<!-- source-page: 191 -->

<table><tr><td>S33</td><td>Stress in the circumferential direction or in the local 3-direction.</td></tr><tr><td>S12</td><td>Shear stress.</td></tr><tr><td>S13</td><td>Shear stress.</td></tr><tr><td>S23</td><td>Shear stress.</td></tr></table>

# Heat flux components

Available for elements with temperature degrees of freedom.

HFL1 Heat flux in the radial direction or in the local 1-direction.

HFL2 Heat flux in the axial direction or in the local 2-direction.

# Pore fluid velocity components

Available for elements with pore pressure degrees of freedom, except for acoustic elements.

FLVEL1 Pore fluid effective velocity in the radial direction or in the local 1-direction.

FLVEL2 Pore fluid effective velocity in the axial direction or in the local 2-direction.

# Mass concentration flux components

Available for elements with normalized concentration degrees of freedom.

MFL1 Concentration flux in the radial direction or in the local 1-direction.

MFL2 Concentration flux in the axial direction or in the local 2-direction.

# Electrical potential gradient

Available for elements with electrical potential degrees of freedom.

EPG1 Electrical potential gradient in the 1-direction.

EPG2 Electrical potential gradient in the 2-direction.

# Electrical flux components

Available for piezoelectric elements.

EFLX1 Electrical flux in the 1-direction.

EFLX2 Electrical flux in the 2-direction.

# Electrical current density components

Available for coupled thermal-electrical elements.

ECD1 Electrical current density in the 1-direction.

ECD2 Electrical current density in the 2-direction.

<!-- source-page: 192 -->

![](images/page-192_b339ef825fba9b4cdaa9474c09d418e9dd1f6378d72a95698164de10274b4daa.jpg)

<details>
<summary>text_image</summary>

face 1
1
face 2
2
</details>

2 - node element

![](images/page-192_96237f752dc6dd57d86301bbcfb7d33df5e9e5e697d5051d7e04ba306a91be72.jpg)

<details>
<summary>text_image</summary>

3
face 3
face 2
1
face 1
2
</details>

3 - node element

![](images/page-192_abf12202cf2f694260fbf11004de3d335133fd6c034fee74dcaaaef1adb2413c.jpg)

<details>
<summary>text_image</summary>

face 3
face 4
face 2
face 1
face 4
1
2
3
</details>

4 - node element

![](images/page-192_3a498a632d3603ee51370cace0a0069cae0026e72ea413fd8b617fd4a3059732.jpg)

<details>
<summary>flowchart</summary>

```mermaid
graph TD
    1 --> 3
    1 --> 4
    1 --> 2
    2 --> 3
    2 --> 4
    3 --> 5
    4 --> 5
    5 --> 6
    6 --> 3
```
</details>

![](images/page-192_a6b7649dca67dcfb8bcd6e5b422c4cd80fc07cb4618836e13bfe554e52896f9a.jpg)

<details>
<summary>text_image</summary>

6 - node element
z
r
</details>

![](images/page-192_c36a2fa5eddf6d0e02ba3190ffd809ab7c4d1548e2abd0960401854d4be84e87.jpg)

<details>
<summary>flowchart</summary>

```mermaid
graph TD
    1 --> 2
    1 --> 3
    1 --> 4
    2 --> 3
    2 --> 4
    3 --> 4
    3 --> 5
    4 --> 5
    4 --> 6
    5 --> 6
    6 --> 7
    7 --> 8
    8 --> 1
```
</details>

8 - node element

# 2-node element faces

Face 1

Section at node 1

Face 2

Section at node 2

<!-- source-page: 193 -->

Triangular element faces 

<table><tr><td>Face 1</td><td>1 - 2 face</td></tr><tr><td>Face 2</td><td>2 - 3 face</td></tr><tr><td>Face 3</td><td>3 - 1 face</td></tr></table>

Quadrilateral element faces 

<table><tr><td>Face 1</td><td>1 – 2 face</td></tr><tr><td>Face 2</td><td>2 – 3 face</td></tr><tr><td>Face 3</td><td>3 – 4 face</td></tr><tr><td>Face 4</td><td>4 – 1 face</td></tr></table>

<!-- source-page: 194 -->

![](images/page-194_fb6b435299f6c5421dbfb77215641a3f5e84f1b2cc98c27d4e1a9d86bf609960.jpg)

<details>
<summary>natural_image</summary>

Simple diagonal line connecting two numbered points (1 and 2) on a plain background
</details>

2 - node element

![](images/page-194_4d2ca68510840d557842a67e2d9624049a709fe3096cd4d09426f9155f23bdf7.jpg)

<details>
<summary>text_image</summary>

3
×1
1
2
</details>

3 - node element

![](images/page-194_10dacaf4dcc17eea408d16bc8a3c80ee5f0b58f7aee8a4369079dab5bf0ac490.jpg)

<details>
<summary>text_image</summary>

4 ×3 4×
×1 2×
1 2 3
</details>

4 - node element

![](images/page-194_590cfaf0e642c52ed53e3df4be78aa47102d1affec189e5ee8ce9baa46c8d094.jpg)

<details>
<summary>text_image</summary>

4
3
×1
1
2
</details>

4 - node reduced integration element   
![](images/page-194_a5b0f2c31a6c7ec598d62f42e4f20b78ed594e3561b27676248f1e909e2f3574.jpg)

<details>
<summary>flowchart</summary>

```mermaid
graph TD
    1 --> 2
    1 --> 4
    1 --> 6
    2 --> 3
    2 --> 5
    3 --> 6
    4 --> 5
    5 --> 6
    6 --> 3
    3 --> 2
    2 --> 4
    4 --> 6
    5 --> 3
    6 --> 3
    3 --> 2
    2 --> 4
    4 --> 6
    5 --> 3
    6 --> 3
    3 --> 2
    2 --> 4
    4 --> 6
    5 --> 3
    6 --> 4
    3 --> 2
    4 --> 5
    5 --> 3
    6 --> 4
    3 --> 5
    4 --> 6
    5 --> 3
    6 --> 4
    3 --> 5
    4 --> 6
    5 --> 3
    6 --> 4
    3 --> 5
    4 --> 6
    5 --> 3
    6 --> 4
    3 --> 5
    4 --> 6
    5 --> 3
    6 --> 4
```
```
</details>

6 - node element   
![](images/page-194_f71f5b4cdcfe3effd3599dcc4b6f15907550554b72e96ea843b9b2a3d632cf15.jpg)

<details>
<summary>text_image</summary>

4
×7 ×8 ×9
8 ×4 ×5 ×6
×1 ×2 ×3
1 5 2
3
6
</details>

8 - node element

![](images/page-194_c93b74aa1374b7f09d0bf354850639aaf8eff8f8933ffdb846d93414d34186a7.jpg)

<details>
<summary>flowchart</summary>

```mermaid
graph TD
    1 -->|×1| 5
    1 -->|×3| 7
    2 -->|2×| 6
    2 -->|2×| 5
    3 -->|4×| 7
    3 -->|4×| 6
    4 -->|×3| 8
    5 -->|×1| 1
```
</details>

8 - node reduced integration element

For heat transfer applications a different integration scheme is used for triangular elements, as described in “Triangular, tetrahedral, and wedge elements,” Section 3.2.6 of the Abaqus Theory Guide.

<!-- source-page: 195 -->

# 28.1.7 AXISYMMETRIC SOLID ELEMENTS WITH NONLINEAR, ASYMMETRIC DEFORMATION

Product: Abaqus/Standard

# References

• “Choosing the element’s dimensionality,” Section 27.1.2   
• “Solid (continuum) elements,” Section 28.1.1   
• \*SOLID SECTION

# Overview

This section provides a reference to the axisymmetric solid elements available in Abaqus/Standard. These elements are intended for analysis of hollow bodies, such as pipes and pressure vessels. They can also be used to model solid bodies, but spurious stresses may occur at zero radius, particularly if transverse shear loads are applied.

# Conventions

Coordinate 1 is r, coordinate 2 is z. Referring to the figures shown in “Choosing the element’s dimensionality,” Section 27.1.2, the r-direction corresponds to the global X-direction in the $\theta \ : = \ : 0 ^ { \circ }$ plane and the negative global Z-direction in the $\theta = 9 0 ^ { \circ }$ plane, and the z-direction corresponds to the global Y-direction. Coordinate 1 must be greater than or equal to zero.

Degree of freedom 1 is $u _ { r } ,$ degree of freedom 2 is $u _ { z }$ . The $u _ { \theta }$ degree of freedom is an internal variable: you cannot control it.

# Element types

Stress/displacement elements 

<table><tr><td>CAXA4N</td><td>Bilinear, Fourier quadrilateral with 4 nodes per r-z plane</td></tr><tr><td>CAXA4HN</td><td>Bilinear, Fourier quadrilateral with 4 nodes per r-z plane, hybrid with constant Fourier pressure</td></tr><tr><td>CAXA4RN</td><td>Bilinear, Fourier quadrilateral with 4 nodes per r-z plane, reduced integration in r-z planes with hourglass control</td></tr><tr><td>CAXA4RHN</td><td>Bilinear, Fourier quadrilateral with 4 nodes per r-z plane, reduced integration in r-z planes, hybrid with constant Fourier pressure</td></tr><tr><td>CAXA8N</td><td>Biquadratic, Fourier quadrilateral with 8 nodes per r-z plane</td></tr><tr><td>CAXA8HN</td><td>Biquadratic, Fourier quadrilateral with 8 nodes per r-z plane, hybrid with linear Fourier pressure</td></tr></table>

<!-- source-page: 196 -->

CAXA8RN Biquadratic, Fourier quadrilateral with 8 nodes per r–z plane, reduced integration in r–z planes

CAXA8RHN Biquadratic, Fourier quadrilateral with 8 nodes per r–z plane, reduced integration in r–z planes, hybrid with linear Fourier pressure

Active degrees of freedom

1, 2

Additional solution variables

The bilinear elements have 4N and the biquadratic elements 8N additional variables relating to .

Element types CAXA4HN and CAXA4RHN have additional variables relating to the pressure stress.

Element types CAXA8HN and CAXA8RHN have additional variables relating to the pressure stress.

Pore pressure elements

CAXA8PN Biquadratic, Fourier quadrilateral with 8 nodes per r–z plane, bilinear Fourier pore pressure

CAXA8RPN Biquadratic, Fourier quadrilateral with 8 nodes per r–z plane, bilinear Fourier pore pressure, reduced integration in r–z planes

Active degrees of freedom

1, 2, 8 at corner nodes

1, 2 at midside nodes

Additional solution variables

8N additional variables relating to .

Nodal coordinates required

r, z

Element property definition

Input File Usage: \*SOLID SECTION

Element-based loading

Even though the symmetry in the r–z plane at allows the modeling of half of the initially axisymmetric structure, the loading must be specified as the total load on the full axisymmetric body. Consider, for example, a cylindrical shell loaded by a unit uniform axial force. To produce a unit load on a CAXA element with 4 modes, the nodal forces are 1/8, 1/4, 1/4, 1/4, and 1/8 at $\theta = 0 , \pi / 4 , \pi / 2$ , , and , respectively.

<!-- source-page: 197 -->

# Distributed loads

Distributed loads are specified as described in “Distributed loads,” Section 34.4.3.

<table><tr><td>Load ID (*DLOAD)</td><td>Units</td><td>Description</td></tr><tr><td>BX</td><td> $FL^{-3}$ </td><td>Body force per unit volume in the global X-direction.</td></tr><tr><td>BZ</td><td> $FL^{-3}$ </td><td>Body force per unit volume in the z-direction.</td></tr><tr><td>BXNU</td><td> $FL^{-3}$ </td><td>Nonuniform body force in the global X-direction with magnitude supplied via user subroutine DLOAD.</td></tr><tr><td>BZNU</td><td> $FL^{-3}$ </td><td>Nonuniform body force in the z-direction with magnitude supplied via user subroutine DLOAD.</td></tr><tr><td>Pn</td><td> $FL^{-2}$ </td><td>Pressure on face n.</td></tr><tr><td>PnNU</td><td> $FL^{-2}$ </td><td>Nonuniform pressure on face n with magnitude supplied via user subroutine DLOAD.</td></tr><tr><td>HPn</td><td> $FL^{-2}$ </td><td>Hydrostatic pressure on face n, linear in the global Y-direction.</td></tr></table>

# Foundations

Foundations are specified as described in “Element foundations,” Section 2.2.2.

<table><tr><td>Load ID(*FOUNDATION)</td><td>Units</td><td>Description</td></tr><tr><td>Fn</td><td> $FL^{-3}$ </td><td>Elastic foundation on face n.</td></tr></table>

# Distributed flows

Distributed flows are available for elements with pore pressure degrees of freedom. They are specified as described in “Coupled pore fluid diffusion and stress analysis,” Section 6.8.1.

<!-- source-page: 198 -->

<table><tr><td>Load ID(*FLOW/*DFLOW)</td><td>Units</td><td>Description</td></tr><tr><td>Qn</td><td> $F^{-1}L^{3}T^{-1}$ </td><td>Seepage (outward normal flow) proportional to the difference between surface pore pressure and a reference sink pore pressure on face n (units of  $FL^{-2}$ ).</td></tr><tr><td>QnD</td><td> $F^{-1}L^{3}T^{-1}$ </td><td>Drainage-only seepage (outward normal flow) proportional to the surface pore pressure on face n only when that pressure is positive.</td></tr><tr><td>QnNU</td><td> $F^{-1}L^{3}T^{-1}$ </td><td>Nonuniform seepage (outward normal flow) proportional to the difference between surface pore pressure and a reference sink pore pressure on face n (units of  $FL^{-2}$ ) with magnitude supplied via user subroutine FLOW.</td></tr><tr><td>Sn</td><td> $LT^{-1}$ </td><td>Prescribed pore fluid velocity (outward from the face) on face n.</td></tr><tr><td>SnNU</td><td> $LT^{-1}$ </td><td>Nonuniform prescribed pore fluid velocity (outward from the face) on face n with magnitude supplied via user subroutine DFLOW.</td></tr></table>

# Element output

The numerical integration with respect to employs the trapezoidal rule. There are $2 ( N + 1 )$ equally spaced integration planes in the element, including the $\theta = 0 ^ { \circ }$ and $\theta = 1 8 0 ^ { \circ }$ planes, with N being the number of Fourier modes. Consequently, the radial nodal forces corresponding to pressure loads applied in the circumferential direction are distributed in this direction in the ratio of in the 1 Fourier mode element, in the 2 Fourier mode element, and in the 4 Fourier mode element. The sum of these consistent nodal forces is equal to the integral of the applied pressure over .

Output is as defined below unless a local coordinate system in the r–z plane is assigned to the element through the section definition (“Orientations,” Section 2.2.5) in which case the components are in the local directions. These local directions rotate with the motion in large-displacement analysis. See “State storage,” Section 1.5.4 of the Abaqus Theory Guide, for details.

<!-- source-page: 199 -->

# Stress, strain, and other tensor components

Stress and other tensors (including strain tensors) are available for elements with displacement degrees of freedom. All tensors have the same components. For example, the stress components are as follows:

<table><tr><td>S11</td><td>Stress in the radial direction or in the local 1-direction.</td></tr><tr><td>S22</td><td>Stress in the axial direction or in the local 2-direction.</td></tr><tr><td>S33</td><td>Hoop direct stress.</td></tr><tr><td>S12</td><td>Shear stress.</td></tr><tr><td>S13</td><td>Shear stress.</td></tr><tr><td>S23</td><td>Shear stress.</td></tr></table>

# Node ordering and face numbering on elements

The node ordering in the first r–z plane of each element, at , is shown below. Each element must have N more planes of nodes defined, where N is the number of Fourier modes. The node ordering is the same in each plane. You can specify the nodes in each plane. Alternatively, you can specify the node ordering in the first r–z plane of an element, and Abaqus/Standard will generate all other nodes for the element by adding successively a constant offset to each node for each of the N planes of the element. By default, Abaqus/Standard uses an offset of 100000 (see “Element definition,” Section 2.2.1).

![](images/page-199_a3893ccbd4df34e57d9395696a3afc96f5b7fb70067c7ad0faf9bd9e83299082.jpg)

<details>
<summary>text_image</summary>

face 3
face 4
face 2
face 1
face 4
1
2
z
r
</details>

4 - node element

![](images/page-199_a8e676cd91bab1f34de2a9bbc72a3470b091eead5a47d1d6b057950808979be9.jpg)

<details>
<summary>flowchart</summary>

```mermaid
graph TD
    1 --> 2
    1 --> 5
    1 --> 8
    2 --> 3
    2 --> 6
    3 --> 4
    4 --> 7
    5 --> 8
    6 --> 3
    7 --> 4
    8 --> 1
```
</details>

8 - node element

Element faces 

<table><tr><td>Face 1</td><td>1 - 2 face</td></tr><tr><td>Face 2</td><td>2 - 3 face</td></tr><tr><td>Face 3</td><td>3 - 4 face</td></tr><tr><td>Face 4</td><td>4 - 1 face</td></tr></table>

<!-- source-page: 200 -->

# Numbering of integration points for output

The integration points in the first r–z plane of integration, at $\theta = 0 _ { ; }$ , are shown below. The integration points follow in sequence at the r–z integration planes in ascending order of location.

![](images/page-200_16c3b9d9784e8ec86abbefb0c083ef68ac8464d4c59b8464caf1ac51a34bd077.jpg)

<details>
<summary>text_image</summary>

4
×3
4×
×1
2×
1
2
3
</details>

4 - node element

![](images/page-200_551503d51eac22c8bd640634fbd26ee58812ed25303fd57984c52fd76466cedc.jpg)

<details>
<summary>text_image</summary>

4
3
×1
1
2
</details>

4 - node reduced integration element

![](images/page-200_4252e795d40cf375e521a42f9db3720cf1436a943fe7866374b1e1366137621d.jpg)

<details>
<summary>text_image</summary>

4
×7 ×8 ×9
8 ×4 ×5 ×6
×1 ×2 ×3
1 5 2
3
6
</details>

8 - node element

![](images/page-200_2c886bbf3a483052ea90fb167bb051fa83ccb01a41fd2c2f59b325e7bedfce6a.jpg)

<details>
<summary>text_image</summary>

4
×3
7
3
4×
8
×1
1
5
2×
6
2
</details>

8 - node reduced integration element
