.MCAD 304020000 1 76 1102 0 .CMD PLOTFORMAT 0 0 1 1 1 0 0 1 1 0 0 1 1 1 0 0 1 1 0 1 0 0 1 1 NO-TRACE-STRING 0 2 1 0 1 1 NO-TRACE-STRING 0 3 2 0 1 1 NO-TRACE-STRING 0 4 3 0 1 1 NO-TRACE-STRING 0 1 4 0 1 1 NO-TRACE-STRING 0 2 5 0 1 1 NO-TRACE-STRING 0 3 6 0 1 1 NO-TRACE-STRING 0 4 0 0 1 1 NO-TRACE-STRING 0 1 1 0 1 1 NO-TRACE-STRING 0 2 2 0 1 1 NO-TRACE-STRING 0 3 3 0 1 1 NO-TRACE-STRING 0 4 4 0 1 1 NO-TRACE-STRING 0 1 5 0 1 1 NO-TRACE-STRING 0 2 6 0 1 1 NO-TRACE-STRING 0 3 0 0 1 1 NO-TRACE-STRING 0 4 1 0 1 1 NO-TRACE-STRING 0 1 1 21 15 0 0 3 .CMD FORMAT rd=d ct=10 im=i et=10 zt=15 pr=4 mass length time charge temperature tr=0 vm=0 .CMD SET ORIGIN 0 .CMD SET TOL 0.001000000000000 .CMD SET PRNCOLWIDTH 8 .CMD SET PRNPRECISION 4 .CMD PRINT_SETUP 1.200000 1.000000 1.000000 1.000000 0 .CMD HEADER_FOOTER 1 1 |F *empty* *empty* 0 1 *empty* |P *empty* .CMD HEADER_FOOTER_FONT fontID=14 family=Times^New^Roman points=8 bold=0 italic=0 underline=0 colrid=-1 .CMD HEADER_FOOTER_FONT fontID=15 family=Times^New^Roman points=8 bold=0 italic=0 underline=0 colrid=-1 .CMD DEFAULT_TEXT_PARPROPS 0 0 0 .CMD DEFINE_FONTSTYLE_NAME fontID=0 name=Variables .CMD DEFINE_FONTSTYLE_NAME fontID=1 name=Constants .CMD DEFINE_FONTSTYLE_NAME fontID=2 name=Text .CMD DEFINE_FONTSTYLE_NAME fontID=4 name=User^1 .CMD DEFINE_FONTSTYLE_NAME fontID=5 name=User^2 .CMD DEFINE_FONTSTYLE_NAME fontID=6 name=User^3 .CMD DEFINE_FONTSTYLE_NAME fontID=7 name=User^4 .CMD DEFINE_FONTSTYLE_NAME fontID=8 name=User^5 .CMD DEFINE_FONTSTYLE_NAME fontID=9 name=User^6 .CMD DEFINE_FONTSTYLE_NAME fontID=10 name=User^7 .CMD DEFINE_FONTSTYLE fontID=0 family=Times^New^Roman points=10 bold=0 italic=0 underline=0 colrid=1 .CMD DEFINE_FONTSTYLE fontID=1 family=Times^New^Roman points=10 bold=0 italic=0 underline=0 colrid=1 .CMD DEFINE_FONTSTYLE fontID=2 family=Times^New^Roman points=12 bold=0 italic=0 underline=0 colrid=2 .CMD DEFINE_FONTSTYLE fontID=4 family=Times^New^Roman points=10 bold=1 italic=0 underline=0 colrid=1 .CMD DEFINE_FONTSTYLE fontID=5 family=Courier^New points=10 bold=0 italic=0 underline=0 colrid=-1 .CMD DEFINE_FONTSTYLE fontID=6 family=System points=10 bold=0 italic=0 underline=0 colrid=-1 .CMD DEFINE_FONTSTYLE fontID=7 family=Script points=10 bold=0 italic=0 underline=0 colrid=-1 .CMD DEFINE_FONTSTYLE fontID=8 family=Roman points=10 bold=0 italic=0 underline=0 colrid=-1 .CMD DEFINE_FONTSTYLE fontID=9 family=Modern points=10 bold=0 italic=0 underline=0 colrid=-1 .CMD DEFINE_FONTSTYLE fontID=10 family=Times^New^Roman points=10 bold=0 italic=0 underline=0 colrid=-1 .CMD UNITS U=1 .CMD DIMENSIONS_ANALYSIS 0 0 .CMD COLORTAB_ENTRY 0 0 0 .CMD COLORTAB_ENTRY 128 0 0 .CMD COLORTAB_ENTRY 0 128 0 .CMD COLORTAB_ENTRY 128 128 0 .CMD COLORTAB_ENTRY 0 0 128 .CMD COLORTAB_ENTRY 128 0 128 .CMD COLORTAB_ENTRY 0 128 128 .CMD COLORTAB_ENTRY 128 128 128 .CMD COLORTAB_ENTRY 192 192 192 .CMD COLORTAB_ENTRY 255 0 0 .CMD COLORTAB_ENTRY 0 255 0 .CMD COLORTAB_ENTRY 255 255 0 .CMD COLORTAB_ENTRY 0 0 255 .CMD COLORTAB_ENTRY 255 0 255 .CMD COLORTAB_ENTRY 0 255 255 .CMD COLORTAB_ENTRY 255 255 255 .CMD COLORTAB_ENTRY 255 128 64 .CMD COLORTAB_ENTRY 255 0 128 .CMD COLORTAB_ENTRY 0 64 128 .TXT 1 0 676 0 0 Cg a76.625000,76.625000,102 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard ------------------------------------------------------------------------------ -----------------------} .TXT 3 1 675 0 0 Cg a75.625000,75.625000,85 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard {\b Transmission and Reflection Properties of L-C Band Pass filters with Dissipation Loss}} .TXT 3 0 869 0 0 Cg a75.625000,75.625000,25 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard \tab \tab \tab { \fs20 Michael A. Earle}} .TXT 2 27 1044 0 0 Cg a75.625000,75.625000,26 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard {\fs16 michael.earle@sympatico.ca}} .TXT 3 -27 1043 0 0 Cg a75.625000,75.625000,22 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard \tab \tab \tab {\fs20 October 2000}} .TXT 3 0 678 0 0 Cg a75.625000,75.625000,100 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard ------------------------------------------------------------------------------ ----------------------} .TXT 3 0 681 0 0 Cg a75.625000,75.625000,7 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard {\i General}} .TXT 4 0 679 0 0 Cg a75.625000,75.625000,1338 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard The frequency response of L-C band pass filters derived from low pass prototypes can be determined from the prototype circuit parameters using a transformed frequency variable that includes a term to account for the loss. The loss term depends upon the unloaded Q factor of each resonator in the band pass circuit. For convenience however, each resonator is assumed to have the same unloaded Q factor.\par \par Transmission and reflection properties are found from the overall chain matrix of the cascaded ladder elements that form the prototype. From the elements of the overall chain matrix, a transmission function is derived from which rejection, pass band insertion loss, phase and group delay are found. The insertion loss characteristic shows the impact of the unloaded Q factor upon the pass band insertion loss. Also, the elements of the overall chain matrix are used to find the reflection coefficient function, hence the pass band return loss. \par \par The development which follows is confined to conventional Chebyshev filters of odd or even order. In addition, only filters which begin with a shunt capacitance are selected rather than their dual circuits in which shunt capacitors are replaced with series inductors and vice versa. A simple modification to the expression for the chain matrix allows the dual cases to be considered. } .TXT 41 0 868 0 0 Cg a75.625000,75.625000,10 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard {\i Input data}} .TXT 4 5 819 0 0 Cg a75.625000,75.625000,58 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Here, the desired properties of the filter are specified } .TXT 5 0 820 0 0 Cg a75.625000,75.625000,29 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Lower pass band edge - GHz\tab \tab :} .EQN 0 42 974 0 0 {0:f.1}NAME:3.39 .TXT 4 -42 822 0 0 Cg a75.625000,75.625000,29 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Upper pass band edge - GHz\tab \tab :} .EQN 0 42 975 0 0 {0:f.2}NAME:3.41 .TXT 4 -42 982 0 0 Cg a70.625000,70.625000,34 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Pass band return loss Db \tab \tab :} .EQN 0 42 983 0 0 {0:R}NAME:26 .TXT 4 -42 826 0 0 Cg a75.625000,75.625000,22 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Number of sections\tab \tab \tab :} .EQN 0 42 977 0 0 {0:N}NAME:7 .TXT 3 -42 1100 0 0 Cg a49.625000,49.625000,38 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Termination resistance - Ohms \tab :\tab } .EQN 0 42 1101 0 0 {0:R.o}NAME:50 .TXT 4 -42 828 0 0 Cg a39.750000,39.750000,51 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Start of frequency response range - GHz \tab :} .EQN 0 42 978 0 0 {0:f.s}NAME:3.3 .TXT 4 -42 830 0 0 Cg a40.125000,40.125000,33 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Frequency interval - GHz\tab \tab :} .EQN 0 42 979 0 0 {0:\df}NAME:.0005 .TXT 4 -42 832 0 0 Cg a75.625000,75.625000,29 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Number of frequency points\tab \tab :} .EQN 0 42 980 0 0 {0:nf}NAME:400 .TXT 4 -42 834 0 0 Cg a75.625000,75.625000,21 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Unloaded Q factor\tab \tab \tab :} .EQN 0 42 981 0 0 {0:Q.u}NAME:2000 .TXT 7 -47 705 0 0 Cg a75.625000,75.625000,19 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard {\i Low pass parameters}} .TXT 3 0 706 0 0 Cg a75.625000,75.625000,42 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Centre frequency and normalized pass band.} .EQN 5 24 707 0 0 {0:f.o}NAME:\({0:f.1}NAME*{0:f.2}NAME) .EQN 0 14 708 0 0 {0:w}NAME:({0:f.2}NAME-{0:f.1}NAME)/({0:f.o}NAME) .TXT 4 -38 709 0 0 Cg a75.625000,75.625000,29 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Low pass prototype constants.} .EQN 6 9 710 0 0 {0:\e}NAME:(((10)^(0.1*{0:R}NAME)-1))^(-.5) .EQN 0 18 713 0 0 {0:\b}NAME:{0:ln}NAME((\(1+({0:\e}NAME)^(2))+1)/(\(1+({0:\e}NAME)^(2))-1)) .EQN 0 21 715 0 0 {0:\G}NAME:{0:sinh}NAME(({0:\b}NAME)/(2*{0:N}NAME)) .TXT 7 -48 716 0 0 Cg a75.625000,75.625000,68 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Test for odd or even order and set normalized resistive termination.} .EQN 6 22 717 0 0 ({0:g}NAME)[({0:N}NAME+1):{0:if}NAME(({0:N}NAME-2*{0:floor}NAME(({0:N}NAME)/(2))),1,({0:coth}NAME(({0:\b}NAME)/(4)))^(2)) .EQN 0 35 948 0 0 {0:r}NAME:((({0:g}NAME)[({0:N}NAME+1)))^(-1) .TXT 5 -57 718 0 0 Cg a75.625000,75.625000,38 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Low pass prototype circuit parameters.} .EQN 4 0 719 0 0 {0:j}NAME:1;{0:N}NAME .EQN 5 5 720 0 0 ({0:b}NAME)[({0:j}NAME):({0:\G}NAME)^(2)+({0:sin}NAME({0:j}NAME*({0:\p}NAME)/({0:N}NAME)))^(2) .EQN 0 18 721 0 0 ({0:a}NAME)[({0:j}NAME):{0:sin}NAME((2*{0:j}NAME-1)*({0:\p}NAME)/(2*{0:N}NAME)) .EQN 0 20 748 0 0 ({0:g}NAME)[(1):2*(({0:a}NAME)[(1))/({0:\G}NAME) .EQN 0 12 752 0 0 ({0:g}NAME)[(0):1 .EQN 0 8 953 0 0 ({0:g}NAME)[({0:N}NAME+1)={0}?_n_u_l_l_ .EQN 8 -63 956 0 0 {0:j}NAME:2;{0:N}NAME .EQN 0 28 753 0 0 ({0:g}NAME)[({0:j}NAME):(4*({0:a}NAME)[({0:j}NAME)*({0:a}NAME)[({0:j}NAME-1))/(({0:g}NAME)[({0:j}NAME-1)*({0:b}NAME)[({0:j}NAME-1)) .TXT 6 -28 754 0 0 Cg a75.625000,75.625000,22 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard {\i Transmission functions}} .TXT 3 0 755 0 0 Cg a75.625000,75.625000,28 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Required matrix definitions.} .EQN 8 0 860 0 0 {0:U}NAME:{0:identity}NAME(2) .EQN 0 19 858 0 0 {0:u}NAME({0:n}NAME):({2,2}ö0ö(1+((-1))^({0:n}NAME))/(2)ö1-(1+((-1))^({0:n}NAME))/(2)ö0) .EQN 0 36 759 0 0 {0:r.l}NAME:({2,2}ö(1)/(\({0:r}NAME))ö0ö0ö\({0:r}NAME)) .TXT 9 -55 760 0 0 Cg a75.625000,75.625000,19 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Chain matrix terms.} .EQN 6 25 762 0 0 {0:F}NAME({0:\W}NAME):((1,{0:N}NAME,{0:n}NAME,({0:U}NAME+1j*{0:\W}NAME*((({0:g}NAME)[({0:n}NAME)*{0:u}NAME({0:n}NAME))){49})){65})*{0:r.l}NAME .EQN 7 1 846 0 0 {0:A}NAME({0:\W}NAME):({0:F}NAME({0:\W}NAME))[(0,0) .EQN 0 15 847 0 0 {0:B}NAME({0:\W}NAME):({0:F}NAME({0:\W}NAME))[(0,1) .EQN 4 -15 848 0 0 {0:C}NAME({0:\W}NAME):({0:F}NAME({0:\W}NAME))[(1,0) .EQN 0 15 849 0 0 {0:D}NAME({0:\W}NAME):({0:F}NAME({0:\W}NAME))[(1,1) .TXT 5 -41 856 0 0 Cg a75.625000,75.625000,134 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard {\i Note that for dual circuits, the sequencing matrix }u(n){\i is replaced with its transpose }u(n){\fs20\up T} {\i and termination r is replaced with } r {\fs20\up -1}{\fs20 .}} .TXT 8 0 763 0 0 Cg a75.625000,75.625000,13 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Transmission.} .EQN 0 25 908 0 0 {0:t}NAME({0:\W}NAME):(2)/(({0:A}NAME({0:\W}NAME)+{0:B}NAME({0:\W}NAME)+{0:C}NAME({0:\W}NAME)+{0:D}NAME({0:\W}NAME))) .TXT 7 -25 472 0 0 Cg a75.625000,75.625000,15 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Insertion loss.} .EQN 0 32 909 0 0 {0:L}NAME({0:\W}NAME):-20*{0:log}NAME(|({0:t}NAME({0:\W}NAME))) .TXT 7 -32 488 0 0 Cg a75.625000,75.625000,6 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Phase.} .EQN 0 21 937 0 0 {0:\f}NAME({0:\W}NAME):{0:arg}NAME({0:t}NAME({0:\W}NAME)) .EQN 0 27 938 0 0 {0:\f.deg}NAME({0:\W}NAME):{0:\f}NAME({0:\W}NAME)*({0:deg}NAME)^(-1) .TXT 7 -48 921 0 0 Cg a75.625000,75.625000,22 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Prototype group delay.} .EQN 0 32 919 0 0 {0:t.g}NAME({0:\W}NAME):-({0:\W}NAME"({0:\f}NAME({0:\W}NAME))) .TXT 7 -32 871 0 0 Cg a75.625000,75.625000,24 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Reflection coefficient. } .EQN 0 25 922 0 0 {0:\r}NAME({0:\W}NAME):(1)/(2)*({0:A}NAME({0:\W}NAME)+{0:B}NAME({0:\W}NAME)-{0:C}NAME({0:\W}NAME)-{0:D}NAME({0:\W}NAME))*{0:t}NAME({0:\W}NAME) .TXT 6 -25 925 0 0 Cg a9.625000,9.625000,12 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Return loss.} .EQN 1 29 987 0 0 {0:R.l}NAME({0:\W}NAME):-20*{0:log}NAME(|({0:\r}NAME({0:\W}NAME))) .TXT 4 -29 769 0 0 Cg a75.625000,75.625000,19 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Frequency variable.} .EQN 5 1 927 0 0 {0:q}NAME:0;{0:nf}NAME .EQN 0 10 928 0 0 ({0:f}NAME)[({0:q}NAME):{0:f.s}NAME+{0:q}NAME*{0:\df}NAME .EQN 0 20 929 0 0 ({0:\W}NAME)[({0:q}NAME):((({0:f}NAME)[({0:q}NAME))/({0:f.o}NAME)-({0:f.o}NAME)/(({0:f}NAME)[({0:q}NAME)))*(1)/({0:w}NAME)+(1)/(1j*({0:Q.u}NAME*{0:w}NAME)) .TXT 11 -31 932 0 0 Cg a75.625000,75.625000,22 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Band pass group delay.} .EQN 0 30 930 0 0 {0:t.d}NAME:((({0:t.g}NAME({0:\W}NAME))/(2*{0:\p}NAME*({0:f.2}NAME-{0:f.1}NAME))*(1+((({0:f.o}NAME)/({0:f}NAME)))^(2)))){49} .TXT 15 -30 1038 0 0 Cg a75.625000,75.625000,12 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard {\i Application.}} .TXT 3 0 1039 0 0 Cg a75.625000,75.625000,459 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}{\f1\fcharset2\fnil Symbol;}}\plain \cf1\fs24 \pard The formulae presented above specifically apply to L-C band pass filters and are therefore useful up to frequencies where L-C elements can be usefully realized in practice. These expressions are also useful for narrow band microwave filters realized in transmission line structures where the frequency transformation is approximately represented by the expression for {\f1 W}{\dn q }above. This usually means restricting the band width f{\dn 2} -f{\dn 1} to one or two percent of f{\dn o.}} .TXT 34 0 895 0 0 Cg a75.625000,75.625000,11 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard {\i Output data}} .EQN 3 0 896 0 0 100&0&(_n_u_l_l_&_n_u_l_l_)&{0:L}NAME(({0:\W}NAME)[({0:q}NAME))@3.5&3.3&(_n_u_l_l_&_n_u_l_l_)&({0:f}NAME)[({0:q}NAME) 0 1 1 0 0 4 0 1 1 Frequency GHz 0 1 1 0 0 5 0 1 1 Rejection Db 0 1 0 0 1 1 NO-TRACE-STRING 0 2 1 0 1 1 NO-TRACE-STRING 0 3 2 0 1 1 NO-TRACE-STRING 0 4 3 0 1 1 NO-TRACE-STRING 0 1 4 0 1 1 NO-TRACE-STRING 0 2 5 0 1 1 NO-TRACE-STRING 0 3 6 0 1 1 NO-TRACE-STRING 0 4 0 0 1 1 NO-TRACE-STRING 0 1 1 0 1 1 NO-TRACE-STRING 0 2 2 0 1 1 NO-TRACE-STRING 0 3 3 0 1 1 NO-TRACE-STRING 0 4 4 0 1 1 NO-TRACE-STRING 0 1 5 0 1 1 NO-TRACE-STRING 0 2 6 0 1 1 NO-TRACE-STRING 0 3 0 0 1 1 NO-TRACE-STRING 0 4 1 0 1 1 NO-TRACE-STRING 1 1 1 25 15 10 0 3 Rejection .EQN 0 39 985 0 0 40&0&(_n_u_l_l_&_n_u_l_l_)&{0:R.l}NAME(({0:\W}NAME)[({0:q}NAME))@3.45&3.35&(_n_u_l_l_&_n_u_l_l_)&({0:f}NAME)[({0:q}NAME) 0 1 1 0 0 4 0 1 1 Frequency GHz 0 1 1 0 0 4 0 1 1 Return Loss Db 0 1 0 0 1 1 NO-TRACE-STRING 0 2 1 0 1 1 NO-TRACE-STRING 0 3 2 0 1 1 NO-TRACE-STRING 0 4 3 0 1 1 NO-TRACE-STRING 0 1 4 0 1 1 NO-TRACE-STRING 0 2 5 0 1 1 NO-TRACE-STRING 0 3 6 0 1 1 NO-TRACE-STRING 0 4 0 0 1 1 NO-TRACE-STRING 0 1 1 0 1 1 NO-TRACE-STRING 0 2 2 0 1 1 NO-TRACE-STRING 0 3 3 0 1 1 NO-TRACE-STRING 0 4 4 0 1 1 NO-TRACE-STRING 0 1 5 0 1 1 NO-TRACE-STRING 0 2 6 0 1 1 NO-TRACE-STRING 0 3 0 0 1 1 NO-TRACE-STRING 0 4 1 0 1 1 NO-TRACE-STRING 1 1 1 26 15 10 0 3 Return Loss .EQN 26 -39 899 0 0 10&0&(_n_u_l_l_&_n_u_l_l_)&{0:L}NAME(({0:\W}NAME)[({0:q}NAME))@{0:f.2}NAME&{0:f.1}NAME&(_n_u_l_l_&_n_u_l_l_)&({0:f}NAME)[({0:q}NAME) 0 1 1 0 0 4 0 1 1 Frequency GHz 0 1 1 0 0 5 0 1 1 Passband Loss Db 0 1 0 0 1 1 NO-TRACE-STRING 0 2 1 0 1 1 NO-TRACE-STRING 0 3 2 0 1 1 NO-TRACE-STRING 0 4 3 0 1 1 NO-TRACE-STRING 0 1 4 0 1 1 NO-TRACE-STRING 0 2 5 0 1 1 NO-TRACE-STRING 0 3 6 0 1 1 NO-TRACE-STRING 0 4 0 0 1 1 NO-TRACE-STRING 0 1 1 0 1 1 NO-TRACE-STRING 0 2 2 0 1 1 NO-TRACE-STRING 0 3 3 0 1 1 NO-TRACE-STRING 0 4 4 0 1 1 NO-TRACE-STRING 0 1 5 0 1 1 NO-TRACE-STRING 0 2 6 0 1 1 NO-TRACE-STRING 0 3 0 0 1 1 NO-TRACE-STRING 0 4 1 0 1 1 NO-TRACE-STRING 1 1 1 25 15 10 0 3 Passband Loss .EQN 0 37 900 0 0 100&0&(_n_u_l_l_&_n_u_l_l_)&({0:t.d}NAME)[({0:q}NAME)@{0:f.2}NAME&{0:f.1}NAME&(_n_u_l_l_&_n_u_l_l_)&({0:f}NAME)[({0:q}NAME) 0 1 1 0 0 4 0 1 1 Frequency GHz 0 1 1 0 0 5 0 1 1 Group delay nSec 0 1 0 0 1 1 NO-TRACE-STRING 0 2 1 0 1 1 NO-TRACE-STRING 0 3 2 0 1 1 NO-TRACE-STRING 0 4 3 0 1 1 NO-TRACE-STRING 0 1 4 0 1 1 NO-TRACE-STRING 0 2 5 0 1 1 NO-TRACE-STRING 0 3 6 0 1 1 NO-TRACE-STRING 0 4 0 0 1 1 NO-TRACE-STRING 0 1 1 0 1 1 NO-TRACE-STRING 0 2 2 0 1 1 NO-TRACE-STRING 0 3 3 0 1 1 NO-TRACE-STRING 0 4 4 0 1 1 NO-TRACE-STRING 0 1 5 0 1 1 NO-TRACE-STRING 0 2 6 0 1 1 NO-TRACE-STRING 0 3 0 0 1 1 NO-TRACE-STRING 0 4 1 0 1 1 NO-TRACE-STRING 1 1 1 27 15 10 0 3 Group Delay .EQN 25 -37 1026 0 0 180&-180&(_n_u_l_l_&_n_u_l_l_)&{0:\f.deg}NAME(({0:\W}NAME)[({0:q}NAME))@{0:f.2}NAME&{0:f.1}NAME&(_n_u_l_l_&_n_u_l_l_)&({0:f}NAME)[({0:q}NAME) 0 1 1 0 0 4 0 1 1 Frequency GHz 0 1 1 0 0 4 0 1 1 Phase Deg 0 1 0 0 1 1 NO-TRACE-STRING 0 2 1 0 1 1 NO-TRACE-STRING 0 3 2 0 1 1 NO-TRACE-STRING 0 4 3 0 1 1 NO-TRACE-STRING 0 1 4 0 1 1 NO-TRACE-STRING 0 2 5 0 1 1 NO-TRACE-STRING 0 3 6 0 1 1 NO-TRACE-STRING 0 4 0 0 1 1 NO-TRACE-STRING 0 1 1 0 1 1 NO-TRACE-STRING 0 2 2 0 1 1 NO-TRACE-STRING 0 3 3 0 1 1 NO-TRACE-STRING 0 4 4 0 1 1 NO-TRACE-STRING 0 1 5 0 1 1 NO-TRACE-STRING 0 2 6 0 1 1 NO-TRACE-STRING 0 3 0 0 1 1 NO-TRACE-STRING 0 4 1 0 1 1 NO-TRACE-STRING 1 1 1 24 15 10 0 3 Phase .EQN 8 42 996 0 0 {0:f.o}NAME={0}?_n_u_l_l_ .EQN 3 0 1027 0 0 {0:f.1}NAME={0}?_n_u_l_l_ .EQN 0 12 1028 0 0 {0:f.2}NAME={0}?_n_u_l_l_ .EQN 0 11 1029 0 0 {0:w}NAME={0}?_n_u_l_l_ .EQN 3 -23 1030 0 0 {0:R}NAME={0}?_n_u_l_l_ .EQN 3 0 1031 0 0 {0:N}NAME={0}?_n_u_l_l_ .EQN 0 12 1032 0 0 {0:r}NAME={0}?_n_u_l_l_ .TXT 14 -53 1007 0 0 Cg a74.625000,74.625000,11 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard {\i References.}} .TXT 3 0 1020 0 0 Cg a74.625000,74.625000,97 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard Some useful references from the vast body of literature on the subject of filters are as follows.} .TXT 3 0 1022 0 0 Cg a74.625000,74.625000,130 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard 1]\tab Microwave Filters, Impedance Matching Networks and Coupling Structures \par \tab by Young, Mathai and Jones. Pub. McGraw-Hill. pp95-103} .TXT 5 0 1023 0 0 Cg a74.625000,74.625000,105 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard 2]\tab Notes on Microwave Circuits vol. 2, ch 8, \par \tab by Darko Kajfez. Pub. Kajfez Consulting, Oxford Mississipi} .TXT 5 0 1025 0 0 Cg a74.625000,74.625000,112 {\rtf\ansi \deff0{\colortbl;\red128\green0\blue0;}{\fonttbl{\f0 \fcharset0\fnil Times New Roman;}}\plain\cf1\fs24 \pard 3]\tab Synthesis of Lumped Element, Distributed and Planar Filters.\par \tab by Joseph Helszajn. Pub. Mc. Graw-Hill. ch 12. }