Difference between revisions of "Nodal Stresses"

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= Nodal Stresses =
 
When you issue the command <code>STREss,NODE,n1,n2,n3</code> at the Macro prompt, FEAP will compute a nodal projection of the Gauss point values and print them for nodes n1 to n2 in increments of n3 (default 1).   
When you issue the command <code>STREss,NODE,n1,n2,n3</code> at the Macro prompt, FEAP will compute a nodal projection of the Gauss point values and print them for nodes n1 to n2 in increments of n3 (default 1).   


== Mechanical Elements ==
= Mechanical Elements =


=== First set of values ===
== First set of values ==
The values printed consist for mechanical elements of the three principal stresses <math>\sigma_I, \sigma_{II}, \sigma_{III}</math>, then the max shear <math>(\sigma_I - \sigma_{III})/2</math>, then the pressure <math>p = \frac{1}{3}\mathrm{tr}[\sigma]</math>, then "J2" printed as <math> \sqrt{\frac{3}{2}} \Vert \mathbf{s} \Vert </math> (the equivalent tensile stress, also known as the equivalent Mises stress, note <math> \mathbf{s} </math> is the deviatoric stress tensor), and finally "J3" printed as <math> \sqrt[3]{ \frac{1}{3}[ (\sigma_I-p)^3 + (\sigma_{II}-p)^3 + (\sigma_{III}-p)^3] }</math>.
The values printed consist for mechanical elements of the three principal stresses <math>\sigma_I, \sigma_{II}, \sigma_{III}</math>, then the max shear <math>(\sigma_I - \sigma_{III})/2</math>, then the pressure <math>p = \frac{1}{3}\mathrm{tr}[\sigma]</math>, then "J2" printed as <math> \sqrt{\frac{3}{2}} \Vert \mathbf{s} \Vert </math> (the equivalent tensile stress, also known as the equivalent Mises stress, note <math> \mathbf{s} </math> is the deviatoric stress tensor), and finally "J3" printed as <math> \sqrt[3]{ \frac{1}{3}[ (\sigma_I-p)^3 + (\sigma_{II}-p)^3 + (\sigma_{III}-p)^3] }</math>.


=== Second set of values (# Value) ===
== Second set of values (# Value) ==
This is then followed by the six components of the stress tensor <math> \sigma_{11}, \sigma_{22}, \sigma_{33}, \sigma_{12}, \sigma_{23}, \sigma_{31} </math> and the six components of the strain tensor <math> \varepsilon_{11}, \varepsilon_{22}, \varepsilon_{33}, \varepsilon_{12}, \varepsilon_{23}, \varepsilon_{31} </math>.
This is then followed by the six components of the stress tensor <math> \sigma_{11}, \sigma_{22}, \sigma_{33}, \sigma_{12}, \sigma_{23}, \sigma_{31} </math> and the six components of the strain tensor <math> \varepsilon_{11}, \varepsilon_{22}, \varepsilon_{33}, \varepsilon_{12}, \varepsilon_{23}, \varepsilon_{31} </math>.


=== Third set of values (# History) ===
== Third set of values (# History) ==
If the user has mapped element history variables for plotting using the <code>HIST PLOT hvar hpnum</code> card in the material definition, then these values will be printed, the enumeration matching hpnum.
If the user has mapped element history variables for plotting using the <code>HIST PLOT hvar hpnum</code> card in the material definition, then these values will be printed, the enumeration matching hpnum.

Latest revision as of 10:15, 23 May 2018

When you issue the command STREss,NODE,n1,n2,n3 at the Macro prompt, FEAP will compute a nodal projection of the Gauss point values and print them for nodes n1 to n2 in increments of n3 (default 1).

Mechanical Elements

First set of values

The values printed consist for mechanical elements of the three principal stresses , then the max shear , then the pressure , then "J2" printed as (the equivalent tensile stress, also known as the equivalent Mises stress, note is the deviatoric stress tensor), and finally "J3" printed as .

Second set of values (# Value)

This is then followed by the six components of the stress tensor and the six components of the strain tensor .

Third set of values (# History)

If the user has mapped element history variables for plotting using the HIST PLOT hvar hpnum card in the material definition, then these values will be printed, the enumeration matching hpnum.