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Lumped electronic RFfilters content:




Lumped electronic RFfilters
Rffilter design starts in the same manner than usual filter design:
 Clarifying specification values of bandwidth, band middle frequency, roll off, rejection, impedance.
 Find out which kind of filter shall be used: Butterworth, Tschebischeff, Cauer, Wave, Zig Zag or Parametric filter.
 To minimize the number of coils, a Parametric filter shout be the first choice .
 Estimation of pole and zeros and solving the filter equations with a computer software or find the filter values in a catalog.
Filter catalog:
 [1] ZWEREV, “ELECTRONIC FILTERS” ;
 [2] SAAL, “THE CATALOG OF NORMALIZED LOW PASS FILTERS”;
 [3] H: RÜHL H.H.NGUYEN, “PRAKTISCHER ENTWURF VON WELLENPARAMETERFILTERN”;
 [4]ECKHARD GLEISSNER , “ZUM ENTWURF VON HOCHFREQUENZ BANDBASSFILTERN”>>, Dissertation TU München  Telefunken Sonderdruck
Up to this design activity, the design of RFfilter differs not from the usual filter design, but the number of electrical components which must
solve the characteristic equation, is very limited .This elements are:
Fig.1 Circuit components to solve filterroots designing RFfilters
The characteristic equation must be solved, using only this elements to nullify the roots of the equation [1]. At the same
time ,expected parasitic values which my appear in a practical circuit, and the coil losses, must be watched. Using series
resonators my lead to unacceptable parasitics. A computeranlysis of the circuit will at least show if it really works what has been designed . After that we can simplify the circuit using Norton’s equations watching the appearing component values.This maximum and minimum values in the frequency range from 70 MHz to 1 GHz are:
 12 nH < L < 500  3000 nH
 0.2 pF < C < 5 nF
 Qmin = 20 , Qmax =140




Parametric filter detects corona in molted transformers
The insulation of high voltage transformers usually is measured by watching the DCleakage current. But in
molted transformers the problem of unknown tiny air bubbles exist. This bubbles my create ionization in the captive air.The corona effect may exist in a transformer for years after the high voltage breakdown
will happen.The ionization bubbles can be found, watching the MHz leakage current with a scope. But this will lead to lot of mismeasurements due of added radio frequencys.To filter this radiowaves , a proper
filter must used. The requirement of the filter is : Fo = 1 MHz, Zin = 1 kOhm, Zout = 50 Ohm, B =100 khz, Fig. 1 shows the measurement circuit, using a sensitive oscilloscope to watch the corona.
Fig 1 Corona measurement equipment
The Filter is a transforming parametric circuit using lumped components rare then an OPactive filter which could be damaged from high voltage sparks. Fig.2. Fig.3 shows S21 .
Fig.2 Corona measurement filter
Fig.3 corona measurement filter S12 (Number ONE Linear Circuit Analyser)
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2 Pole parametric IF bandpass matches OPAMP
The above simple 2 pole parametric bandpass can be modified to be a 10Mhz IFFilter
matched to the OPAMP in and outputs.The input of the filter has 1 Ohm to fit to the OPoutput, whereas the output is resistive matched with a 100 Ohm resistor to fit the Megaohm input of OPAMPs.The series
connection of two or three filters between OPs give an high selectivity IfFilter. Fig 1 shows the circuit and Fig.2 the selectivity of one single filter.
Fig.1 OPAMP bandpass
Fig.2 S21 of op Bandpass (Number ONE Linear Circuit Analyzer)
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A simple parametric IFFilter
We get a simple narrow band IF filter using:
The circuit is gained using Norton’s transformation and matches the output of RFAmp to a transistor. Fig.1
Fig. 1 IFFilter 10 MHz
 C1 = 200 pF; C2 = 100 pF; C3 = 400 pF; C4 =1 2 pF; C5 = 560 pF; C6 = 200 pF; C7 = 200 pF; C8 = 2 pF;
L1 = 450 nH; L2 = 430 nH; L3 =4 000 nH; L4 = 1014 nH;
 C1, C8 and L3 are problem less components and may be fixed SMDcomponents.
 The parasitics at this frequencies are uncritical
Fig. 2 Simple IFFilter (Number ONE Linear Circuit Analyser)
Bandwidth switch able Iffilter
To enhance the selectivity in a receiver, it is often help full to decrease the bandwidth with a switch. Fig.1 shows a IFfilter
having two bandwidths. The switches can be a small coaxial relays. Their little parasitic capacitors will not affect the function of the filter to much, because on their nodes are big capacitors of 400 pF:
Fig.1 Double bandwidth iffilter
The component values are:
 C1 = 200 pF; C2 = 100 pF; C3 = 400 pF(+10 pF); C4 =15 pF (7 pF); C5 = 555 pF (+5 pF); C6 = 300 pF; C7
= 2000 pF; C8 = 2 pF; L1 =440 nH; L2 = 430 nH; L3 = 4000 nH; L4 =1014 nH;
Fig.2 S12 of the double bandwidth filter (Number ONE Linear Circuit Analyser)
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DVBCovering Filter
Outside band signals my disturb the digital television DVB especially at the upper frequencies of 800 Mhz. To reject this
unwanted signals, a DVBCovering filter was developed. We get a practical circuit using a the following parametric filter:
The circuit shows Fig 1 and is developed using a parametric filter software and Norton’s transformation.
Bild 3 DVBCovering Filter !!! Z=50Ohm
 C1 = 0,5 pF; C2 =10 pF; C3 = 2,2 pF; C4 = 1,5 pF; C5 = 2,4 pF; C6 = 0,5 pF;
 C7 = 0,5 pF; C8 = 1 pF; Cpar.= 0,5 pF
 L1 =15 nH; L2 = 20 nH; L3 = 160 nH; L4 = 18 nH; L5 = 11,6 nH;
 C Values are CADvalues, in a practical circuit, the measured parasitic values must taken into account
Fig. 2 S21of Pf341 (Number ONE Linear Circuit Analyser)
 Frequency band = 400 MHz to 800 MHz
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1 GHz Mixeroutput filter
A Mixer must work into some resonating device to gather the wanted mixing products. A small filter can do this job, but it
must be properly matched. We use: and find the circuit of Fig.1
where the parasitics do not affect the function as Fig.2 shows. The low output coil in a practice circuit is only a small path on the PCB
and is calculated with a Q of 20. The black component values are computed values.The PCB capacitors must be subtracted.
Fig.1 Mixeroutputfiltercircuit
Fig.2 S21 of Mixer filter. Matching values are :S11 and S22 = 12dB.
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(Number ONE Linear Circuit Analyser)
A receiverunversalpolefilter
This filter is an example of filters having certain frequency poles.This example shows the high increase on rejection outside
the band. We use a wave parameter filter from [3] having two resonators at Fo and two poles at frequencies near the band
end. As we want high low insertion loss in the band, we add a third resonator at Fo. This filter is an universal filter to be
changed for many purposes. For instance narrow band channel filter or high selectivity if filter. Impedance or frequency
changing is easy. To change the bandwidth , the poles at band end must equally changed in percentage to broaden the
band. This filter is easy to handle in a CADprogram, the three resonators are always at Fo and the poles can than be
adjusted. This allows to build a bandwidth switchable filter. Fig.1 shows the circuit for Fo =100 Mhz and Fig.2 the
transmission S21setting Q=100 . Lower impedance on the input or output can be realized as it is well known , using taping of the first coil.
Fig.1 Wpo2 high selectivity universal filter
Fig.2 wpo2 universalhigh selectivityfilter (Number ONE Linear Circuit Analyser)
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Noise measurement using a parametric if filter German Patent : DE4009076 C2
To measure the noise produced in a communication system, the bandwidth of the noise measurement device has to be
limited over the bandwidth of the system. The noise power must be measured after the filter and the generated noise in the source can be computed from the ENR value:
Fig:1 Noise measurement in a communication channel
Fig.2 Formulas to compute the generated noise
The necessary data’s are: fo=140 MHz; Bandwidth 1dB =+6 MHz, Bandwidth 3dB =+ 10 MHz , Bandwidth 20dB =
+15 Mhz. The used filter is a parametric filter having the grade of 11. The poles are : 4,1,3, Grad =11 . A PCB circuit
using fixed air coils is used. To tune the filter, SMDtrimmers have been used .To manufacture a series product a lot of
tolerance considerations still has to be made.The circuit up to now is shown in Fig. and the transmission S12 in Fig.4.
Fig.3 MHz noise measurementfilter
Fig.4 S21; 413Filter
Fig.5 S12; 413Filter
Fig.6 S22; 413Filter (Number ONE Linear Circuit Analyser)
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QPSKData Filters for digital radio
Today , digital modulated communication channels are everywhere. Ignorant people may think its digital communication,
using data jumps from 1 to zero, the same as digital logic . But this is not the case.We look how the communication bit’s
look like and show how to design lumped RFdata filters for high bit rates. Look at two different digital bit’s, the hard jump
and the soft cosines shape jump and its amplitude density. We get this density from a Fourier transformation . Fig.1.
Fig.1 Amplitude density of data bits
Fig. 2 shows the graphical results of this power density .The hard data bit produces power at multiples of the bitrate. To
avoid data confusion due of this unwanted power, soft square cosines bits are used in digital data communication.
Fig.2 Power density of different bit’s.. Fig. 3 Filter specification of digital radio moddemod filter
Now we look to a classical specification of a filter to change the digital output bits of a QPSKmodulator into a cosines
square shape. And look too, to a QPSK demodulator specification to transform the data bit’s content , back to analog
values. Fig.3. We see the shape of a very broadband low pass filter having a little sinx /x over swing before crossing the
Nyquist frequency fbit. At this frequency the roll off function is working, which is a cosines square function having a variable
steepness n. The demodulator filter is indeed a sinus function, written in cosines form without sin x/x increase. At Fig 4, the equations can be found:
Fig.4 Digital radio moddemod filter specification. formulas
The Filters
Mod and demod filters are both low pass filters, I use the same simple basic filter , it’s a npole low pass from a catalogue
[3] and select it to match approximately the specification requirements. Now how can we get the cos roll off and the sinx / x
increase? We get the roll off, by shaping the poles resonator with a resistor only damping at a certain series resonator
frequency .The sinx / x increase is very easy to get. A little differentiating resistor into the infinite pole capacitor enhances
the corner frequency over swing. This filter is much more easier to adjust than an full computed over swing filter without
resistors, where all components my change the roll off too. Fig 5 shows one pole of the filter. Fig.6 Shows the
transmission of such a modulator filter, using 5 poles in series. At the 2 upper frequency s, the poles work without resistors..
Fig.5 Universal data filter pole
Fig.6 Example of communication modulator filter transmission
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Minimum Coil Parametric 70 MHz If Filter
Parametric filters need less coils than
every other filter type. Here is a minimum coil broadband 70 Mhz Parametric Filter The circuit of Fig.1 is the result of computerized solving of the H(s)
and K(s) equations, of a parametric filter.The components are found in a computer iteration process to nullify the equation H(s).The Circuit shows the typical
CInput of Parametric filters and has only 5 coils to get a grade of 11. Fig.2 presents the transmission .
Infinit poles = 3. Zero poles =4. Finite Poles = 2. Grad = 2*2+4+3=11.
Fig.1 Circuit and values of Fil342
Fig.2 Fil.342 Transmission (Number ONE Linear Circuit Analyser)
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IF ParametricFilter has cos roll off
RF
Receivers for digtital data have three main sections, the RF section, including the input front end, the If section and a digital demodulator. As it can bee seen
at PQSKData Filters for digital radio , the digital demodulator needs a low pass having a very tight specified cos roll off. This low pass, can be simplified, if the already existing IF filter has a cos roll off. . But realizing an IF Filter having this roll off; is not very easy . If we look to the filter catalogues; only very high graded Tschebischeff or Cauer filter can met this specification, but both filter circuits will not work prober at RF frequencies. Beside the specification, the filter to be designed must have a minimum number of coils having a value greater than 30nH. The here shown filter is a computer designed parametric filter having a grade of 10, see Fig.1. The values of the coils, are big enough to use fixed standard SMD Coils with a Q of >70 at 70 MHz. ( For instance Stettner, Componex or Coilcraft types) To adjust the very tight roll off specification an adjustment is used for the roll off. (R1 and R2). The poles must be adjusted, using SMD trimmers. The adjustment is easy , only the poles must be set to its frequencys. Fig.2 shows the computed filter transmission and its specification .Matching is S11= S22 =15dB;

. Fig.1 If Filter with cos roll off
The values are:
 C1=4.2pF; C2=53pF; C3=0.5pF; C4= 500pF; C5=42pF; C6=0.5pF; C7=29,6pF; C8=53pF; C9=25pF;
C10=4.2pF;C11=16pF; C12=132pF; C13=91pF; C14=40pF; C15=27pF; C16=4.2pF;
 L1=42nH; L2=378nH; L3=56nH; L4=127nH; L5=200nH; L7=500nH;
 R1,2=100300Ohm ;
 POLES: 38MHz 48MHz 92MHz 106MHz
Fig.2 Transmission of the cos roll off filter LCA Linear Circuit Analysis
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IF ParametricFilter has cos roll off for wider specification
RF Receivers for Digital data have three main sections, the RF section, including the input front end, the If
section and a digital demodulator. As it can bee seen at PQSKData Filters for digital radio , the digital demodulator needs a low pass having a very tight specified cos roll off. This low pass, can be simplified, if the already existing IF filter has a cos roll off. Above, a very complicated filter has been shown, fulfilling a very tight specification. Here a 70 MHz bandpass is shown, having a cosines roll off, to fit in a somewhat wider specification: The electrical values fits SMD components. Adjustment is easy if the two poles are tuned to its frequencies. Fig. 1 shows the the circuit and Fig.2 the transmission.
Fig.1 Simplified Parametric bandpass having cosines roll off.
The values are:
C1=30pF; C2=28pF; C3=20.4pF; C4=1pF parasitic; C5=13.8pF; C6=5pF; C7=63pF; C8=120pF; C9=83pF;
L1=185nH; L2=137nH; L3=185nH; L4=200nH;L5=118nH;
Fig.1 Simplified parametric cos roll off band filter
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Classical Butter worth Bandpass is realized with SMD Coils
Classical Radio Bandpasses have been realized by means of magnetic coupled
trimmed coils in a metallic housing. A better modern design, is a capacitor coupled filter having small SMD coils used as resonators. Here is an
example of a 4 resonator 70 MHz broadband bandpass to be used in a telecommunication data receiver. Fig.1 shows the circuit. As the SMD coils are
not trimmed at all, three adjustment SMD capacitors are used to compensate the 5 % delivery tolerances of the coils. Fig 2 shows the S12
transmission at 200 Ohm matching, S11/ 22 is 20 dB. On a PCB, the coils must be placed between small flat metal shields, soldered on the PCB, to
prevent magnetic coupling.
The circuit values are :
 C1=30pF; C2=10pF ; C3=1,5 2,5pF, C4=0,81,5pF ; C5=1,5 2,5pF; C6=10pF; C7=47pF;
 L1 =415nH; L2 =520nH; L3 =470nH; L4=330nH;
 Z = 200Ohm; Q = 100;
 Tolerances of capacitors 1%
 Tolerances of coils 5%
As the components are very tight selected, adjustment time of the filter is only a few minutes.
Fig.1 Classic Butter worth bandpass data filter
Fig.2 Tuned bandpass (Number ONE Linear Circuit Analyzer)
The numbered shapes are : (S12 is matched gain) :
 #1 is S12 IF all coil values at +5% .
 #2 is S12 IF all coil values at 5% .
 #3 is S12 of #1 tuned to fo using C3, C4, C5.
 #4 is S12 of #2 tuned to fo using C3, C4, C5.
 S22/S11 = 22dB
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Parametric filter matches receiver input
Show IFfilter The IF Filter shown above in this site can be transformed using Norton’s
transformation, to match input antennas to a RF inputamplifier. To tune this grade 7 filter, only two variable capacitors are
necessary. The matchings are:
 50 Ohm antenna to 25 Ohm common base transistor input. The circuit is at Fig. 1 and the transmission S21 at Fig.2
 High Q Coil on
a ferrite antenna having a impedance of 2kOhm to a 100 Ohm Amplifier input. It is the same circuit, but input and output have been
changed.
Fig.1, 50 Matching of a 50 antenna to a common base transistor
The values are: C1=8pF; C2=15pF, C3=27pF; C4=1,5pF; C5=40pF; C6=5pF; C7=40pF;C8=1pF;
L1=33nH;L2=33nH;L3=300nH; L4=100nH; (High Q SMD Coilcraft Aircoils)
Fig.2 S21 at frequency tuning . C3 from 20 to 28 pF and synchrony C5 from 30 to 40 pF
Fig.3 Matching of a ferrite antenna
The values at fo = 80 Mhz are: C1=15pF; C2=30pF, C3=1pF; C4=2pF; C5=25pF; C6=25pF; L1=200nH;
L2=160nH; L3=4uH; L4=180nH; The resonance frequency of L3 must be >3fo, therefore this coil must be realized using
a high permeability RFFerrite, to need only 3 to 7 turns. Component Values can be scaled by fo1/fo2 to change fo.
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Parametric Data IF Bandpass has 2 finite poles
Parametric Bandpasses with finite poles are a good choice for broadband data
filtering .As an example, a 2 finite pole bandpass has been computed using a FORTRAN Program . The circuit was found by means
of nullifying the roots with circuit elements in an interactive process. The program finds many solution circuits which all solves the
roots.The designer has to decide which circuit has to be used. Fig 1 shows the chosen circuit.The output impedance is set to the 90 Ohm to
optimize PCB wiring. Fig.2 shows the computed S21 transmission values for broad and narrowband. If the infinite pole frequencies are
changed using C2 and C6 synchronously, the bandwidth may be changed up to 30 % .
Fig.1 Broadband parametricbandpass realized with 2 infinite Poles
The Component values are:
 C1=300pF;C2=57pF; C3=35pF; C4=15PF;C5=130pF;C6=90pF; C7=18pF;
 L1=230nH; L2=350nH; L3=60nH; L4=30nH;
 Q1,2,3,4 = 120;
Fig.2 Transmission of Broadband parametric bandpass (Number ONE Linear Circuit Analyzer)
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QPSKtransmitter lowpass with groups delay compensation
Here is an example of the
application of a run time equalizer application to compensate groups run time in a digital communication modem. The groups
runtime which will be compensated is the delay of a lowpass in a QPSK transmitter modulator , having a sinx/ x part ,
befor the roll off frequency. This lowpass is shaping the bits but it should not delay it. Fig.1 shows the transfer S21 of the
filter. We see at 5Mhz a sinx/x increase of 0.5dB followed by a very steep roll off. The phase of the combination of sinx/x
increase and sharp roll off, produces a lot of groups run time which must be compensated . The run time behavior of of the lowpass
with and without groups run time compensation, shows fig.2. The circuit of the lowpass has 5 sections (Fig.3),
2 groups run time equalizer, and 2 lowpass poles and a sin x/x circuit using the combination of series and parallel resonator
driven by means of a RF OpAmp. The equalizers are standard 45 degree circuits , explained at :
Go to run time equalizer circuits:
Fig.1 Transfer of QPSK transmitter lowpass
Fig.2 Groups run time os QPSK lowpass, 1= without equalizer, 2= with equalizer
Fig.3 Circuit of QPSK transmitter lowpass
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Broadband IFfilter realized by means of single resonators between FET’s or tubes
The broadband filters shown above, are the outcome of complicated computer
filter software including NORTON transformation. Here is a very simple method to realize an other type of
broadband bandfilter. Such simple filters have been used in the earlier years of electronics. The only thing we need
for calculation is a pocket calculator. Fig. 1 shows the basic block diagram of the filter. We see between two amplifiers, which
have a very high input and output resistance, one detuned L C resonator. This amplifierresonator circuit
is connected in series n times and it is assumed, that Zi and Zo are very high. The amplifier can be a FET or a Tube.
If the impedances are low, they can be transformed, using coiltaps. The gain must be stable fixed, using a feedback circuit.
Fig.1 Simple broadband amplifier
First we define the parameters :
 Gain1=Gain2= Gain3= Gain4=Gain,
 Zin = < infinite; Zout = < infinite,
 C1=C2=C3=C4=C,
 B = summing voltage gain factor at 0.7, bandwidth ,
 Resonant frequencies = fo1, fo2, fo3, fo4,
 dv = detuning of resonators,
 dv = ; dv =~ 2delta(f)/fo;
 dv(1,2) = detuning of resonator 1 and 2,
 dv(3,4) = detuning of resonator 3 and 4,
 dv(5) = detuning=0,
 f(0) = mittfrequency,
 z = number of resonators,
 z = can be even or odd,
 z = 4. or 5. (or other numbers),
 n = number of resonator,
 phf = phase factor,
 phf = 90/z,
In case of z = 4, the resonator values for a butterworth shaped filter can be found using the following equations:
 dv(1,2)= 1/Q(2,4) = B sin 22.5/f(0), (deg)
 dv(3,4)= 1(Q(3,4) = B cos 22.5/f(0), (deg)
 middfrequency f(1) = f(0) + dv(1,2) f(0),
 middfrequency f(2) = f(0)  dv(1,2) f(0),
 middfrequency f(3) = f(0) + dv(3,4) f(0),
 middfrequency f(4) = f(0)  dv(3,4) f(0),
 resonant frequencies must be adjusted using tunable Inductors,
 Q(1) =1/dv(1,2),
 Q(2) =1/dv(1,2),
 Q(3) =1/dv(3,4),
 Q(4) =1/dv(3,4),
 The different Q values can be realized by using extern resistors at the resonators.
 In case of Z=5 we have one more resonator at f(0),
 The total gain is :
 S = Gain slope of one amplifier (can be computed from a tube, or the amplifiers quadrupole data),),
The same filter can be constructed with tschebischev behavior if the following parameters are used:
 w = Vmax/Vmin = transmission ripple inside the bandwidth,
 n = number of resonators,
 dvb =detuning for factor 0.7 bandwith.
 detuning: ,
 Resonator quality: ,
Fig.1 shows, how the single resonators are added together.
Fig.1 Addition of resonator shapes
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The classical radio bandpass filter.
This article is written for tube radio fans, for understanding the classical radio LC, I Fband filter, which are not used any more in todays radios. This bandpass, was
realized , using two high Q Coils as of part of two resonators, which are coupled using the magnetic field of the coils. Fig.1
shows the mechanical arrangement. The coils have been placed on two small plastic tubes with ferrite adjustment screws. Turning
this screws, the mittfrequency of the resonators can be changed. The distance between the coils determines the
bandwidth of the bandpass. This two resonators are connected between tube amplifiers as fig.2 shows.
Fig.1 mechanical filter design.
Fig.2 circuit of classical radio bandpass
The following parameters are valid:
 MittFrequency, fo is the frequency in the middle of the passband.
 Bandwidth , B, is defined between the points of 1/SQR( 2) = 0.7 of the output voltage
 Coil quality , Q1,Q2, is defined as Q= Ro/(6.28fo)
 Resonance resistor Ro is the paralleled sum of the real loss resistances of coil, capacitor, and adjacent tube resistors.
 Coupling, k = grade of coupling between the coils.
 in case of Q1=Q2 and k=1/Q, k is called kc = critical coupling.
 in case of overcritical coupling we get two ripple peaks in the pass band, the difference between the peaks is h;
 Fig.3 shows the influence of the coupling to the filter ripple.
 detuning of resonators: v = 2delta(f)/fo; deviation from resonator frequency fo=1/SQR(6.28 L C)
 ripple at Q1=Q2 w = Vmax/Vo, w= (1+(QQkk)/2kQ;
The main formulas are:
 Selectivity at Q1=Q2; Qk=1 :
 Transitional coupling :
 Over transitional coupling:
 Untertransitional coupling:
 Bandwidth at over critical coupling:
At Fig.3, 460 kHz Radio IF Bandpass curves depending on different coupling factors are shown.The stop band attenuation
at 9kHz must be as high as possible!
Fig.3 Radio IF bandpass curves.
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Lumped coil quality Q
Computing
of an electronics filter is one thing, realizing the hardware, is another, because of coils quality and selfresonance. Fig.1 shows this coil losses.
Before build up the hardware, the filter should be tested with the coildatas and its parasitic values, in a CAD Program.
The self resonant capacity and the Qvalues, can be taken from the data sheets. Here is an overview of possible Q
Values of different kind of Coils versus the frequency. Fig.2
The losses have the following formulas:
 <<< Coil quality:
 <<< Angel of loss :
 <<< Parasitic C:
Fig.2 CoilQ versus frequency
 ______The red line shows the maximum possible Q for coils made out of single wire
windings on ferrite.
 _______The green line shows the maximum possible Q for coils made
out of RF litz (stranded) wire windings on ferrite.
 For red and green coils,
the optimum ferrite should be used.
 _________The yellow line shows the maximum possible Q for lambda /4 resonators.
 The single points are
examples of SMD coils.
We see in the frequency range between 100 MHz and 2 GHz, only air coils and coax resonators have high Q values. .
As coaxial resonators with high Q values are very bulky, the only solutions are air coils especially SMD air coils. That is, the filter tuning must be made with capacitors.
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140 MHz Broadband ParametricIF Filter for a Digital Modem. German Patent DE 4009075 C2
A 140 MHz ParametricBandpass Filter for a Receiver Data Modem has been developed. The Input matched Filter
circuit has been found, by using “ Saals”* Formulas in a Fortran Program for Zin =50Ohm,. The output of 1.5 Ohm then
was matched using a “ Norton” transforming Software. The testing has been made using “Compact “ linear analysis.
*SAAL, “THE CATALOG OF NORMALIZED LOW PASS FILTERS”;
 Circuit: Fig.1
 Gain, S21 : Fig.2
 Input, Output, S11,S22: Fig.3
Fig 1 Circuit of parametric MHz Bandpass
ParametricFilterComponents are:
 L1=83,7; L 2=419; L 3 =70; L 4=200; L 5= 70; L6= 519 ; L7=70 ; L8=500 ; L9=77,8 nH
 C1=14,4 ; C2=12 ; C3=8,9; C4=0.35; C5=22,5; C6=3,88; C7=18,5; C8=4,8; C9=19,1;pF
 C10=77,8; C11=12; C12=14,3 pF
Fig.2 Gain of parametric MHz Bandpass, ao=1,8dB.
Fig.3 Inputoutputreflection of parametric 140 MHz Bandpass.
Simplification of the
140 MHz Broadband ParametricIF Filter for a Digital Modem.
German Patent DE 4009076 C2
If C10, C12, L8 of Fig.1 are set to 0, C11and L9 to infinite, the Norton Transforming program tries to find positiv finite
other values. After working a few hours, with norton, we get a simpler circuit. Fig.4 . The out of band rejection is even
greater. Fig.5.
Fig.4 Simplified 140 MHz parametric bandpass circuit and values
Fig.5 S21, S12 of the simplified parametric 140 MHz bandpass
Fig.6 S11,S22, of the simplified parametric 140 MHz Bandpass
Practical realisation of the parametric filter
As the capacitor data shoes, all capacitor values to ground have been made with the Nortonprogramm relatively large.
Therefore, the FilterPCB has a full grounding layer. The actual C values than must be smaller than the parasitic values
from the board. As Fig 4 shoes, the filter has a dimension of 6 cm * 2cm. To get the ground really cold I have soldered
two angel plates along the board at the ground side. To prevent parasitic inductance the string from input to output must
be made very broad. The hard ware was tested an I got nearly the computed values.
Fig. 7 TestPCB of the parametric Bandpass filter, (about real) size.
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