Center of element method

The following table lists element types supported by the center of element conduction method and how the thermal solver identifies their center of location and sub-elements to create conductances between elements.

Element Type Element Center Location Sub-elements
Lump mass Node N/A
Beam Center of gravity (CG) N/A
Triangular shell Point where the three perpendicular bisectors of the edges meet

N/A
Quadrilateral shell—regular shape, such as a rectangle Point where the perpendicular bisectors of the edges meet Single sub-element
Quadrilateral shell—irregular shape Center of the sub-element closest to the CG (blue point)

Two triangular sub-elements created by connecting the diagonal corners that form the largest angle sum
Tetrahedron solid Point where the perpendiculars that derive from the center of side triangular surfaces meet N/A
Wedge and hexahedron solid—regular surface shapes, such as triangles, rectangles, or isosceles trapezoids Unique center

Single sub-element
Wedge and hexahedron solid—irregular surface shapes Center of the sub-element closest to the CG, by default

When the software uses custom settings, the thermal solver can also compute a unique element center near solid element's CG.

Tetrahedral sub-elements

Thick shell elements

The thermal solver identifies the thickness direction for solid elements and computes the smallest average edge length in the thickness direction, as the approximate thickness. For example, in wedge elements, the thickness direction is considered from one triangular face to the other. The aspect ratio of a solid element is defined as the ratio of the longest edge to the approximate thickness. When the aspect ratio of a solid element is greater than 5, the thick shell approximation is used.

In-plane conductances are calculated as if the solid element were planar with a thickness equal to the mean thickness of the solid element.

The through-thickness conductance is calculated as if the solid element were solid with a unique element center.