node

Nodes are basic components in FE models. The node command is used to construct nodes.

Syntax

node (1) [2...]
# (1) int, unique tag
# [2...] double, coordinates

Usage

A unique tag is required to identify different nodes. The tag shall be an unsigned integer, negative values are not allowed. Although zero is a valid tag, it is suggested to label nodes starting with one. It is not recommended to use arbitrarily large tag for any nodes, although the maximum tag is about four billion (unsigned int). Any unnecessarily large node tag may lead to memory leakage as some functions create matrix depending on the largest node tag to ensure all nodes could be stored.

There is no limitation on the dimension of the node defined. A trivial node (without a location) can be defined as follows. Such a node will not be used to define elements in general cases.

node 1

Nodes with different dimensions can coexist.

node 1
node 2 2. 0.
node 3 0.
node 4 9. 8. 7. 1.

In fact, during initialisation, the dimension of each node will be double-checked to ensure the connected elements could work properly. Meanwhile, excessive dimensions would be ignored (but not discarded) during analysis. If for example one is performing a 2D analysis and the model contains the following snippet.

node 1 3.
node 2 2. 1.
# later define a 2D element connecting node 1 and node 2

The dimension of node 1 will be automatically expanded to two with zero filling, so node 1 represents node (3.0,0.0)(3.0,0.0) in the 2D space. If, on the other hand, an 1D analysis is performed, then the second coordinate will be ignored.

It is still recommended defining nodes with proper coordinates. Generating a node list from ABAQUS input file is an easy task.

Output Types

The following quantities can be recorded using the commands similar to plainrecorder 1 Node (output_type) (nodes...).

variable label
physical meaning

U

all displacement components

U1, U2, U3, UR1, UR2, UR3

displacement along each DoF

V

all velocity components

V1, V2, V3, VR1, VR2, VR3

velocity along each DoF

A

all acceleration components

A1, A2, A3, AR1, AR2, AR3

acceleration along each DoF

RF

all resistance components

RF1, RF2, RF3, RM1, RM2, RM3

resistance along each DoF

DF

all damping force components

DF1, DF2, DF3, DM1, DM2, DM3

damping force along each DoF

IF

all inertial force components

IF1, IF2, IF3, IM1, IM2, IM3

inertial force along each DoF

Remarks

  1. For static analysis, normally only displacement U and resistance RF are activated. Thus, recording other quantities returns trivial results.

  2. If the required quantity is not active, the output will be empty.

  3. The damping and inertial forces are collected from all the elements in the model. It must be noted that the recorded values do not include any contributions that do not stem from elements. For example, the damping force given by global damping models cannot be split to individual elements; thus it is not reflected in the nodal damping force. This design is necessary as one may wish to separate contributions from various sources apart.

  4. To record global damping and inertial forces that account for the total force, use GDF, GDF1, GDF2, GDF3, GDF4, GDF5, GDF6, GIF, GIF1, GIF2, GIF3, GIF4, GIF5, GIF6, which stand for global damping force and global inertial force.

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