The Eigenvalue (

) study and study step are used to compute the eigenvalues and eigenmodes of a linear or linearized model in a generic eigenvalue formulation where the eigenvalues are not necessarily frequencies. The Eigenvalue study gives you full control of the eigenvalue formulation, in contrast to the eigenfrequency study that is adapted for specific physics interfaces. The Eigenvalue study is typically used for equation-based modeling.
From the Eigenvalue solver list, choose
ARPACK (the default),
FEAST,
LAPACK (filled matrix), or
ARPACK nonlinear:
From the Eigenvalue search method list, select a search method:
From the Unit list, choose a suitable unit (default rad/s).
Use the Search method around shift list to control how the eigenvalue solver searches for eigenvalues around the specified shift value:
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Select Closest in absolute value (the default value) to search for eigenvalues that are closest to the shift value when measuring the distance as an absolute value.
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Select Larger real part to search for eigenvalues with a larger real part than the shift value.
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Select Smaller real part to search for eigenvalues with a smaller real part than the shift value.
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Select Larger imaginary part to search for eigenvalues with a larger imaginary part than the shift value.
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Select Smaller imaginary part to search for eigenvalues with a smaller imaginary part than the shift value.
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Use the Approximate number of eigenvalues field to specify the approximate number of eigenvalues you want the solver to return (default: 20). The value of the
Approximate number of eigenvalues will affect the
Dimension of Krylov space used by the algorithm; see the
Advanced section of the
Eigenvalue Solver. It means that increasing the value of the
Approximate number of eigenvalues will increase the memory requirement and the computational time. If the solver indicates that the value of the
Approximate number of eigenvalues is smaller than the actual number of eigenvalues in the given region, it will perform a search for more eigenvalues, which increases the computational time; see
The Eigenvalue Region Algorithm. Within limits it is often more efficient to provide a too large value of
Approximate number of eigenvalues than a too small.
In the Maximum number of eigenvalues field, you can specify a maximum number of eigenvalues to limit the eigenvalue solver’s search for additional eigenvalues (default: 200).
Under Rectangle search region, you define the size of the search region for eigenvalues as a rectangle in the complex plane by specifying the
Smallest real part,
Largest real part,
Smallest imaginary part, and
Largest imaginary part in the respective text fields. The search region also works as an interval method if the
Smallest imaginary part and
Largest imaginary part are equal; the eigenvalue solver then only considers the real axis and vice versa.
The Perform consistency check checkbox is available and selected by default to increase confidence that the solver finds all eigenvalues in the search region. The work required for performing the consistency check constitutes a significant part of the total work of the eigenvalue computation
Eigenvalue computations can be performed with a nonsymmetric solver or, if applicable, a real symmetric solver. From the Use real symmetric eigenvalue solver list, choose
Automatic (the default) or
Off. For the
Automatic option there is the option to select the
Real symmetric eigenvalue solver consistency check checkbox. This consistency check increases the computational time and memory requirements but provides a rigorous check of the applicability of the real symmetric solver.
Use the Taylor expansion truncation list to specify in which way to truncate the Taylor expansion in order to approximate the nonlinear dependence in
λ with a polynomial. There are two options:
Tolerance and
Fixed truncation.
With the Tolerance option, specifying a
Maximum degree of the Taylor expansion (default: 5), all the latest Taylor coefficients that are smaller then the specified
Tolerance (default: 1·e
−12) will be disregarded.
With the Fixed truncation option, the number of Taylor coefficients to keep is specified in
Degree of the Taylor expansion (default: 3), and no further approximation is performed.
From the Eigenvalue search method list, select a search method:
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Ellipse (the default), to define an eigenvalue search contour as an ellipse in a complex plane. See Ellipse Search Region settings below.
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Half ellipse (Hermitian problem), to define an eigenvalue search contour by half of the whole ellipse. See Half Ellipse Search Region below.
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For an eigenvalue problem for which you know how many eigenvalues there are, the solver can compute the eigenvalues directly. For that case, choose Manual from the
Number of eigenvalues list and enter the desired number of eigenvalues in the
Approximate number of eigenvalues field. If you do not know the number of eigenvalues in the defined region, there are two cases: You can just estimate the number of eigenvalues without computing them, or you can let the software estimate the number of eigenvalues and then compute them automatically afterward. The former is achieved by clicking the
Stochastic Estimation button (

) at the top right of the
Study Settings section. The latter is achieved by choosing
Stochastic estimation from the
Number of eigenvalues list, and then click
Compute. Both cases require doing stochastic estimation, which needs the setting of an
Approximate number of eigenvalues field as an initial guess in the estimation stage.
There is an option to select the Store linear system factorization checkbox. If selected, linear system factorizations are stored from the first FEAST iteration and reused in later iterations.
If the Study >
Batch and Cluster checkbox is selected in the
Show More Options dialog, select the
Distribute linear system solution checkbox to run the FEAST eigenvalue solver in parallel. See
Running FEAST in a Parallel MPI Mode for more information.
From the Unit list, choose a suitable unit (default rad/s).
You define the Ellipse by specifying the
Center,
Real semiaxis,
Imaginary semiaxis, and
Rotation angle in the respective text fields. It is important that the real semiaxis that you specify in the
Real semiaxis field is large enough to enclose the eigenvalues of interest. In the
Imaginary semiaxis field, you specify the imaginary semiaxis in a similar way. In the
Rotation angle field, specify the rotation angle in degrees from the vertical axis in the range of
−180 degrees to 180 degrees.
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The Stochastic Estimation works as a Compute to Selected step. Because the Stochastic Estimation action does not solve the eigenvalue problem, there will not be any valid solution from this action. So, if the Stochastic Estimation action is done for a single step or the first step in a multistep study, there will not be any solution that can be used for postprocessing and results analysis. If the action is done for a step after the first step in a multistep study, the main solution of the sequence corresponds to the study step right before the eigenstep for which the estimation is done.
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You define the Half ellipse (Hermitian problem) by specifying the
Smallest real part,
Largest real part, and
Imaginary semiaxis in the respective text fields.
For the Ellipse eigenvalue search method, eigenvalue computations can be performed with a nonsymmetric solver or, if applicable, a real symmetric solver. From the
Use real symmetric or Hermitian eigenvalue solver list, choose
Automatic (the default) or
Off. For the
Automatic option there is the option to select the
Real symmetric or Hermitian eigenvalue solver consistency check checkbox. This consistency check increases the computational time and memory requirements but provides a rigorous check of the applicability of the real symmetric solver.
To specify a shift to use in the modes computation, select the Shift used in the modes computation checkbox and then enter a shift (in rad/s) in the associated text field.
In the Maximum matrix size field, enter an upper limit on the matrix size (default: 2000).
From the Unit list, choose a suitable unit (default: rad/s).
From the Settings list, choose
Physics controlled (the default) to use linearization point settings controlled by the physics interfaces. Choose
User defined to specify the linearization point using the
Method list. Select:
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Initial expression to use the expressions specified on the Initial Values nodes under a specific physics interface as a linearization point.
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Solution to use a solution as a linearization point.
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Use the Study list to specify which solution to use from the available studies. Select:
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Zero solution to use a linearization point that is identically equal to zero.
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The eigenvalues can be excluded if there is a filter expression that they do not satisfy. In the table below, in the Filter expression (store if true or >0) column, add expressions for the filtering Those expressions can be functions of the eigenvalue
lambda or eigenfrequency
freq and can be logical expressions such as
lambda>10. If desired, add some descriptive text in the
Description column for the expressions.
The Store solutions list is always available: Choose
All converged solutions (the default) or
First Nth for the first
Nth solutions. Then specify that number in the
Maximum number of stored solutions field (default: 1000).
The eigenvalues can be sorted in Ascending (the default) or
Descending order depending on the
Ordering setting. When the
Sorting method is
Predefined, you can choose to
Sort primarily based on the
Real part,
Imaginary part,
Real part magnitude,
Imaginary part magnitude, or
Absolute value. The same settings are available for the
Sort secondly option, which is used to resolve conflicts. The defaults for eigenvalues are
Real part for
Sort primarily and
Imaginary part magnitude for
Sort secondly. For eigenfrequencies, the defaults are
Imaginary part for
Sort primarily and
Imaginary part magnitude for
Sort secondly. Also, the
Sort based on transformed eigenvalues checkbox is selected by default to take and eigenvalue transformation into account when sorting.
Alternatively, Manual can be chosen for the
Sorting method and then an arbitrary number of (ordered) custom sorting priority expressions can be defined in the table that appears. In the
Sorting priority expression column, add expressions for the sorting, in order of priority. Those expressions can be functions of the eigenvalue
lambda or eigenfrequency
freq. For example, you can specify an expression such as
abs(freq-1) to sort according to the distance from a given shift (1 in this case). If desired, add some descriptive text in the
Description column for the expressions.
The Conjugate-pair consecutive sort checkbox is selected by default to make sure that complex-conjugate eigenpairs appear one after the other, regardless of the sorting rules.
If you have selected ARPACK as the
Eigenvalue solver and selected the
Auxiliary sweep checkbox, these additional settings are available:
From the ARPACK starting vector list, choose
Default, giving a random starting vector, or
From previous eigenvectors. If you chose
From previous eigenvectors, a
From previous eigenvectors list appears, where you can choose
Summation of all eigenvectors (the default) or
Eigenvector with eigenvalue closest to the shift as the new starting vector. These options can always be used without compromising the convergence. Use
Summation of all eigenvectors when more than one eigenpair is requested. Use
Eigenvector with eigenvalue closest to the shift when only one eigenpair is requested.
From the ARPACK shift list, choose
As specified (the default) or
Based on eigenvalues for last parameter. If you chose
Based on eigenvalues for last parameter, also choose an option from the
From previous eigenvalues list that appears: Choose
Average of converged eigenvalues (the default) or
Eigenvalue closest to the previous shift. In the case where the eigenvalue shift value has not been parameterized, these options could be useful, but use them only if the eigenvalues are expected to have a small variation between two consecutive parameters. If this is not the case, ARPACK may converge to unwanted eigenpairs. Use
Average of converged eigenvalues when the wanted eigenvalues are “around” the shift. More precisely, when the shift is an “internal point” of the convex hull of the wanted eigenvalues. Use
Eigenvalue closest to previous shift if the shift is an “external point” of the convex hull of the wanted eigenvalues. For example, if the eigenvalues are known to have positive real part and the shift is set to zero.
The shift corresponds to the value of the Search for eigenvalues around field in the
Study Settings section. The eigenpairs, computed with respect to the previous parameter, are ordered from the closest to the shift to the one farthest from the shift.
If you are running an auxiliary sweep and want to distribute it by sending one parameter value to each compute node, select the Distribute parametric solver checkbox. To enable this option, click the
Show More Options button (

) and select
Batch and Cluster in the
Show More Options dialog.