The INTEGRATED Advantage

High Frequency Solutions

  • Solution to an Electromagnetic(EM) model can be obtained in SINGULA based on the Method of Moments(MoM) or Finite Element Method, or the hybrid method with MoM and Physical Optics (PO).
  • SINGULA can solve electrically-large-size problems by the Fast Fourier Transform (FFT) technique or the hybrid method with MoM and PO.

  • SINGULA’s FFT technique can deal with the model with the high lossy materials, which Multi-level Fast Multi-pole Method could not deal with.

  • SINGULA can solve the full-matrix problem with over half a million unknowns on a PC computer.

  • Simultaneous use of lossless and lossy electrical materials in a model is permitted in SINGULA , whereas restrictions in some form exist in competing programs.

  • Waveguide sources can be used in the open or in the closed region problems.

  • Radiation patterns of antennas fed by waveguides surrounded by dielectric radomes can accurately be obtained in SINGULA.

  • Solution convergence with increased mesh density is easily accomplished in SINGULA . This increases the confidence on the arrived solution.

  • SINGULA can be coupled with LORENTZ or CELSIUS for particle trajectory calculation or thermal analysis.

  • The team of Engineers that are responsible for the development of SINGULA offer design and technical support to the users of SINGULA throughout.

Maximum Versatility of Field Solvers

BEM, FEM or Hybrid; Choose the Right Tool for Your Application

Since 1984, INTEGRATED has been the industry leader in Boundary Element Method (BEM) CAE software. BEM not only provides the most accurate numerical field solutions, but also is the method of choice for problems involving large open regions.

In contrast, field solvers using the Finite Element Method (FEM) often require artificial "smoothing" algorithms to average out numerical errors. In addition, artificial boundaries must be used to handle open region problems, and even then, the large meshes required may lead to excessively long solution times.

However, the relative simplicity of implementation of FEM solvers leads to advantages when complex nonlinear or transient analysis is required. FEM very often provides sufficient accuracy for engineering purposes, and many problems are by their nature inherently closed region. Recognizing this, INTEGRATED incorporated FEM solvers to provide users the choice of both methods. A significant side benefit of having both BEM and FEM solvers is the ability to check the validity of solutions using two completely different analysis methods.

The most challenging analysis problems occur when both nonlinearities and open regions are present. Here again INTEGRATED takes the lead providing HYBRID field solutions using BEM and FEM simultaneously to exploit the strengths of both methods.

More Benefits

- Link to CAD packages for true representation of complex geometric shapes

- Powerful parametric solvers allow designers to automatically vary and experiment with geometry, materials and sources – reducing the tedious, repetitive task of fine –tuning multiple design parameters

- Easy-to-learn programs allow designers to focus on product development, not software training

 

Beam Optics & Charged Particle Trajectory Analysis

The LORENTZ module for charged particle calculations is available with any INTEGRATED field solvers or combination thereof. Advantages of LORENTZ include:

Best Field Solver

No single method is the fastest or most accurate for every problem. However, accurate field results are a critical start to getting correct trajectory calculations. INTEGRATED field solvers have been proven in a diverse range of applications for over 20 years. BEM, FEM, and a HYBRID solvers are available to give the user a high level of choice. This also provides the ability to independently verify the solution within the same program, with much less effort than using two separate programs for verification. The BEM method is especially noted for producing more accurate field results than FEM in most cases.

Mixed Fields

In many applications it is necessary to use more than one field type, for example, a magnetic field from coils plus electric fields from electrodes, or high frequency fields in a waveguide plus a DC bias field. LORENTZ can have more than one field solver built in to handle these cases. Furthermore, LORENTZ is able to import fields (see below).

Importing Fields

Users often want to specify a field rather than model it. Reasons include:

1. making use of measured fields from the actual equipment

2. theoretical studies of the effect of field shape to determine whether it is worth designing equipment to achieve that field shape

3. making use of pre-existing results from software purchased prior to LORENTZ

The interface for importing includes a simple text file format to interpolate from the input data, and (for more advanced users) a DLL link.

Secondary Emission

LORENTZ provides two options for Secondary Emission calculations. Probabilities are determined from the energy of peak gain, the gain at this energy, and the mean energy of the secondary electrons.

A variety of inputs specify the individual probablities for reflection, rediffused electrons, and "true secondaries".

Space Charge and Surface Charge

All variants of LORENTZ with a static electric solver module included are able to model space charge with a variety of standard emission regimes. In 2D programs it is also possible to model the charging of dielectric surfaces. This includes the charge difference between the incident beam and any secondary electrons emitted.

Mobility, Viscosity, Wind Tunnels, and Residual Gas

LORENTZ is able to model any particle trajectory with electric mobility, and macroparticles with either mobility or viscosity. In both cases a wind speed can be applied to "Wind Tunnel" regions of the model. Advanced users with external data for a wind tunnel velocity distribution can import this via a DLL that they write. Residual gases provide random changes to particle momentum based statistically on the mass, radius, temperature and pressure of the gas molecules.

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