ELCT564 Spring 2012 Chapter 8: Microwave Filters 4/13/2015 ELCT564 1 Filters • Two-port circuits that exhibit selectivity to frequency: allow some frequencies to go through while block the remaining • In receivers, the system filters the incoming signal right after reception • Filters which direct the received frequencies to different channels are called multiplexers • In many communication systems, the various frequency channels are very close, thus requiring filters with very narrow bandwidth & high out-of band rejection • In some systems, the receive/transmit functions employ different frequencies to achieve high isolation between the R/T channels. • In detector, mixer and multiplier applications, the filters are used to block unwanted high frequency products • Two techniques for filter design: the image parameter method and the insertion loss method. The first is the simplest but the second is the most accurate 4/13/2015 ELCT564 2 Periodic Structures Passband Stopband Bloch Impedance 4/13/2015 ELCT564 3 Terminated Periodic Structures Symmetrical network 4/13/2015 ELCT564 4 Analysis of a Periodic Structure Consider a periodic capacitively loaded line, as shown below. If Zo=50 Ω, d=1.0 cm, and Co=2.666 pF, compute the propagation constant, phase velocity, and Bloch impedance at f=3.0 GHz. Assume k=k0. 4/13/2015 ELCT564 5 Image Parameter Method 4/13/2015 ELCT564 6 Constant-k Filter m-derived section 4/13/2015 ELCT564 7 Composite Filter 4/13/2015 ELCT564 8 Summary of Composite Filter Design 4/13/2015 ELCT564 9 Example of Composite Filter Design Design a low-pass composite filter with a cutoff frequency of 2MHz and impedance of 75 Ω, place the infinite attenuation pole at 2.05 MHz, and plot the frequency response from 0 to 4 MHz. 4/13/2015 ELCT564 10 Insertion Loss Method Filter response is characterized by the power loss ratio defined as: Where Γ(ω) is the reflection coefficient at the input port of the filter, assuming the the output port is matched. Low-pass & Band-pass filter 4/13/2015 Insertion Loss: ELCT564 11 Filter Responses Maximally Flat, Equal Ripple, and Linear Phase Maximally Flat: Provides the flattest possible pass band response for a given complexity. Cutoff frequency is the freqeuncy point which determines the end of the pass band. Usually, where half available power makes it through. Cut-off frequency is called the 3dB point Equal Ripple or Chebyshev Filter: Power loss is expressed as Nth order Chebyshev polynomial TN(ω) T (x)= cos (Ncos-1x), |X| ≤1 N TN(x)= cosh (Ncosh-1x), |X|≥ 1 Much better out-of-band rejection than maximally flat response of the same order. Chebyshev filters are preferred a lot of times. 4/13/2015 ELCT564 12 Filter Responses Linear Phase Filters • Need linear phase response to reduce signal distortion (very important in multiplexing) • Sharp cut-off incompatible with linear phase– design specifically for phase linearity • Inferior amplitude performance • If φ(ω) is the phase response then filter group delay 4/13/2015 ELCT564 13 Filter Design Method • Development of a prototype (low-pass filter with fc=1Hz and is made of generic lumped elements) • Specify prototype by choice of the order of the filter N and the type of its response • Same prototype used for any low-pass, band pass or band stop filter of a given order. • Use appropriate filter transformations to enter specific characteristics • Through these transformations prototype changes – low-pass, band-pass or bandstop • Filter implementation in a desired from (microstrip or CPW) use implementation transformations. 4/13/2015 ELCT564 14 Maximally Flat Low-Pass Filter g0=1,ωc=1, N=1 to 10 4/13/2015 ELCT564 15 Equal-Ripple Low-Pass Filter g0=1,ωc=1, N=1 to 10 4/13/2015 ELCT564 16 Maximally-Flat Time Delay Low-Pass Filter g0=1,ωc=1, N=1 to 10 4/13/2015 ELCT564 17 Filter Transformations • Impedance Scaling • Frequency Scaling for Low-Pass Filters • Low-Pass to High-Pass Transformation 4/13/2015 ELCT564 18 Filter Implementation • Richards’ Transformation • Kuroda’s Identities • • • Physically separate transmission line stubs Transform series stubs into shunt stubs, or vice versa Change impractical characteristic impedances into more realizable ones 4/13/2015 ELCT564 19 Design Steps • Lumped element low pass prototype (from tables, typically) • Convert series inductors to series stubs, shunt capacitors to shunt stubs • Add λ/8 lines of Zo = 1 at input and output • Apply Kuroda identity for series inductors to obtain equivalent with shunt open stubs with λ/8 lines between them • Transform design to 50Ω and fc to obtain physical dimensions (all elements are λ/8). 4/13/2015 ELCT564 20 Low-pass Filters Using Stubs Design a low-pass filter for fabrication using microstrip lines. The specifications include a cutoff frequency of 4GHz, and impedance of 50 Ω, and a third-order 3dB equal-ripple passband response. • • 4/13/2015 Distributed elements—sharper cut-off Response repeats due to the periodic nature of stubs ELCT564 21 Bandpass and Bandstop Filters A useful form of bandpass and bandstop filter consists of λ/4 stubs connected by λ/4 transmission lines. Bandpass filter 4/13/2015 ELCT564 22 Stepped Impedance Low-pass Filters • Use alternating sections of very high and very low characteristics impedances • Easy to design and takes-up less space than low-pass filters with stubs • Due to approximations, electrical performance not as good – applications where sharp cut-off is not required 4/13/2015 ELCT564 23 Stepped Impedance Low-pass Filter Example Design a stepped-impedance low-pass filter having a maximally flat response and a cutoff frequency of 2.5 GHz. It is necessary to have more than 20 dB insertion loss at 4 GHz. The filter impedance is 50 Ω; the highest practical line impedance is 120 Ω, and the lowest is 20 Ω. Consider the effect of losses when this filter is implemented with a microstrip substrate having d = 0.158 cm, εr =4.2, tanδ=0.02, and copper conductors of 0.5 mil thickness. 4/13/2015 ELCT564 24 Coupled Line Theory 4/13/2015 ELCT564 25 Coupled Line Bandpass Filters • This filter is made of N resonators and includes N+1coupled line sections • dn ≈ λg/4 = (λge + λgo)/8 • Find Zoe, Zoo from prototype values and fractional bandwidth • From Zoe, Zoo Calculate conductor and slot width • N-order coupled resonator filter N+1 coupled line sections •Use 2 modes to represent line operation 4/13/2015 ELCT564 26 Coupled Line Bandpass Filters 1. Compute Zoe, Zoo of 1st coupled line section from 2. Compute eve/odd impedances of nth coupled line section 3. Compute even/odd impedances of (N+1) coupled line section 4. Use ADS to find coupled line geometry in terms of w, s, & βe, βo or εeff,e , εeff,o 5. Compute 4/13/2015 ELCT564 27 Coupled Line Bandpass Filters Example I Design a 0.5dB equal ripple coupledline BPF with fo=10GHz, 10%BW & 10-dB attenuation at 13 GHz. Assume Zo=50Ω. From atten. Graph N=4 ok But use N=5 to have Zo=50 Ω go=ge=1, g1=g5=1.7058, g2=g4=1.229, g3=2.5408 4/13/2015 ELCT564 28 Coupled Line Bandpass Filters Example II Design a coupled line bandpass filter with N=3 and 0.5dB equal ripple response. The center frequency is 2GHz, 10%BW & Zo=50Ω. What is the attenuation at 1.8 GHz 4/13/2015 ELCT564 29 Capacitively Coupled Resonator Filter • Convenient for microstrip or stripline fabrication • Nth order filter uses N resonant sections of transmission line with N+1 capacitive gaps between then. • Gaps can be approximated as series capacitors • Resonators are ~ λg/2 long at the center frequency 4/13/2015 ELCT564 30 Capacitively Coupled Resonator Filter Design a bandpass filter using capacitive coupled series resonators, with a 0.5 dB equal-ripple passband characteristic. The center frequency is 2.0 GHz, the bandwidth is 10%, and the impedance is 50 Ω. At least 20 dB of attenuation is required at 2.2GHz 4/13/2015 ELCT564 31 Bandpass Filters using Capacitively Shunt Resonators 4/13/2015 ELCT564 32 Bandpass Filters using Capacitively Shunt Resonators Design a third-order bandpass filter with a 0.5 dB equal-ripple response using capacitively coupled short-circuited shunt stub resonators. The center frequency Is 2.5 GHz, and the bandwidth is 10%. The impedance is 50 Ω. What is the resulting attenuation at 3.0 GHz? 4/13/2015 ELCT564 33