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The procedure for a p-method static analysis consists of four main steps:
Select the p-method procedure.
Build the model.
Apply loads and obtain the solution.
Review the results.
Each step is discussed in detail in the following sections.
You can activate the p-method solution procedure in two ways: through the GUI or by defining a p-element [ET].
Activating p-method through the GUI:
| Command(s): | /PMETH |
| GUI: | Main Menu> Preferences> p-method Electr. |
Defining a p-element: The p-method solution procedure can also be activated by defining a p-element. If you are working outside of the GUI, the definition of a p-element lets the program know that a p-method solution is to be done; no other commands are necessary to initiate p-method. From within the GUI, you can also issue the ET command in the "Input Window" to activate the p-method procedure. (Remember, the ET command must be entered in the "Input Window," since, by default, only h-elements are displayed in the GUI unless p-method is active.)
| Command(s): | ET |
| GUI: | Main Menu> Preprocessor> Element Type> Add/Edit/Delete |
To build a model with p-elements, you may follow the procedure listed below.
Define the element types.
Specify material properties.
Define the model geometry.
Mesh the model into elements.
The above steps are common to most analyses. The Modeling and Meshing Guide explains those steps in detail. In this section we will explain the techniques that are unique to a p-analysis.
You can use the following two p-elements to build your model:
| Element | Dimens. | Shape or Characteristic | DOFs |
|---|---|---|---|
| SOLID127 | 3-D | Tetrahedral, 10 nodes | Voltage at each node |
| SOLID128 | 3-D | Hexahedral, 20 nodes | Voltage at each node |
h-elements and p-elements cannot be active at the same time in your model (except for the MATRIX50 element use as a superelement for a Trefftz domain).
Various options are available for use with p-elements. One important option is the ability to specify, either locally or globally, a range in which the p-level may vary.
The range within which the p-level may vary can be controlled locally through the p-element KEYOPT settings (KEYOPT(1) and KEYOPT(2)), or globally across the entire model with PPRANGE. By default, the p-level range is 2 to 8.
When both KEYOPT values and PPRANGE have been used to specify p-level ranges, the local p-level range set by KEYOPT(1) and KEYOPT(2) will take precedence over the global p-level range [PPRANGE].
For example, if you set a global p-level range between 3 and 8 with PPRANGE, then define a local p-level range of 4 to 6 for SOLID127 elements (ET,1,127,4,6), the p-level for the SOLID127 elements may only vary between 4 and 6, while the rest of the model may vary between 3 and 8.
At the (default) starting p-level of 2, convergence checking is performed (PEMOPTS command) to determine those elements which are converged and may have their p-level fixed at 2. That is, these elements will remain at a p-level of 2, and will be eliminated from any further convergence checking. Additional checking is performed at each iteration to fix the p-levels of the elements which are converged.
Use local p-range control to eliminate regions of little importance from high p-escalation. Use global p-range control for overall control of the p-level. These range controls are not necessary, but p-escalations to high p-levels increase CPU run time. Therefore, it is advantageous to have such controls available.
See the Elements Reference for complete descriptions of each of the above element types.
You may solve electrostatic field problems in a variety of units. ANSYS requires that all geometry dimensions, properties, and input loads (excitations) be consistent with respect to a units system. By default, ANSYS supports the MKS (or MKSV) system of units (meter, kilogram, second, volt, ampere). For microsystems, it may be more advantageous to work in other systems of units such as a µMKSV (micrometer, kilogram, second, volt, pico-ampere) or a µMSVfA (micrometer, second, volt, femto-ampere, gram). For electrostatic analysis, you must select an appropriate value of free-space permittivity consistent with the system of units to be used. This is done via the EMUNIT command. By default, the free-space permittivity is 8.854e-12 Farads/meter (MKSV units). For µMKSV units, you should use 8.854e-6 pico-Farads/micro-meter. For µMSVfA units, you should use 8.854e-3 femto-Farads/micro-meter. See Building the Model for a more complete description of alternate systems of units.
To specify a system of units, issue one of the following:
| Command(s): | EMUNIT |
| GUI: | Main Menu> Preprocessor> Material Props> Electromag Units |
Material properties for p-elements (relative permittivity) may be either constant or temperature-dependent, as well as isotropic or orthotropic.
To define relative permittivity, issue one of the following:
| Command(s): | MP |
| GUI: | Main Menu> Preprocessor> Material Props> Material Models> Electromagnetics> Relative Permittivity> Isotropic |
Element coordinate systems [ESYS] may be used for orthotropic material directions. All element results in POST1 however may only be viewed in Global Cartesian Coordinations.
You can create your model using any of the various techniques outlined in the Modeling and Meshing Guide, or you can import it from a CAD system. If you are generating your model from within ANSYS, you can use either solid modeling or direct generation techniques.
Using direct generation is not recommended when you plan to create a p-mesh since all p-elements require that midside nodes be included in their geometric definition. In cases where surface curvature is important, it would not only be tedious, but possibly imprecise to manually define each midside node. In addition, the EMID command does not place nodes on a curved line. It is much more convenient to let the program generate the midside nodes using solid modeling.
You may not drop any midside nodes from p-elements.
If you use direct generation or import your mesh from an outside source, keep the following guidelines in mind:
A curved element edge should not cover more than a 30° arc.
The angles between adjacent edges should be between 10° and 170°. Element shape checking will warn that adjacent edges should be between 30° and 150°, but it is usually acceptable to have angles in the range of 10° to 170° for p-elements.
A good rule of thumb is to keep the aspect ratio (ratio of element length to width) less than 20:1.
For electrostatic field analysis it is not necessary to mesh the conductor region of the model with p-elements since the surface of the conductor is assumed to be at an equipotential. Therefore, only the surrounding dielectric material and the free-space (air) regions require p-element meshing.
The surfaces which make up a conductor do require special treatment. They must either have a specified potential applied, or have the nodes at the surface of the conductor coupled if the voltage is unknown. See Coupling below for details.
After you have generated your solid model, you are ready to mesh it with p-elements. The general procedure for meshing your solid model is outlined in "Generating the Mesh" in the Modeling and Meshing Guide. Compared to h-elements, the program will generate a coarser mesh under default settings for p-elements. Normally, you will not need to specify any meshing size controls because the program defaults will give you an adequate mesh. In addition, each element's p-level will be manipulated during solution to obtain accurate and efficient results. For engineering design studies, the accuracy obtained with a relatively coarse, ungraded mesh is usually sufficient. (A graded mesh is one where there are more elements near an area of interest. These elements are smaller relative to the other areas of the model, and a transition region occurs from the large to the smaller elements.)
By default, the DESIZE command controls automatic element sizing. For free meshing, you have the option of using the SmartSize feature [SMRTSIZE] to control element sizing. SmartSizing generally produces a better quality mesh and is recommended for meshing a p-element model. (SmartSizing is not available for mapped meshing.)
To specify meshing parameters for automatic (smart) element sizing, issue one of the following:
| Command(s): | SMRTSIZE |
| GUI: | Main Menu> Preprocessor> Meshing> Size Cntrls> SmartSize> Basic |
To specify default element sizes, issue one of the following:
| Command(s): | DESIZE |
| GUI: | Main Menu> Preprocessor> Meshing> Size Cntrls> Global> Other |
Since p-method prefers a coarser mesh, the default element size values for a p-method analysis are different than those used for h-elements. See the SMRTSIZE and DESIZE commands for details.
You may also want to specify meshing controls for curved geometries, where successful meshes are more difficult to achieve with the default size settings. Under default conditions, badly shaped elements may be produced because of the difficulty of filling a curved domain with as few elements as possible. User-defined meshing controls can make the task less difficult.
Subdivide complex geometries, or build them as separate geometries. As a general rule, if you were to stand inside a volume, you should be able to see all of its vertices. If this is not possible, you might wish to consider subdividing the volume into more manageable pieces.
The number of divisions on lines "parallel" and near to each other should be fairly equivalent. The SmartSizing method of meshing [SMRTSIZE] handles this situation well. However, if the DESIZE method of element sizing is used, you should set local mesh controls to achieve a good mesh in these areas.
A subgrid approach is used for plotting the model in which the amount of displayed element curvature can be controlled. You may display varying degrees of curvature in your model by specifying the number of facets to be used for element display. Facets are piece-wise linear approximations of the actual curve represented by the element face or edge. A greater number of facets will result in a smoother representation of the element surface for p-element plots. PowerGraphics is the default graphics display method used for p-method plots. This method will display the plot at a much faster speed than the Full Model method. See "PowerGraphics" in the Basic Analysis Guide for more information on PowerGraphics. For more information on /EFACET, see the discussion on the p-element subgrid later in this section.
To specify the number of facets per element edge for PowerGraphics displays, issue one of the following:
| Command(s): | /EFACET |
| GUI: | Utility Menu> PlotCtrls> Style> Size and Shape |
The Trefftz method may be used to model the far-field effects at the boundary of the finite element model. The Trefftz method combines the efficiency of boundary techniques in open domain treatment with a finite element-like positive definite stiffness matrix. For the p-method, a Trefftz domain may be used on 3-D models containing no planes of symmetry. Details on setting up and using a Trefftz domain are exactly the same as for the h-method electrostatic elements. For details on this procedure, see Trefftz Method for Open Boundary Representation.
You may couple degrees of freedom (DOFs) between nodes on p-elements to control nodal solution behavior. All coupled nodes are forced to assume the same electric potential value in the specified nodal coordinate direction. The value of this electric potential is unknown until the analysis has been completed.
To define a set of coupled degrees of freedom, issue one of the following:
| Command(s): | CP |
| GUI: | Main Menu> Preprocessor> Coupling/Ceqn> Couple DOFs |
You normally use coupling on conductor surface nodes to prescribe an equipotential surface of unknown voltage or to prescribe a periodic boundary condition on two surfaces of a model with matching node pairs.
The first degree of freedom defined on the coupled set is the "prime" degree of freedom. All other degrees of freedom in the coupled set are eliminated from the solution matrices as a result of their relationship to the prime degree of freedom.
For p-elements, only the corner nodes may be defined as prime degrees of freedom if midside nodes are also part of the same coupled set.
For a p-method analysis, only the nodal combinations described below are permitted when coupling, and any deviation from these combinations will most likely result in singularities.
Both corner nodes on the element's edge or face are part of the same coupled set. Only the corner nodes may be defined as prime degrees of freedom. This is the most common occurrence in electrostatics whereby an entire edge of a model or a conductor is coupled.
All nodes in the coupled set are midside nodes. In this case, a midside node must be defined as the prime degree of freedom, but this is only valid as long as there are no corner nodes defined as part of the same coupled set.
You may write constraint equations between nodes on p-elements to control nodal solution behavior. A constraint equation forces all nodes to a specified relationship. In electrostatics, constraint equations usually prescribe a periodic behavior of the potential from one surface to another surface with matching node pairs. For example, the potential solution on one surface of a model is equal in magnitude but opposite in sign to the potential values on another surface of the model. They are also used with a Trefftz domain to model the far-field. The value of the potential is unknown until the analysis has been completed.
To define a constraint equation relating degrees of freedom, issue one of the following:
| Command(s): | CE |
| GUI: | Main Menu> Preprocessor> Coupling/Ceqn> Constraint Eqn |
Constraint equations for p-elements have the following limitations:
As shown in Figure 14.5: "Constraint Equations Relating Corner Nodes", you may write VOLT constraint equations relating any corner node to any other corner node. You may not write a constraint equation relating a corner node to a midside node.
As shown in Figure 14.6: "Acceptable Constraint Equations Relating Midside Nodes", you may write VOLT constraint equations relating any midside node to any other midside node, if you write VOLT constraint equations for all three nodes on an edge, or all nodes on a face.
As shown in Figure 14.7: "Unacceptable Constraint Equations Relating Midside Nodes", you may NOT write a constraint equation that only relates midside nodes.
These restrictions come from the fact that in a p-method electrostatic analysis, the VOLT DOF of a corner node represents the electric potential value at the node, while the VOLT DOF of a midside node is the second order hierarchic edge mode value. By following these restrictions, a potential solution of second order (p = 2) can be achieved on the edges or faces with constraint equations defined.
These loads specify flux-parallel, flux-normal, far-field, and periodic boundary conditions, as well as an imposed external magnetic field. The following table shows the value of volt required for each type of boundary condition:
| Boundary Condition | Value of VOLT |
|---|---|
| Flux-parallel | None required (naturally occurring). |
| Flux-normal | Specify a constant value of VOLT using the D command (Main Menu> Solution> Define Loads> Apply> Electric> Boundary> Voltage> J-Normal> On Nodes (On Lines or On Areas). |
| Far-field | For 2-D analysis, use INFIN9 (planar analyses only) or INFIN110 elements. For 3-D analysis, use the Trefftz formulation or INFIN47 or INFIN111 elements. |
| Imposed external field | Apply nonzero values of VOLT. Use Main Menu> Solution> Define Loads> Apply> Electric> Boundary> Voltage> On Keypoints (On Nodes, On Lines or On Areas). |
Flux-parallel boundary conditions force the flux to flow parallel to a surface, while flux-normal boundary conditions force the flux to flow normal to a surface. You do not need to specify far-field zero boundary conditions if you use the Trefftz formulation or far-field elements to represent the "infinite" boundary of the model. For an imposed external field, specify the appropriate nonzero value of VOLT.
In this section you will take the following steps to obtain a solution for your model:
Enter SOLUTION.
| Command(s): | /SOLU |
| GUI: | Main Menu> Solution |
Define the analysis options. Choose any of three options to solve the simultaneous equations generated by a p-method analysis. These solvers are discussed at length in "Solution" in the Basic Analysis Guide.
Frontal equation solver
Jacobian Conjugate Gradient equation solver (JCG) (recommended)
Incomplete Cholesky Conjugate Gradient (ICCG)
Preconditioned Conjugate Gradient equation solver (PCG)
To specify the type of equation solver, issue one of the following:
| Command(s): | EQSLV |
| GUI: | Main Menu> Solution> Analysis Type> Analysis Options |
We generally recommend that you use the JCG solver for a p-element analysis. For most 3-D solid models and for very large 2-D models (usually greater than 40,000 DOF), the JCG solver is usually faster than the frontal solver.
In certain cases, such as when your model contains elements with high aspect ratios or material type discontinuities, a greater number of iterations may be required to achieve convergence for the PCG solver. You may increase the maximum number of iterations by using the MULT option on the EQSLV command. This option is only valid when solving with the PCG solver. See the EQSLV command description in the Commands Reference for more information on this capability.
For more information on the general use of the PCG solver, refer to "Solution" in the Basic Analysis Guide.
Apply the loads to the solid model (keypoints, lines, areas, etc.) or the finite element model (nodes and elements), except for inertia loads (gravity, rotational velocity, etc.), which are independent of the model. For a general discussion of solid model loads versus finite element loads, see "Loading" in the Basic Analysis Guide.
Loads Applicable to a p-Method Analysis
"Electrostatic Field Analysis (h-Method)" of this manual describes the loads applicable to an electrostatic analysis, including the commands associated with each type of loading.
Potential (VOLT) are DOF constraints that you would usually prescribe at a ground plane, a conductor, or at a far-field boundary. You can also use them to indicate symmetry boundary conditions.
Potential boundary conditions applied to all nodes of an element edge or face will also constrain the higher order potential variation along that edge or face.
You should not apply a potential only at a midside node. You may apply a potential at a corner node only.
Charge (CHRG) are point-wise loads that you would usually specify on a corner node.
Observe the following cautions:
You should be cautious applying single-point charge, since they cause field singularities. If these loads are applied, exclude the elements attached to these nodes from the convergence computations. See "Accounting for Singularities" below.
Do not apply charge to the midside nodes. You may only apply these loads at the corner nodes.
Surface Charge Densities (CHRGS) are surface loads, also usually applied on the exterior of a body.
Volume Charge Densities (CHRGD) are body loads usually applied to elements.
Maxwell Surface Flag (MXWF) are flags indicating surfaces to compute forces. Surfaces of air elements adjacent to conductors or mechanical structures are usually flagged. Elements with flagged surfaces will have surface forces computed and stored. These forces can be reviewed in the postprocessor, or automatically transferred to a structural analysis (of the conductor or mechanical structure). The total “Global” force on a body may also be used as consequence criteria in the adaptive process.
You apply surface flags using the SF family of commands. Remember to apply these flags to electrostatic air elements adjacent to the conductor or mechanical body. In a pure electrostatic model, these conductors are not physically represented by elements so application of the surface flags is straightforward. In a multiphysics analysis, you can mesh the conductor region with finite elements which are inactive for the electrostatic run (using the 'null' element type (ET,,0). In this case, you can apply Maxwell surface flags by grouping the conductor elements into an element component (CM command) and calling the FMAGBC command macro.
The electrostatic p-elements output forces that are compatible with lower and higher order structural h-elements only. Transfer forces from the electrostatic analysis to a structural analysis by using the LDREAD command. Use element KEYOPT(7) for SOLID127 and SOLID128 to prescribe force computations for either lower order or higher order structural elements.
The structural p-elements (SOLID147 and SOLID148) do not support electrostatic-structural coupling.
Temperatures (TEMP) are applied to study the effects of temperature dependent permittivity. You can read in temperatures from a thermal analysis, or you can specify temperatures directly on the nodes or the solid model keypoints.
To obtain temperatures from a thermal analysis:
Mesh the p-element model.
Convert the p-element types to the following thermal element types: SOLID128 to SOLID90, and SOLID127 to SOLID87.
Run the thermal analysis.
Change the element types back to the p-element types in order to perform the p-method electrostatic analysis.
For the remainder of the analysis, continue with the same procedure as defined for h-elements (see the Thermal Analysis Guide).
Specify load step options. The following solution options are available to aid in solving a p-Method analysis:
Convergence criteria specifications
Specifications for controlling p-levels
Accounting for singularities
As mentioned earlier in this section, a p-method analysis works with a series of iterations, or p-loops, checking for convergence each time. The PPRANGE command is used to specify the overall range where the p-level may vary (somewhere between 2 and 8). For analyses beginning at p = 2, each element will have its solution checked for convergence against established criteria [PCONV]. If the solution is within the requested tolerance [PEMOPTS], that element will have its p-level held to 2. Those elements that did not converge within the specified criteria (that is, not fixed at p = 2 for the first iteration), will have their p-level increased, and another solution (iteration) will then be performed. At each iteration the convergence criteria (energy, potential, electric field, global forces, etc.) is checked, and if converged, the solution stops. Also, those elements whose individual solutions are considered to be converged will have their p-level held at the current p-level. This process is continued until all specified convergence criteria are met, or the maximum p-range has been reached.
Convergence Criteria Specifications
Convergence criteria may be global (for energy or surface Maxwell) forces) or local. Global energy is a good criteria to use when capacitance is the desired result. Electrostatic forces (Maxwell forces) on a body may be used as a convergence criteria. Forces are summed over all flagged surfaces to obtain a global force. This global force is then used as a convergence criteria.
Caution must be exercised when using the global force (EFORC) criteria. Since all flagged surface forces are summed, only a single body should be flagged. Otherwise, for more than one flagged body, the total force may be meaningless (or in fact, may sum to zero).
If you are specifically interested in the results at certain points in the model, then you should use local convergence criteria. Use this option to specify which areas of your model you would like to monitor for analysis convergence, as well as the type of criteria you would like to use to control convergence. Typically, you should select a few points of interest (nodes), at which to specify the convergence criteria (potential, electric field, etc.). In most cases, the default convergence tolerance (5%) is sufficient for generally good results. You may want to lower this tolerance if you require a more accurate solution. For a design study or optimization analysis, a higher tolerance will cut down on run times.
To set convergence values for p-method solutions, issue one of the following:
| Command(s): | PCONV |
| GUI: | Main Menu> Preprocessor> Loads> Load Step Opts> p-Method> Convergence Crit |
Do not specify electric field or flux density criteria at nodes where there are singularities. These locations will not converge due to the singularity. Caution must be used in assigning criteria at material discontinuities. In this case, the criteria should only be applied to the continuous component of the field across the material interface.
When choosing locations for specifying convergence criteria, you should concentrate your monitoring in the areas of high electric field or at the point of maximum potential rather than locations where the electric field or potential are relatively insignificant.
Specifications for Controlling p-levels
You may specify the starting (defaults to 2) and maximum (defaults to 8) p-levels that you wish to allow for your analysis [PPRANGE]. You may wish to start at a higher p-level if you have already completed an analysis and you want to perform a re-analysis (for a design change, for instance) and you know the final p-level where convergence will occur for most elements. You may also want to restrict the maximum p-level to less than 8 if conserving disk space or run time.
Adjust the starting and maximum p-level in portions of your model using element KEYOPT selections.
Accounting for Singularities
If the model contains any re-entrant (internal or concave) corners that are not modeled with a fillet radius, or contains point charges or any other areas of singularities, you should consider excluding these areas from the convergence computations. All elements that have a node at the singularity should be excluded.
To specify elements to be excluded from p-level escalations, issue one of the following:
| Command(s): | PEXCLUDE |
| GUI: | Main Menu> Solution> Load Step Opts> p-Method> Stored Energy> Exclude Elems |
You can reassign, or re-include, elements for convergence checking. You may determine which elements have been included or excluded by listing [PINCLUDE,STAT; PEXCLUDE,STAT; or *GET] or plotting elements [EPLOT]. Excluded elements will appear `whited-out' in the plot. You may also select included or excluded elements by issuing the ESEL command directly [ESEL,,PEXC or ESEL,,PINC] (no GUI equivalent). This facilitates using these elements as a component [CM].
To specify elements to be included in p-level escalations, issue one of the following:
| Command(s): | PINCLUDE |
| GUI: | Main Menu> Solution> Load Step Opts> p-Method> Stored Energy> Include Elems |
Save a backup copy of the database.
| Command(s): | SAVE |
| GUI: | Utility Menu> File> Save As |
Start the p-level iterations and solution process. The output will provide a summary of each loop, indicating the current p-level, the convergence statistics, and the status of how many elements have converged.
| Command(s): | SOLVE |
| GUI: | Main Menu> Solution> Solve> Current LS |
For a p-method electrostatic analysis, ANSYS computes convergence norms for each p-loop. Available in both batch and interactive sessions, the Graphical Solution Tracking (GST) feature displays the computed convergence norms and criteria while the solution is in process. By default, the GST feature is on for interactive sessions and off for batch runs. To turn the GST feature on or off, use either of the following:
| Command(s): | /GST |
| GUI: | Main Menu> Solution> Output Ctrls> Grph Solu Track |
Refer to Tracking Convergence Graphically to see a typical GST display.
If the analysis is not successful, try the following steps to identify and correct the cause for failure:
| Problem: "Negative Pivot" error encountered. |
| Possible Cause: No constraints on the potential in the model. At least one node must be restrained to a fixed potential. |
| Solution: Apply a fixed potential to at least one node. |
| Problem: Solution does not converge to within the requested tolerance. |
| Possible Causes: There are several possible causes. You may use the general postprocessor [/POST1] to look at this solution in order to determine the difficulty. |
| Possible Causes | Solution |
|---|---|
| The convergence criteria is too tight for the maximum allowable p-level and the mesh. | Relax the convergence criteria. |
| The convergence criterion was specified at a singularity (infinite field value, such as under a point charge) or the elements near the singularity were not excluded. | Do not monitor a singularity point. |
| The mesh is too coarse, especially in the area where the electric field is high. | Refine the mesh. |
| The maximum p-level was restricted lower than that required for convergence. | Allow the maximum p-level to go higher. |
| The convergence criterion is at a location where the angle made by adjacent element edges is greater than 55° on a curved boundary. | Refine the mesh in that region. |
You may not restart a p-method analysis.
The fundamental procedures for general postprocessing of results [/POST1] in the ANSYS program are discussed in "An Overview of Postprocessing" in the Basic Analysis Guide. Although most of these capabilities are directly applicable to p-method analyses, some techniques for reviewing results are unique to p-method, such as
p-Element Subgrid Plotting
Printing and Plotting Node and Element Results
Specialized p-Method Displays and Listings
The results from a p-method analysis are written to the results file, Jobname.RMG. Primary data are the potential (VOLT) results calculated at each node. Derived data are the nodal and element results for electric field, flux density, Maxwell forces, and energy.
You must read the results data from the results file (Jobname.RMG) into the database [SET] before potentials may be reviewed during postprocessing.
As mentioned previously, p-method finite element models generally contain fewer elements than do models meshed with h-elements. Since fewer elements correspond to a coarser mesh, a subgrid approach has been devised for viewing results in POST1. In this approach, each element is divided into smaller, "h-like" elements. Both the display of geometric curvature and the display and printout of field quantities (equipotentials, electric field, etc.) are affected by this approach. In most cases, a greater number of facets will result in a smoother representation of the element surface and results contours for p-element plots.
The key command involved in the subgrid approach is /EFACET,NUM where NUM represents the number of facets per element edge (GUI path Utility Menu> PlotCtrls> Style> Size and Shape). The example below illustrates how /EFACET subdivides a quadrilateral element. If NUM = 2, the element has 2 facets per edge and is divided into 4 subgrid facets by adding a pseudo node at the "center". If NUM = 4, the element has 4 facets per edge which means two pseudo nodes per edge and 9 interior pseudo nodes are added for each p-element, dividing the quadrilateral into 16 subgrid facets.
As a general rule, for a model with a very coarse mesh or any model in which the p-levels are high (p>3) you should consider using NUM = 4 to view your field quantities. Since results are available at each subgrid location, more information will be available at NUM = 4.
Potentials, electric field, Maxwell forces, and electric flux density can be listed [PRNSOL] at all node locations (both corner and midside nodes). Likewise, these nodal values can be contoured for display purposes [PLNSOL], with the contour resolutions being controlled by the /EFACET command.
When viewing nodal field values across p-element boundaries ([PRNSOL, PLNSOL], or when using the Query function), results may be displayed in various ways. The results data may be averaged along element boundaries with the AVRES command. You can average results at all boundaries (the default), or at all boundaries except where real constant, and/or material type discontinuities exist. If a geometric discontinuity exists, results will not be averaged at those locations.
AVRES has no effect on the nodal potentials (VOLT).
Electric field and electric flux density can be listed [PRESOL] at all node locations for each element.
Printout is similar to that for h-elements, with nodal results being unaveraged and sorted by element number. Unlike higher order h-element printout, results are for all nodal locations (corner and midside nodes). Results may be printed or plotted for the entire model [/GRAPHICS,FULL] or for the model surface only [/GRAPHICS,POWER] (default).
There are three commands specifically designed for listing or plotting p-element results data [PRCONV, PLCONV, PPLOT]. You may print [PRCONV] or plot [PLCONV] the previously-specified convergence values [PCONV] versus characteristic p-levels. The characteristic p-level refers to the p-level range from the minimum specified [PPRANGE] to the maximum p-level reached during SOLUTION. Final p-levels that were assigned to individual elements can be viewed by means of the PPLOT command. A convenient way to visualize local convergence criteria at specified locations in the model is to display a symbol at the location of interest, [/PSYMB,PCON], then issue an element or node plot.