is assumed to follow across, with flow moving to the<br />

left and right from the x-wise center/mid CV to each edge. The resistance to resin flow depends<br />

on the state of all the CVs the resin must pass through on its way out. This is analogous to 2<br />

42<br />

HR<br />

HR<br />

HR<br />

V<br />

R<br />

CV<br />

V<br />

R<br />

CV<br />

V<br />

R<br />

CV<br />

HR<br />

HR<br />

HR<br />

Boundary Boundary Conditions Conditions

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