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Sonnet User's Guide - Sonnet Software

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<strong>Sonnet</strong> User’s <strong>Guide</strong><br />

When we vary the number of cells per wavelength, along the length of the line, we<br />

see an inverse square relationship. Double the number of cells per wavelength<br />

along the length of the line and the percent error decreases by a factor of four.<br />

An equation which expresses the error as a function of subsectioning is:<br />

16<br />

E T ≅ ------- + 2 ⎛------<br />

16 ⎞ 2<br />

N<br />

N ⎝ W<br />

N ⎠ W ≥ 3 N L ≥ 16<br />

L<br />

where<br />

N W = Number of cells per line width,<br />

N L = Number of cells per wavelength along line<br />

length,<br />

E T = Total Error (DMAC) (%).<br />

This equation estimates subsectioning error only. For example, any de-embedding<br />

errors are added to the above error. This error estimate should be valid for any<br />

electromagnetic analysis which uses roof-top subsectioning.<br />

Notice that the quantities used for the error estimate are in terms of cells, not subsections.<br />

Cells are the smallest possible subsections size. In <strong>Sonnet</strong>, subsections<br />

in the corners of polygons are one cell on a side. Subsections along the edge of<br />

polygons are one cell wide and can be many cells long. Interior subsections can<br />

be many cells in both dimensions.<br />

We have found that, for most cases, the cell size is the important parameter in determining<br />

error. Or in other words, the smallest subsection size is important. For<br />

example, the stripline benchmark geometry projects, mentioned before, are set to<br />

make the lines 16 cells wide, even though those 16 cells may be merged into only<br />

4 or 5 subsections. It is the 16 cells which determine the level of error, not the 4<br />

or 5 subsections.<br />

In performing this error evaluation, we also found that the error in characteristic<br />

impedance due to N W is always high, never low. Also, there is very little variation<br />

in the error for different impedance lines. The above equation can be very accurate<br />

in evaluating error. And, finally, for N L above about 40 cells per wavelength, all<br />

the error is in the characteristic impedance. The error in velocity of propagation is<br />

essentially zero.<br />

The above equation can be very accurate in evaluating error. With this precise<br />

knowledge of the error, we can now do something about it.<br />

342

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