This has turned out to be a bit of a steep hill and I have learned some new things, one of which I wanted to share in this post - a good place to turn for getting poles and zeros or corner frequencies, Qs and zero frequencies for an Elliptic filter having specifications of my choosing. I found two very good references for this information: 1 a book of Elliptic Filter Tables, very well presented: "Handbook of tables for elliptic-function filters" By Kendall L. The program is available at the web page link given above, and there is a nice overview of it shown there. This should make designing and building elliptic filters and crossovers a snap!
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He came from a long line of academics. His early grammar school gymnasium was the Kaiserin Augusta Gymnasium , an institution founded by his great-grandfather, Ludwig Cauer. This school was located on Cauerstrasse, named after Ludwig, in the Charlottenburg district of Berlin. Cauer became interested in mathematics at the age of thirteen and continued to demonstrate that he was academically inclined as he grew.
He married Karoline Cauer a relation  in and eventually fathered six children. For reasons that are not clear, he changed his field after this to electrical engineering. He graduated in applied physics in from the Technical University of Berlin. He also worked on timer relays.
He had two telecommunications-related publications during this period on "Telephone switching systems" and "Losses of real inductors".
Bell were at the forefront of filter design at this time with the likes of George Campbell in Boston and Otto Zobel in New York making major contributions.
Foster that Cauer had much correspondence and it was his work that Cauer recognised as being of such importance. His paper, A reactance theorem,  is a milestone in filter theory and inspired Cauer to generalise this approach into what has now become the field of network synthesis. In he obtained his habilitation and became an external university lecturer.
He worked with Vannevar Bush who was building machines for the solution of mathematical problems. Essentially, these were what we would now call analogue computers : Cauer was interested in using them to solve linear systems to aid in filter designs.
His work on Filter circuits [b] was completed in while still in the US. However, he was unable to obtain funding due to the depression. According to Rainer Pauli, his correspondence with them was usually brief and business-like, rarely, if ever, discussing issues in depth. By contrast, his correspondence with his American and European acquaintances was warm, technically deep and often included personal family news and greetings.
The anti-Jewish hysteria of the time forced many academics to leave their posts, including the director of the Mathematics Institute, Richard Courant. While this revelation was not sufficient to have Cauer removed under the race laws , it stifled his future career. Thus he gained the title of professor but was never given a chair. Nevertheless, he did continue to lecture at the Technical University in Berlin from Although Cauer was able to reproduce this work, he was not able to publish it and it too was lost during the war.
Some time after his death, however, his family arranged for the publication of some of his papers as the second volume, [f] based on surviving descriptions of the intended contents of volume II.
His body was located after the end of the war in a mass grave of victims of Russian executions. Cauer had been shot dead in Berlin-Marienfelde by Soviet soldiers  as a hostage. Indeed, he is considered the founder of the field and the publication of his principal work in English was enthusiastically greeted, even though this did not happen until seventeen years later in The accuracy of predictions of response from such designs depended on accurate impedance matching between sections.
This could be achieved with sections entirely internal to the filter but it was not possible to perfectly match to the end terminations. For this reason image filter designers incorporated end sections in their designs of a different form optimised for an improved match rather than filtering response. The choice of form of such sections was more a matter of designer experience than design calculation.
Network synthesis entirely did away with the need for this. It directly predicted the response of the filter and included the terminations in the synthesis. Whereas network analysis asks what is the response of a given network, network synthesis on the other hand asks what are the networks that can produce a given desired response.
Cauer solved this problem by comparing electrical quantities and functions to their mechanical equivalents. Then, realising that they were completely analogous, applying the known Lagrangian mechanics to the problem. The first is the ability to determine whether a given transfer function is realisable as an impedance network. The second is to find the canonical minimal forms of these functions and the relationships transforms between different forms representing the same transfer function.
Finally, it is not, in general, possible to find an exact finite- element solution to an ideal transfer function - such as zero attenuation at all frequencies below a given cutoff frequency and infinite attenuation above. The third task is therefore to find approximation techniques for achieving the desired responses. The transfer function between a voltage and a current amounting to the expression for the impedance itself.
A useful network can be produced by breaking open a branch of the network and calling that the output. That is, those impedance expressions that could actually be built as a real circuit. The well known Chebyshev filters can be viewed as a special case of elliptic filters and can be arrived at using the same approximation techniques.
So can the Butterworth maximally flat filter, although this was an independent discovery by Stephen Butterworth arrived at by a different method. This made his circuits of less practical use to engineers. From then on network synthesis began to supplant image design as the method of choice. In his habilitation thesis [c] Cauer begins to extend this work by showing that a global canonical form cannot be found in the general case for three-element kind multiports that is, networks containing all three R, L and C elements for the generation of realisation solutions, as it can be for the two-element kind case.
He also studied antimetric 2-ports. Akademie d. Wissenschaften, phys-math Klasse, pp—, Mathematikervereinigung DMV , vol 38, pp63—72, Wissenschaften, phys-math.
Klasse, pp—, On a problem where three positive definite quadratic forms are related to one-dimensional complexes in German Cauer, W, "Ideale Transformatoren und lineare Transformationen", Elektrische Nachrichtentechnik ENT , vol 9, pp—, Ideal transformers and linear transformations in German Cauer, W, "The Poisson integral for functions with positive real part", Bull. Gesellschaft d.
I, Akad. Verlags-Gesellschaft Becker und Erler, Leipzig, II, Akademie-Verlag, Berlin,
What is an Elliptic / Cauer Filter: the basics
Contact 5 pole Cauer filters for the HF bands To build a solid state amplifier today, one has the availability of many fets. Preferably Ldmos as this is the most sturdy and the most forgiving to mistakes from the operator. The normal attenuation of a push pull amplifier on the HF bands is about dB. Thus requiring a filter.
Daigore Compute the frequency response dauer the filter at points. As is clear from the image, elliptic filters are sharper than all the others, but they show ripples on the whole bandwidth. For analog filters, the passband edge frequencies must cayer expressed in radians per second and can take on any positive value. After gain his degree he became a lecturer at St Petersburg University, lecturing main on elliptic functions. Smaller values of passband ripple, Rpand larger values of stopband attenuation, Rsboth result in wider transition bands. Power management RF technology Test Wireless.
5 pole Cauer filters for the HF bands
Kajitaxe If the ripple in both stop-band and pass-band become zero, then the filter transforms into a Butterworth filter. The resulting filter has Rp decibels of peak-to-peak passband ripple and Rs decibels of stopband attenuation down from the peak passband value. Elliptic Cauer filter basics The elliptic filter is characterised by the ripple in both pass-band and stop-band as well as the fastest transition between pass-band and ultimate roll-off of any RF filter type. The other version of the Elliptic filter of Cauer filter has a series inductor and capacitor between the two signal lines as below:. Sadly Zolotarevwas met an untimely death when was on his way to his dacha and was run over by a train in the Tsarskoe Selo station, later dying from the resultant blood poisoning on 19 July As the ripple in the passband approaches zero, the filter becomes a type II Chebyshev filter and finally, as both ripple values approach zero, the filter becomes a Butterworth filter. Elliptic filters offer steeper rolloff characteristics than Butterworth or Chebyshev filters, but are equiripple in both the passband and the stopband. Smaller values of passband ripple, Rpand larger values of stopband attenuation, Rsboth result in wider transition bands.