Corrugated Waveguide Low-Pass Filter
(quasi-periodic structure design method)

By R. Goulouev, Sept. 2020

Contents

About this Tool
Regular Corrugated Filters
Iregular Corrugated Filters
Composite Corrugated Filters
Design Method
Getting Started
Related Information Sources

About this Tool

This tool is designed to synthesize a preliminary (a "good starting point") design concept of a low-pass filter based on an E-plane corrugated and generally inhomogeneous [1] waveguide. Corrugated low-pass filters are in great demand in modern microwave technology and many engineering papers, reports and patents have been recently published (see selected references [1-13]). For a beginner designer, for a start, it is advised to look through some of these works to find out about ​​the theoretical and practical foundations. All corrugated waveguide filters researched in referenced papers are divided here in three categories (listed in next paragraphs). This design tool can be applied (directly or indirectly) to all three types of waveguide structures, but the design method used here, however, may differ from the original sources.

Regular Corrugated Filters

These are the filters with a constant width of the waveguide channel [2,3,6,8-12]. Such filters suffer from the presence of spurious pass-bands (responses) [1] corresponding to propagation of higher order waveguide modes of TEN0 origin (where N>1). Nevertheless, the regular corrugated filters can be very efficiently used as harmonic (up to 17 harmonics claimed in [10]) reject filters. In other words, these filters can be preferably used to reject a sparse frequency-scattered spurious interference (for example, harmonics of a transmitter or amplifier). The obvious their advantages are the simplicity, reliability and accuracy. Before you start designing with this tool, try the "Corrugated Low-pass Filter Design Workshop", which was designed to create a simple "cost-effective" harmonic-reject filter of this type. Plus, all design steps (spurious layouts, initial synthesis, simulation, optimization, and sensitivity analysis) perform much faster there. On the contrary, it is advised to use this tool only for more complex designs, which require more flexibility in profiling the corrugations.

Iregular Corrugated Filters

These are the filters with the width of the waveguide channel not being constant, but smoothly changing (tapered way) along its length. Such filters are called here as "irregular" ("inhomogeneous" in [1]). The reason for tapering the channel width is that it significantly narrows the spurious responses. Here, the designer is advised to smoothly expand the channel width from a minimal dimension (A min) at one end to a maximal dimension (A max) at the other end. The dimension (A min) should be slightly greater than the half the wavelength corresponding to the lower frequency bound of the targetted pass-band and the dimension (A max) should be slightly less than the full wavelength corresponding to the upper bound of the targetted pass-band. This channel width range ensures that the pass-band is above the dominant mode (TE10) cut-off and below the first spurious mode (TE 20) cut-off.

Composite Corrugated Filters

These filters are composed from sections (sub-filters), which are based on regular corrugated channels [4,5,7]. Those sub-filters cover the same pass-band for the dominant mode TE10-mode and have different layouts of pass-bands corresponding to spurious TEN0-modes (N>1). Such filters, as claimed in [4,5]), can be designed to completely stop all spurious transmission and perform better than waffle-iron filters. But in this case, the designer actually needs to design two filters (not necessarily finalized) and connect them to each other (after removing the extra sections of transformers).

Design Method

The proposed method for designing a waveguide corrugated filter is based on matching a "slightly" aperiodic corrugated structure of the waveguide channel with the input and output interfaces at a single frequency point (center frequency) [4]. In this case, the corrugated waveguide is represented as an ideal transmission line, but with impedance smoothly varying along the length. Then, such a line is matched to the input and output interface with appropriate quarter-wave transformers at the specified center frequency. Thus, matching with good return loss typically only occurs in a narrow bandwidth and degrades away from the center frequency. Nevertheless, such synthesis method usually leads to a good starting filter concept and can be further easily optimized to meet users preferences. However, prior to optimization, the user is advised to perform a full modal analysis to ensure that the preliminary design concept does not suffer from spurious responses and meets the specified rejection goals with adequate margins.

Getting Started

This tool can be directly used (in a straight forward way) to design the first two types of corrugated waveguide filter (regular and iregular). It is also can be used to design a composite corrugated waveguide filter, consisting from parts such as filters of two first types. In that case, however, the user is expected to do some additional work on composing the filter from the parts (using structure editor) and matching them with each other and I/O interface (more optimization would be required). Anyway, in all cases, the starting procedure is as follows:

  1. Select the I/O waveguide (EIA standard) interface in the top row of table and click "Set Initials" button. This will derive some initials for the internal corrugated waveguide channel and its profile. Those initial settings are based on a common sense guess and can be changed later. The user can also set those parameters manually.
  2. Correct or set the centrer frequency in the second row.
  3. Correct or set the proper ("non-spurious") width of corrugations in case of a regular corrugated filter or their range of tapering in case of iregular corrugated filter. Those A-dimensions (first numbers in the input fields located in 4th and 5th table rows) effect the layout of the spurious.
  4. In a similar manner, set the vertical profile of the corrugated channel, i.e. the B-dimensions for the irises and cavities forming aperiodic and tapered corrugated waveguide on E-plane. It is suggested, that the larger corrugations work for the lower frequencies and, vice versa, the smaller corrugations are more efficient at higher frequencies. In a rough interpretation, we need spread their efficiency bands across the entire cutoff range with no gaps left.
  5. The third number (iris thickness or cavity length) in each text field (in 4th and 5th table rows) can be left same or also be variable. It is generally recommended to keep the iris thickness as thin as technologically acceptable. The cavity length, however, should be reasonably great to achieve a good loaded Q.
  6. Set the number of corrugations or keep the default value.
  7. Set the "Profile Factor" or keep the default value. This factor defines how the appropriate dimensions of corrugations are distributed over the waveguide channel. For example, a harmonic filter designed to reject 2nd and 3rd harmonics should have more smaller corrugations than the one intended to reject just the 2nd harmonics (appropriate guessed values of this parameter can be 1-1.5 and 1.5-2.5).
  8. Click "Setup Project" button (in case if the project has not been set yet). This action will automatically set initial project settings with a frequency sweep as the interface waveguide operational frequency range (as EIA standard). It is required at least once to set the frequency plans, but it can be changed or modified on the "Setup Page". If the project is already set, clicking "Setup Project" could not be required as it would overwrite the settings.
  9. Click "Design Filter" button. The action will generate the filter connectivity schematic, initial dimensions and navigate to the Editor Page with design and simulation tools.
  10. Finalize the design in the "Editor Page":
    1) Verify if the initially generated structure has a right frequency layout. I.e. the targetted pass-band is located where the return loss is most higher and the roll-off is giving adequate rejection in upper near-band (if required).
    2) Run some other waveguide modes also. Make sure that spurious pass-bands are out of targetted stop-band specs.
    3) Make necessary adjustments to fit the pass-band, stop-band and spurious if needed. To do so, try different corrugations dimensions at the ends and the middle (4th and 5th rows of table).
    4) Optimize (when finalizing) the in-band performance using optimization tool. Optimization targets must be set (Setup page) prior to optimization.

Related Information Sources

[1] R. Levy, "Inhomogeneous stepped-impedance corrugated waveguide low-pass filters," in IEEE MTT-S Int. Microw. Symp. Dig., Jun. 2005, pp. 123–126.

[2] S.B. Conh "A theoretical and experimental study of a waveguide filter structure", Office Naval Res., Cruft Lab., Harvard Univ., Cambridge, Mass., Rep. 39, Apr. 25, 1948.

[3] R. Levy, “Tapered corrugated waveguide low-pass filter,” IEEE Trans . Microwave Theory Tech., vol. MTT-21, pp. 526–532, August 1973.

[4] R. Goulouev, "New Type of Spruriosless Waveguide Harmonic Filter," manuscript, 2004. Available here

[5] F. De Paolis, R. Goulouev, J. Zheng, and M. Yu, "CAD procedure for high-performance composite corrugated filters," IEEE Trans. Microw. Theory. Techn., vol. 61, no. 9, pp. 3216–3224, Sept. 2013.

[6] W. Hauth, R. Keller, and U. Rosenberg, “CAD of waveguide low-pass filters for satellite applications,” in Proc. 17th Eur. Microw. Conf., Rome, Italy, 1987, pp. 151–156.

[7] W. Hauth, R. Keller, U. Rosenberg, "The Corrugated-Waveguide Band-Pass Filter - A New Type of Waveguide Filter", 18th EUMC Proc., Stockholm, 1988, pp. 945-949.

[8] O. Ishida, H. Maruf, "Expansion of a Continuous Stop Band of a Corrugated Waveguide by Attenuation Pole Control," Proceedings of APMC 2012, Kaohsiung, Taiwan, Dec. 4-7, 2012.

[9] R. Goulouev, “Corrugated Waveguide Filter Having Coupled Resonator Cavities”, US Patent 6,169,466, Jan. 2001. Available here

[10] R. Goulouev, D. Garcia, Q. Shi, C. McLaren, "Powerful Multiple Harmonics Reject Filter Design, Testing and Acceptance Considering Ultra Overmoded Waveguide Conditions," 5th Workshop on Advanced RF Sensors and Remote Sensing Instruments, ESA/ESTEC, ARSI’17, vol. 1, Noordwijk, Netherlands, 2017. Available here

[11] O. Monerris, P. Soto, S. Cogollos, V. E. Boria, J. Gil, C. Vicente, and B. Gimeno, "Accurate circuit synthesis of low-pass corrugated waveguide filters," in Microwave Conference (EuMC), 2010 European, 2010, pp. 1237-1240.

[12] I. Arregui, I. Arnedo, A. Lujambio, M. Chudzik, D. Benito, R. Jost, F. -1. Gortz, T. Lopetegi, and M. A. G. Laso, "A compact design of high-power spurious-free low-pass waveguide fiters," IEEE Microw. Wireless Compon.Lett., vol. 20, no. 11, pp. 595- 597, Nov. 2010.

[13] F. Teberio, I. Arregui, A. Gomez-Torrent, I. Arnedo, M. Chudzik, M. Zedler, F.-J. Gortz, R. Jost, T. Lopetegi, and M. A. G. Laso, "Chirping Techniques to Maximize the Power-Handling Capability of Harmonic Waveguide Low-Pass Filters," IEEE MTT, v. 64, No. 9, Sept. 2016, pp. 2814-2823.


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