Case Files¶
Each simulation is defined by six required case files:
- SESSION.NAME
- par (runtime parameters)
- re2 (mesh and boundaries)
- usr (user defined functions for inital/boundary condition etc.)
- SIZE (parameters for static memory allocation)
- map/ma2 (element processes mapping)
Additional optional case files may be generated or included:
- f%05d (solution data)
- his (probing point data)
SESSION.NAME¶
To run Nek5000, each simulation must have a SESSION.NAME
file.
This file is read in by the code and gives the path to the relevant files describing the structure and parameters of the simulation.
It contains the name of the simulation and the full path to supporting files.
For example, to run the eddy example from the repository, the SESSION.NAME
file would look like:
eddy_uv
/home/user_name/Nek5000/short_tests/eddy/
This file is generated automatically by the nek
, nekb
, nekmpi
, nekbmpi
, neknek
and neknekb
scripts at runtime.
If you are calling $ mpirun
directly, such as in a submission script for an HPC system, you must manually generate this file or setup your script to generate it for you.
Warning
When using NekNek, SESSION.NAME
is substantially different.
We recommend running the example and checking the neknek
script for further information.
Parameter File (.par)¶
The simulation paramaters are defined in the .par
file.
The keys are grouped in different sections and a specific value is assigned to each key.
The .par
file follows the structure exemplified below.
#
# nek parameter file
#
[SECTION]
key = value
...
[SECTION]
key = value
...
The sections are:
GENERAL
(mandatory, see: General Parameters)PROBLEMTYPE
(see: Problem Type Parameters)MESH
(see: Mesh Parameters)VELOCITY
(see: Velocity Parameters)PRESSURE
(required for velocity see: Pressure Parameters)TEMPERATURE
(see: Temperature Parameters)SCALAR%%
(see: Passive Scalar Parameters)CVODE
(see: CVODE Parameters)
Additionally, some parameters are common to multiple sections:
- Common Parameters (Common to all field variables)
- Temperature and Passive Scalar Common Parameters (Common to both temperature and passive scalar fields)
When scalars are used, the keys of each scalar are defined under the section SCALAR%%
varying between SCALAR01
and SCALAR99
.
The descripton of the keys of each section is given in the following tables (all keys/values are case insensitive).
The value assigned to each key can be a user input (e.g. a <real> value) or one of the avaliable options listed in the tables below.
Values in parentheses denote the default value.
General Parameters¶
Key | Value(s) | Description |
---|---|---|
startFrom |
<string> |
Absolute/relative path of the field file to restart the simulation from. Also includes several restart options (see Restart Options for details) |
stopAt |
(numSteps ), endTime |
Stops the simulation after a given number of time steps or at a given physical time. |
endTime |
<real> |
Final physical time at which we want to our simulation to stop. Required for stopAt = endTime . |
numSteps |
<int> |
Number of time steps until the simulation stops. Required for stopAt = numSteps . |
dt |
<real> |
Specifies the step size or in case of a variable time step, the maximum step size |
variableDT |
(no ), yes |
Controls if the step size will be adjusted to match the targetCFL. |
initialDT |
<real> |
Controls the initial time step size. Requires variableDT = yes . |
targetCFL |
<real> |
Sets stability/target CFL number for OIFS or variable time steps. This is fixed to 0.5 for extrapolation = standard |
writeControl |
(timeStep ), runTime |
Specifies whether checkpointing is based on number of time steps or physical time. |
writeInterval |
<real>/<int> |
Checkpoint frequency in physical time (<real> ) or number of time steps (<int> ) |
filtering |
(none ), explicit , hpfrt |
Specifies the filtering method. See Stabilizing Filters for details. |
filterModes |
<int> |
Specifies the number of modes filtered as an alternative to specifying the cutoff ratio. Note: requires the use of at least 2 modes. See Stabilizing Filters for details. |
filterCutoffRatio |
<real> |
Ratio of modes not affected by the filter. Use as an alternative to specifying the number of modes explicitly. See Stabilizing Filters for details. |
filterWeight |
<real> |
Sets the filter strength of transfer function of the last mode (explicit) or the relaxation parameter in case of hpfrt. See Stabilizing Filters for more information. |
writeDoublePrecision |
no , (yes ) |
Sets the precision of the output field files. |
writeNFiles |
<int> , (1 ) |
Sets the number of output files. By default a parallel shared file is used. |
dealiasing |
no , yes |
Enable/diasble over-integration. |
timeStepper |
BDF1 , (BDF2 ), BDF3 |
Time integration order. |
extrapolation |
(standard ), OIFS |
Extrapolation method. Can be used to achieve CFL > 0.5 with OIFS . |
constFlowRate |
(none ), X , Y , Z |
Prescribes a constant volumetric flow in the given direction. Requires meanVolumetricFlow or meanVelocity . |
meanVolumetricFlow |
<real> |
Sets the volumetric flow rate in the direction of constFlowRate . |
meanVelocity |
<real> |
Sets the mean velocity (volume-weighted velocity mean) in the direction of constFlowRate . |
optLevel |
<int> , (2 ) |
Optimization level |
logLevel |
<int> , (2 ) |
Controls the verbosity level of the logfile. |
userParam%% |
<real> |
User parameter (can be accessed through uparam(%) array in .usr . Supports up to 20 parameters. |
Problem Type Parameters¶
Key | Value(s) | Description |
---|---|---|
equation |
(incompNS ), lowMachNS , steadyStokes , incompLinNS , incompLinAdjNS , incompMHD , compNS |
Specifies equation type |
axiSymmetry |
(no ), yes |
Axisymmetric problem |
swirl |
(no ), yes |
Enable axisymmetric azimuthal velocity component (stored in temperature field |
cyclicBoundaries |
(no ), yes |
Sets cyclic periodic boundaries |
numberOfPerturbations |
(1 ) |
Number of perturbations for linearized NS |
solveBaseFlow |
(no ), yes |
Solve for base flow in case of linearized NS |
variableProperties |
(no ), yes |
Enable variable transport properties |
stressFormulation |
(no ), yes |
Enable stress formulation |
dp0dt |
(no ), yes |
Enable time-varying thermodynamic pressure |
Common Parameters¶
These parameters are available for field variables.
Key | Value(s) | Description |
---|---|---|
residualTol |
<real> |
Residual tolerance used by solver (not for CVODE) |
residualProj |
(no ), yes |
Controls the residual projection |
writeToFieldFile |
no , (yes ) |
Controls if fields will be written on output |
boundaryTypeMap |
<string-list> |
Maps the boundary condition types to boundary IDs for third-party meshes |
Note
Some boundary types have plain-english equivalents that can be used in the .par
file in lieu of the character identifiers. See Table 7 and Table 8.
Additionally, none
can be used to keep the cbc
array empty.
Plain-English BC Identifiers¶
The plain-English boundary condition identifiers can be used in the .par
file instead of the character identifier codes.
Note that some character codes have multiple corresponding plain-English identifiers.
Identifier | Equivalents |
---|---|
A |
axis |
v |
dirichlet, inlet |
int |
interpolated |
O |
outlet |
o |
pressure |
P |
periodic |
SYM |
symmetry |
W |
wall |
Identifier | Equivalents |
---|---|
A |
axis |
c |
convection, robin |
t |
dirichlet, inlet |
f |
flux, neumann |
I |
insulated, outlet, symmetry |
int |
interpolated |
P |
periodic |
r |
radiation |
Mesh Parameters¶
Key | Value(s) | Description |
---|---|---|
boundaryIDMap |
<int-list> , (1,2,3... ) |
Maps the boundary types to their corresponding boundary IDs |
motion |
(none ), user , elasticity |
Mesh motion solver |
viscosity |
<real> , (0.4 ) |
Diffusivity for elasticity solver |
numberOfBCFields |
(nfields ) |
Number of field variables which have a boundary condition in .re2 file |
firstBCFieldIndex |
(1 ) or 2 |
Field index of the first BC specified in .re2 file |
Velocity Parameters¶
Key | Value(s) | Description |
---|---|---|
viscosity |
<real> |
Dynamic viscosity. A negative value sets the Reynolds number |
density |
<real> |
Density |
Pressure Parameters¶
Key | Value(s) | Description |
---|---|---|
preconditioner |
(semg_xxt ) |
Standard preconditioning method. Requires no additional setup. Only recommended for problems with \(E<350,000\). |
– | semg_amg |
First time usage of semg_amg with write three dump files to disc. The amg_hypre tool will then need to be run to create the setup files required for the AMG solver initialization. |
– | semg_amg_hypre |
Recommended for \(E≥350,000\). Requires compiling with HYPRE support. |
– | fem_amg_hypre |
May be faster for meshes with high aspect ratios. Requires compiling with HYPRE support. |
solver |
(GMRES ), CGFLEX |
Solver for pressure |
Temperature and Passive Scalar Common Parameters¶
Key | Value(s)
|
Description
|
---|---|---|
solver |
(
helm )cvode none |
Solver for scalar
|
advection |
no (
yes ) |
Controls if advection is present
|
absoluteTol |
<real> |
Absolute tolerance used by CVODE
|
Temperature Parameters¶
Key | Value(s)
|
Description
|
---|---|---|
ConjugateHeatTransfer |
(
no )yes |
Controls conjugate heat transfer
|
conductivity |
<real> |
Thermal conductivity
|
rhoCp |
<real> |
Product of density and heat capacity
|
Note: [TEMPERATURE] solver = none
is incompatible with [PROBLEMTYPE] equation = lowMachNS
without defining a custom thermal divergence in the usr
file.
Passive Scalar Parameters¶
Key | Value(s)
|
Description
|
---|---|---|
density |
<real> |
Density
|
diffusivity |
<real> |
Diffusivity
|
CVODE Parameters¶
Key | Value(s)
|
Description
|
---|---|---|
relativeTol |
<real> |
Relative tolerance (applies to all scalars)
|
stiff |
no (
yes ) |
Controls if BDF or Adams Moulton is used
|
preconditioner |
(
none )user |
Preconditioner method
|
dtMax |
<real> |
Maximum internal step size
Controls splitting error of velocity
scalar coupling (e.g. set to 1-4 dt)
|
Mesh File (.re2)¶
Stores the mesh and boundary condition.
TODO: Update to re2
Header¶
The 80 byte ASCI header of the file has the following representation:
#v002 200 3 100 hdr
The header states first how many elements are available in total (200), what dimension is the the problem (here three dimensional), and how many elements are in the fluid mesh (100).
Element data¶
¶ ELEMENT 1 [ 1A] GROUP 0
Face {1,2,3,4}
\(x_{1,\ldots,4}=\) 0.000000E+00 0.171820E+00 0.146403E+00 0.000000E+00 \(y_{1,\ldots,4}=\) 0.190000E+00 0.168202E+00 0.343640E+00 0.380000E+00 \(z_{1,\ldots,4}=\) 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Face {5,6,7,8}
\(x_{5,\ldots,8}=\) 0.000000E+00 0.171820E+00 0.146403E+00 0.000000E+00 \(y_{5,\ldots,8}=\) 0.190000E+00 0.168202E+00 0.343640E+00 0.380000E+00 \(z_{5,\ldots,8}=\) 0.250000E+00 0.250000E+00 0.250000E+00 0.250000E+00 Following the header, all elements are listed. The fluid elements are listed first, followed by all solid elements if present.
The data following the header is formatted as shown in Table 16. This provides all the coordinates of an element for top and bottom faces. The numbering of the vertices is shown in Fig. Fig. 1. The header for each element as in Table 16, i.e.
[1A] GROUP
is reminiscent of older Nek5000 format and does not impact the mesh generation at this stage.
Curved Sides¶
This section describes the curvature of the elements. It is expressed as deformation of the linear elements. Therefore, if no elements are curved (if only linear elements are present) the section remains empty.
The section header may look like this:
640 Curved sides follow IEDGE,IEL,CURVE(I),I=1,5, CCURVECurvature information is provided by edge and element. Therefore up to 12 curvature entries can be present for each element. Only non-trivial curvature data needs to be provided, i.e., edges that correspond to linear elements, since they have no curvature, will have no entry. The formatting for the curvature data is provided in Table 17.
¶ IEDGE
IEL
CURVE(1)
CURVE(2)
CURVE(3)
CURVE(4)
CURVE(5)
CCURVE
9 2 0.125713 -0.992067 0.00000 0.00000 0.00000 m 10 38 0.125713 -0.992067 3.00000 0.00000 0.00000 m 1 40 1.00000 0.000000 0.00000 0.00000 0.00000 C There are several types of possible curvature information represented by
CCURVE
. This include:
- ‘C’ stands for circle and is given by the radius of the circle, in
CURVE(1)
, all other compoentns of theCURVE
array are not used but need to be present.- ‘s’ stands for sphere and is given by the radius and the center of the sphere, thus filling the first 4 components of the
CURVE
array. The fifth component needs to be present but is not utilized.- ‘m’ is given by the coordinates of the midside-node, thus using the first 3 components of the
CURVE
array, and leads to a second order reconstruction of the face. The fourth and fifth components need to be present but are not utilized.Both ‘C’ and ‘s’ types allow for a surface of as high order as the polynomial used in the spectral method, since they have an underlying analytical description, any circle arc can be fully determined by the radius and end points. However for the ‘m’ curved element descriptor the surface can be reconstructed only up to second order. This can be later updated to match the high-order polynomial after the GLL points have been distributed across the boundaries. This is the only general mean to describe curvature currrently in Nek5000 and corresponds to a HEX20 representation.
Boundaries¶
Boundaries are specified for each field in sequence: velocity, temperature and passive scalars. The section header for each field will be as follows (example for the velocity):
***** FLUID BOUNDARY CONDITIONS *****and the data is stored as illustarted in Table 18. For each field boundary conditions are listed for each face of each element.
Boundary conditions are given in order per each element, see Table 18 column
IEL
, and faces listed in ascending order 1-6 in columnIFACE
. Note that the header in Table 18 does not appear in the actual.rea
.The ordering for faces each element is shown in Fig. 4. A total equivalent to \(6N_{field}\) boundary conditions are listed for each field, where \(N_{field}\) is the number of elements for the specific field. \(N_{field}\) is equal to the total number of fluid elements for the velocity and equal to the total number of elements (including solid elements) for temperature. For the passive scalars it will depend on the specific choice, but typically scalars are solved on the temeprature mesh (solid+fluid).
Each BC letter condition is formed by three characters. Common BCs include:
E
- internal boundary condition. No additional information needs to be provided.SYM
- symmetry boundary condition. No additional information needs to be provided.P
- periodic boundary conditions, which indicates that an element face is connected to another element to establish a periodic BC. The connecting element and face need be to specified inCONN-IEL
andCONN-IFACE
.v
- imposed velocity boundary conditions (inlet). The value is specified in the user subroutines. No additional information needs to be provided in the.rea
file.W
- wall boundary condition (no-slip) for the velocity. No additional information needs to be provided.O
- outlet boundary condition (velocity). No additional information needs to be provided.t
- imposed temperature boundary conditions (inlet). The value is specified in the user subroutines. No additional information needs to be provided in the.rea
file.f
- imposed heat flux boundary conditions (temperature). The value is specified in the user subroutines. No additional information needs to be provided in the.rea
file.I
- adiabatic boundary conditions (temeperature). No additional information needs to be provided.Many of the BCs support either a constant specification or a user defined specification which may be an arbitrary function. For example, a constant Dirichlet BC for velocity is specified by
V
, while a user defined BC is specified byv
. This upper/lower-case distinction is used for all cases. There are about 70 different types of boundary conditions in all, including free-surface, moving boundary, heat flux, convective cooling, etc. The above cases are just the most used types.
¶ CBC
IEL
IFACE
CONN-IEL
CONN-IFACE
E 1 1 4.00000 3.00000 0.00000 0.00000 0.00000 ..
..
..
..
..
..
..
..
W 5 3 0.00000 0.00000 0.00000 0.00000 0.00000 ..
..
..
..
..
..
..
..
P 23 5 149.000 6.00000 0.00000 0.00000 0.00000
SIZE¶
SIZE file defines the problem size, i.e.the spatial points at which the solution is to be evaluated within each element, number of elements per processor etc. The SIZE file governs the memory allocation for most of the arrays in Nek5000, with the exception of those required by the C utilities. The basic parameters of interest in SIZE are:
ldim
= 2 or 3. This must be set to 2 for two-dimensional or axisymmetric simulations (the latter only partially supported) or to 3 for three-dimensional simulations.lx1
controls the polynomial order of the solution, \(N =\)lx1
\(-1\).lxd
controls the polynomial order of the (over-)integration/dealiasing. Strictly speaking \({\tt lxd=3 * lx1/2}\) is required but often smaller values are good enough.lx2
=lx1
orlx1-2
and is an approximation order for pressure that determines the formulation for the Navier-Stokes solver (i.e., the choice between the \(\mathbb{P}_N - \mathbb{P}_N\) or \(\mathbb{P}_N - \mathbb{P}_{N-2}\) spectral-element methods).lelg
, an upper bound on the total number of elements in your mesh.lpmax
, a maximum number of processors that can be used (Deprecated as of the latest master branch)lpmin
, a minimum number of processors that can be usedldimt
, an upper bound on a number of auxilary fields to solve (temperature + other scalars, minimum is 1).
The optional upper bounds on parameters in SIZE are (minimum being 1 unless otherwise noted):
lhis
, a maximum history (i.e. monitoring) points.maxobj
, a maximum number of objects.lpert
, a maximum perturbations.toteq
, a maximum number of conserved scalars in CMT (minimum could be 0).nsessmax
, a maximum number of (ensemble-average) sessions.lxo
, a maximum number of points per element for field file output (lxo
\(\geq\)lx1
).lelx
,lely
,lelz
, a maximum number of element in each direction for global tensor product solver and/or dimentions.mxprev
, a maximum dimension of projection space (e.g. 20).lgmres
, a maximum dimension of Krylov space (e.g. 30).lorder
, a maximum order of temporal discretization (minimum is2 see also characteristic/OIFS method).lelt
determines the maximum number of elements per processor (should be not smaller than nelgt/lpmin, e.g. lelg/lpmin+1) (promoted to basic section as of the latest master branch).lx1m
, a polynomial order for mesh solver that should be equal to lx1 in case of ALE and in case of stress-formulation (=1 otherwise).lbelt
determines the maximum number of elements per processor for MHD solver that should be equalt to lelt (=1 otherwise).lpelt
determines the maximum number of elements per processor for linear stability solver that should be equalt to lelt (=1 otherwise).lcvelt
determines the maximum number of elements per processor for CVODE solver that should be equalt to lelt (=1 otherwise).lfdm
equals to 1 for global tensor product solver (that uses fast diagonalization method) being 0 otherwise.
Note that one also need to include the following line to SIZE file:
include 'SIZE.inc'
that defines addional internal parameters.
Mesh Partitioning File (.map/.ma2)¶
TODO: Add more details
Restart/Output files (.f#####)¶
Field files are used to read/write physical fields in both serial and parallel. They have extension .f#####
where # is a numeral. The file format is unique to Nek5000 and is described in this section.
The file is composed of:
- Header
- Global element IDs, coordinates, and field data
- Metadata
The header provides information about the types, sizes, and layout of the field data. The header is a fixed size of 132 bytes. Its data elements are encoded as either ASCII or binary values. In the table below, the offsets and widths are measured in bytes. Note that consecutive entries are separated by a single byte, which is the ASCII space character. Finally, note that the data entries do not require all 132 bytes.
Some elements that require additional explanation are:
nz
: This is the number of GLL gridpoints in the z-direction. If equal to 1, the field data were produced for a 2D simulation. If > 1, the data were produced for a 3D simulation.rdcode
: Specifies the type and ordering of fields that are present in this file. The code can consist of the following. All fields are optional, but if present, they are expected to appear in this order.X
: CoordinatesU
: VelocityP
: PressureT
: TemperatureS#
: Passive scalar(s). # is a numeral that specifies the number of different passive scalars.
test value
: When Nek5000 writes the header to file, it writes the specific value 6.54321 as a test value. When the file is later read – possibly on a different computer – the test value is read and compared to the expected value. If the values match, then the computer that wrote the file and the computer that is now reading the file use the same endianness for floating-point numbers. If not, the computers have different endianness. In that case, the floating-point data should be byte-swapped by the computer reading the data.
Name | Offset | Width | Encoding | Datatype | Description |
---|---|---|---|---|---|
tag |
0 | 4 | ASCII | text | The string #std . Tags the start of the fil |
wdsize |
5 | 1 | ASCII | integer | Floating-point precision of field data (in bytes) |
nx |
7 | 2 | ASCII | integer | Number of GLL points per element in x direction |
ny |
10 | 2 | ASCII | integer | Number of GLL points per element in y direction |
nz |
13 | 2 | ASCII | integer | Number of GLL points per element in z direction |
nelt |
16 | 10 | ASCII | integer | Number of elements in this file |
nelgt |
27 | 10 | ASCII | integer | Number of global elements |
time |
38 | 20 | ASCII | decimal | Absolute simulation time of this file’s state |
iostep |
59 | 9 | ASCII | integer | I/O timestep of this file’s state |
fid |
69 | 6 | ASCII | integer | Index of this file (when using multi-file output) |
nfileoo |
76 | 6 | ASCII | integer | Number of files produced at this I/O step |
rdcode |
83 | 10 | ASCII | text | Specifies which fields contained in this file |
p0th |
94 | 15 | ASCII | decimal | Thermodynamic pressure |
if_press_mesh |
110 | 1 | ASCII | text | States whether pressure mesh is being used |
test_value |
112 | 4 | binary | 32-bit float | The decimal 6.54321. Used to test endianness. |
The global element IDs, coordinates, and field data start at offset 136 bytes. Integer data are always 32-bit.
The precision of floating-point data is inferred from the value of wdsize
(see above). The number of
dimensions (ndims
) is inferred from nz
(see above). The global element IDs are required, but the
coordinates and any field data are optional. Their presence of coordinates and field data are inferred from
rdcode
, as described above.
Value | Datatype | Shape |
---|---|---|
Global element IDs | integer | (nelt) |
Coordinates | float | (nelt, ndims, nx * ny * nz) |
Velocity | float | (nelt, ndims, nx * ny * nz) |
Pressure | float | (nelt, nx * ny * nz) |
Temperature | float | (nelt, nx * ny * nz) |
Passive scalars | float | (nscalars, nelt, nx * ny * nz) |
TODO: Describe metadata