
3D Electromagnetics, powered by Palace
The cylinder_cavity_impedance example is an eigenmode analysis of a dielectric-filled cylindrical cavity whose walls carry a finite surface impedance, modeling real copper conductor loss. Unlike the ideal-wall cylinder_cavity_pec, this variant yields complex eigenfrequencies and finite quality factors Q for realistic loss budgeting.
- Impedance boundary condition — the tangential fields on the walls are linked through a surface resistance Rs, so wall dissipation enters the mode and ωn becomes complex
- Quality factor follows directly as Q = Re(ω)/(2·Im(ω)), separating dielectric and conductor loss contributions
- Order-4 elements on a prism mesh, with Rs = 0.0184 Ω representing copper at ~5 GHz
- Problem type: Eigenmode, prism mesh, length unit L0 = 1 cm
- Material: dielectric fill, εr = 2.08, μr = 1.0, loss tangent 0.0004
- Boundaries: cavity walls + end caps = Impedance, Rs = 0.0184 Ω (Cu @ 5 GHz)
- Eigensolver: 15 eigenpairs, target 2.0 GHz, tolerance 1e-8 → complex ω and Q
- Inner solve: GMRES + multigrid preconditioner, GPU device (order 4)
The core transferable physics: real resonators lose energy to conductor and dielectric loss, and that loss sets the quality factor Q — the single number governing filter insertion loss, oscillator phase noise, and sensor resolution. Modeling walls with a surface impedance turns an idealized eigenproblem into a realistic loss budget.
The impedance boundary makes ω complex, so Q comes straight out of the eigensolve rather than a lossy post-processing estimate.
Comparing against the PEC baseline isolates conductor loss from dielectric loss, so you know which to attack.
Swap the surface resistance for silver, gold-plate, or superconductor to compare finish options on Q and cost.
Predicting Q before build replaces the measure-and-hope loop with a targeted design that meets loss spec on the first article.
Select a domain to see how this simulation applies, with industry-specific scenarios and ROI.
A cavity filter's insertion loss and selectivity are governed by the unloaded quality factor Q of its resonators. Q is set by conductor loss (wall material and finish), dielectric loss, and geometry. Designers who cannot predict Q accurately over-design — using bigger cavities, exotic plating, or more resonators than needed — adding cost, size, and weight.
Under-designing is worse: a filter that misses its insertion-loss spec fails acceptance and forces a re-plate or re-machine, each costing thousands and weeks of schedule.
Impedance-wall eigenmode analysis predicts Q for a given material and finish, right-sizing the design for the loss budget.
| Application | How this simulation maps |
|---|---|
| Filter insertion-loss budget | Q from complex ω predicts per-resonator loss and total insertion loss |
| Plating / finish trade-off | Rs for Cu vs Ag vs Au plate compares Q gain against plating cost |
| Size / weight optimization | Q vs cavity size right-sizes hardware to meet loss with minimum volume |
Scenario: A filter maker over-plates with silver on 100% of parts to guarantee Q. Q-prediction shows copper suffices on 60% of designs, and cuts insertion-loss acceptance failures from 12% to 3%.
Right-sized cavities also cut material and machining time on every unit shipped, compounding the savings at volume.
Set your wall material
Enter the surface resistance for your conductor/finish and run the eigensolve to get complex ω and Q.
Sweep finish and geometry
Compare plating options and cavity sizes to hit the target Q at minimum cost, weight, or size.
Compare to the ideal
Benchmark against cylinder_cavity_pec to separate conductor from dielectric loss and target the dominant term.
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