|
sin(w×t)
(w×t) |
In the time-domain, sinc(w×t)
looks like this, a sine wave gradually increasing to its maximum amplitude,
then decreasing to zero.
This is a sinc waveform with a the Sinc Frequency parameter set to 1 GHz,
and Sinc Modulation set to zero.
This is the same sinc waveform, but now with Sinc Modulation set to 10 GHz,
modulating the sinc by a 10 GHz sine wave.
The extent of the leading and trailing tails is controlled by the sigma
parameters, like the Gaussian pulse waveforms.
Rise Sigma controls the length of the increasing half,
while Fall Sigma
controls the length of the decreasing half.
The modulated sinc waveform has a well-defined bandwidth, as show by this
frequency-domain plot of the same waveform show above.
This is the attractive attribute of the modulated sinc.
The smoothness of the frequency-domain curve is controlled by the
sigma parameters, a large value giving a smoother curve but
taking a longer simulation time.
This output option is for users who wish to create their own post-processing
routines for the far field data.
Currently, LC has no capability for reading or processing the saved grid face data.
Documentation for the face data format is available.
OpenMP directives for parallel execution have been added to LC.
OpenMP
is a new high-performance parallel execution scheme for
shared-memory multiprocessor computers.
The main grid field update, the first order Mur ABC, and the PML ABC,
along with the associated initialization steps,
can use multiple processors in parallel.
The above chart shows the ideal speedup (i.e., 2 times faster on 2 processors)
and the actual speedup with the OpenMP version of LC running a sample problem.
Currently, models run with the PML ABC is showing slightly less speedup
than the Mur ABC, but more PML activity is in the works.
The OpenMP version of LC is not included in the regular distribution.
The default version of LC 2.8 will still use the
older (and somewhat less efficient) parallel directives.
If you'd like to try out the OpenMP version, you can
contact me.
Far Field Grid Face Data
New output options have been added to the Define Far Field Sweeps dialog to
save the full two-dimensional grid face far field data.
Using these options, both the accumulated tangential electric and magnetic field
values can be saved for every grid point on the calculation surfaces.
The magnitude and phase values can be written as well as real and imaginary
components. The magnitude and phase values are normalized to the source,
if far field normalization has been configured.
Improved Parallel Performance
Other Changes and Bug Fixes
Return to What's New
Copyright © Cray Inc.
Maintained by Kevin Thomas (kjt@cray.com).
Last modified
Wed Mar 24 14:18:43 CST 1999