Matrix or Vector | Shape Functions | Integration Points |
---|---|---|
Stiffness, Mass, and Damping Matrices | None (nodes may be coincident) | None |
The force-deflection relationship for the combination element under initial loading is as shown below (for no damping).
where:
F1 = force in spring 1 (output as F1) |
F2 = force in spring 2 (output as F2) |
K1 = stiffness of spring 1 (input as K1 on R command) |
K2 = stiffness of spring 2 (input as K2 on R command) |
ugap = initial gap size (input as GAP on R command) (if zero, gap capability removed) |
uI = displacement at node I |
uJ = displacement at node J |
FS = force required in spring 1 to cause sliding (input as FSLIDE on R command) |
The element mass matrix is:
(13–72) |
(13–73) |
(13–74) |
where:
M = element mass (input as M on R command) |
If the gap is open during the previous iteration, all other matrices and load vectors are null vectors. Otherwise, the element damping matrix is:
(13–75) |
where:
c = damping constant (input as C on R command) |
The element stiffness matrix is:
(13–76) |
where:
and the element Newton-Raphson load vector is:
(13–77) |
F1 and F2 are the current forces in the element.
If the gap is open,
(13–78)
If no sliding has taken place, F1 = F2 = 0.0. However, if sliding has taken place during unidirectional motion,
(13–79)
and thus
(13–80)
where:
us = amount of sliding (output as SLIDE) If the gap is closed and the slider is sliding,
(13–81)
and
(13–82)
where:
u2 = uJ - uI + ugap = output as STR2 If the gap is closed and the slider is not sliding, but had slid before,
(13–83)
where:
u1 = u2 - us = output as STR1 and
(13–84)
The above description refers to structural analysis only. When this element is used in a thermal analysis, the conductivity matrix is [Ke], the specific heat matrix is [Ce] and the Newton-Raphson load vector is , where F1 and F2 represent heat flow. The mass matrix [M] is not used. The gap size ugap is the temperature difference. Sliding, Fslide, is the element heat flow limit for conductor K1.