Bulk Data Entry
CONM2 – Concentrated Mass Element Connection, Rigid Body Form
Description
Defines a concentrated mass at a grid point of the structural model.
Format
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(2) |
(3) |
(4) |
(5) |
(6) |
(7) |
(8) |
(9) |
(10) |
CONM2 |
EID |
G |
CID |
M |
X1 |
X2 |
X3 |
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I11 |
I21 |
I22 |
I31 |
I32 |
I33 |
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Field |
Contents |
EID |
Unique element identification number. No default (Integer > 0) |
G |
Grid point identification number. No default (Integer > 0) |
CID |
Coordinate system identification number. Default = 0 (Integer > -1) |
M |
Mass value. No default (Real) |
X1, X2, X3 |
Offset distance from the grid point to the center of gravity of the mass in the coordinate system defined by CID, unless CID = -1, in which case X1, X2, and X3 are the coordinates (not offsets) of the center of gravity of the mass in the basic coordinate system. Default = 0.0 (Real) |
Iij |
Mass moments of inertia measured at the mass center of gravity. If CID is zero, then Iij is defined in the basic coordinate system. If CID > 1, then Iij refers to the local coordinate system. If CID is -1, then Iij refers to the basic coordinate system. Default = 0.0 (Real) |
1. | If the continuation is omitted, all rotary inertia is assigned zero values. |
2. | The form of the inertia matrix about its center of gravity is as follows: |
Where, M is the input mass value, Iij are the input inertia values, and X1, X2, and X3 are offsets.
3. | If CID = -1, the offsets are computed internally as the difference between the grid point location and X1, X2, and X3. The grid points may be defined in a local coordinate system, in which case the values of must be in a coordinate system that parallels the basic coordinate system. |
4. | If CID > 0, then X1, X2, and X3 are defined by a local Cartesian system, even if CID references a spherical or cylindrical coordinate system. |
5. | This card is represented as a mass element in HyperMesh. |
See Also: