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IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 03 Issue: 05 | May-2014, Available @ http://www.ijret.org 312
DESIGN AND SIMULATION OF PRINTED MICRO STRIP LOW PASS
FILTER BASED ON THE ELECTROMAGNETIC MODELS 18GHZ
PRINTED MICROSTRIP LOWPASS FILTER USING X-MODELS
Arfiya Kouser1
, Pramod K B2
, Kumaraswamy H.V3
, Jayaraj N4
1
Department of Electronics and Communication Engineering, The Oxford College of Engineering, Bangalore, Karnataka,
India
2
Department of Electronics Engineering, Jain University, Bangalore, Karnataka, India
3
Department of Telecommunication, R. V. College of Engineering, Bangalore, India
4
Department of Electronics and Communication Engineering, The Oxford College of Engineering, Bangalore, India
Abstract
This paper presents the Design, Simulation and characterization of Printed Micro strip Low Pass Filter based on 15 mil Alumina
substrate. Simulations show a comparison between a pure EM simulation with EM Sight and a more efficient hybrid approach that
combines EM analysis (using X-Models) with conventional circuit simulations and both approaches match the measured data.
Furthermore, the proposed paper has four different low pass filter designs, lumped design; basic designs uses only micro strip lines;
advanced design uses multiple edge coupled micro strip lines, EM sight design provides a very sharp cut-off frequency response with
low insertion loss, results having great agreement with excellent correlation. Tuning and Optimization of the design is carried out
using AWR Microwave office tool.
Keywords— EM sight, AWR, MMIC, X-Models, I-Filter
----------------------------------------------------------------------***--------------------------------------------------------------------
1. INTRODUCTION
A low-pass filter (LPF) offers easy passage to low-frequency
signals and difficult passage to high-frequency signals. It is
highly demanded in modern microwave communication
systems, especially in wireless and mobile communications in
order to suppress harmonics and spurious signals [1]. The
amount of insertion loss and phase shift encountered by a signal
passing through the filter and the amount of rejection of an
undesired signal is a function of the filter design. Filters are
networks that process signals in a frequency-dependent manner
and they can be explained by examining the frequency
dependent nature of the impedance of capacitors and inductors.
With the advent of printed-circuit board (PCB) technology,
microwave system also develop a strip line components and
system with a technique of integrated circuit, called MMIC. It is
a type of Integrated circuit device that operates at microwave
frequencies (300MHz - 300GHz). Inputs and outputs on MMIC
devices are frequently matched to a characteristic impedance of
50 ohms. In advanced filter design, micro strip edge-coupled
filters are used, they have advantages such as easy design
procedures and simple integration into circuits. A general
structure of parallel-coupled (or edge-coupled) micro strip filters
that use half-wavelength line resonators. They are positioned so
that adjacent resonators are parallel to each other along half of
their length. This parallel arrangement gives relatively large
coupling for a given spacing between resonators, therefore this
filter structure is particularly convenient for constructing filters
having a wider bandwidth as compared to the structure for the
end coupled microstrip filters. For the creation of EM waves we
need specific structures with time-varying charges and currents.
At high frequencies hollow waveguides are used to transmit
energy because they do not radiate at any frequency. There are
new design methodologies for EM analysis such as topological
partitioning, functional partitioning, and tuning methodology. In
this filter design topological partitioning method is applied since
it has advantage of gain in speed and also one can make certain
changes very quickly.
This paper deals with the designing and fabrication of microstrip
low pass filters. The designing is done using AWR Microwave
Office simulation program developed by Applied Wave
Research USA. This is a user-friendly software with all of the
capabilities necessary for the accurate modelling and design of
microwave components. It contains a linear, harmonic-balance,
time domain, EM simulation, physical layout and includes linear
and nonlinear noise analysis and can model nonlinear behavior
existing in microwave devices.
2. I-FILTER
I-Filter is specifically developed for synthesis of lumped
element and distributed filters, it brings useful filter synthesis to
the integrated desktop. The module plugs directly into the
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 03 Issue: 05 | May-2014, Available @ http://www.ijret.org 313
Microwave Office design environment and is integrated as a
wizard within the AWR Design Environment (AWRDE), it is
completely integrated into AWRDE and easily accessible.
Limits for minimum line width and minimum line spacing are
specified in iFilter - which are typical dimensions for modern
printed circuit board processes.
I-Filter also provides the ability to adjust secondary parameters
in real time and see the results, in the case of hairpin filters,
includes adjustment of the filter’s nominal impedance. The short
connecting lines between the resonators (in the U-turns), will
have this impedance and the resonator lines will share this line
width. If the area is assumed to be limited to 0.36 x 0.30 inches,
the nominal impedance of the resonators can be adjusted to
examine the effects of line width on performance and required
area. Additionally, I-Filter performs accurate synthesis through
electromagnetic verification with for instance, AWR’s AXIEM
3D planar EM simulator. This is especially important when
designing distributed filters.
Fig 1: Schematic showing ifilter design
2.1 Features:
 Simplicity.
 Power – ideal or real, lumped or distributed, wide variety
 Ease-of-use.
 Integrated – works directly with AWR layout, EM, and
optimization.
 Upgradeable – options for your design needs.
3. MICROSTRIP
Microstrip line consists of thin strip conductor suspended over
ground plane by a low-loss dielectric material. Waves traveling
in microstrip line not only travels in the dielectric medium they
also travel in the air media above the microstrip line. Thus they
don’t support pure TEM waves, rather it supports quasi TEM
approximation.
Fig 2: A basic Microstrip structure
The effective dielectric constant in terms of W (width of the
Microstrip), h (height of the substrate) and εr (relative dielectric
constant) given by Hammerstad and Jensen [11] is:
εre =
εr + 1
2
+
εr − 1
2
1
1 +
12h
W
1
Characteristic impedance of the microstrip line is given by
Zc =
1
c CaCd
(2)
Where c is the velocity of electromagnetic waves in free space
c=2.99x108
m/s. The accuracy of Zc√εre is better than 0.01 %.
4. INITIAL LUMPED DESIGN:
Insertion loss method is used in designing lumped element
filter. It provides ways to shape pass band and stop band of the
filter, although its design theory is much more complex. The
order N of a filter can be found as follows:
𝑁 =
cosh−1
(100.1×𝐼𝐿 − 1)/(100.1×𝛼 − 1)
cosh−1(𝜔/𝜔𝑐)
(3)
The filter design specification has cut-off frequency of 18GHz.
From the above equation order of the filter is found to be 7. For
this design prototype parameters are as follows:
g0 = g8 = 1
g1 = g7 = 1.3722
g2 = g6 = 1.3781
g3 = g5 = 2.2756
g4 = 1.5001
5. IMPLEMENTATION:
5.1 Basic Design:
Basic filter is designed using microstrip lines such as MLIN,
MLEF and MTEE$ microstrips which are available in AWR
tool. Input/Output ports are matched to 50ohms, these are also
available in AWR tool. Microstrip has relative dielectric
constant, ɛᵣ=9.8, substrate thickness H=15mil, conductor
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 03 Issue: 05 | May-2014, Available @ http://www.ijret.org 314
thickness T=0.3mil, metal bulk resistivity normalized to gold
ρ=2 and loss tangent dielectric, Tand=0.002. Basic filter design
has insertion-loss of -1.0896dB and return loss of -42.441dB at
18.95GHz.
Fig 3: Basic schematic of LPF
5.2 Advanced Filter Design:
Advanced filter is designed using edge coupled microstrip line.
The following figure shows the cross section of a coupled line.
They support two modes of excitation, even and odd mode.
Fig 4: A Coupled Line Structure.
5.3 Even Mode:
In even mode excitation both the microstrip coupled lines have
the same voltage potential resulting in a magnetic wall at the
symmetry plane.
Fig 5: Quasi-TEM, Even Mode of a Pair of Coupled Microstrip
Lines
The Odd mode Impedances can be calculated using the
following formulae
(𝑍 𝑜𝑒 )𝑗 ,𝑗+1 =
1
𝑌0
1 +
𝐽01
𝑌0
+
𝐽01
𝑌0
2
(4)
Where,
𝐽01
𝑌0
=
𝜋∆
2𝑔0 𝑔1
(5)
Jj.j+1
Y0 j=1 to n−1
=
𝜋∆
2ω1
′ 2𝑔𝑗 𝑔𝑗 +1
(6)
𝐽𝑛,𝑛+1
𝑌0
=
𝜋∆
2𝑔 𝑛 𝑔 𝑛+1
(7)
5.4 Odd Mode
In odd mode the coupled microstrip line possess opposite
potential. This results into an electric wall at the symmetry. The
following cross section diagram shows the same.
Fig 6: Quasi-TEM, Odd Mode of a Pair of Coupled Microstrip
Lines
The Odd mode impedances can be calculated as same as Even
mode impedances using the following formulae.
(𝑍 𝑜𝑜 )𝑗,𝑗+1 =
1
𝑌0
1 −
𝐽01
𝑌0
+
𝐽01
𝑌0
2
(8)
Where,
𝐽01
𝑌0
=
𝜋∆
2𝑔0 𝑔1
(9)
Jj.j+1
Y0 j=1 to n−1
=
𝜋∆
2ω1
′ 2𝑔𝑗 𝑔𝑗+1
(10)
𝐽𝑛,𝑛+1
𝑌0
=
𝜋∆
2𝑔 𝑛 𝑔 𝑛+1
11
Table 1: Odd and Even Impedances values obtained from the
admittance inverter parameters
J
Even – mode
impedance
(Zoe)j , j+1
Odd – mode
impedance
(Zoo)j , j+1
Characteristic
Impedance Zo
Zo2
 (Zoe)(Zoo)
0 78.777 37.9177 54.6514
1 59.7244 43.0544 50.7089
2 57.3072 44.3672 50.4238
3 56.9688 44.5688 50.3888
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 03 Issue: 05 | May-2014, Available @ http://www.ijret.org 315
Applied Wave Research has developed accurate advanced
numerical models for microstrip edge coupled lines, which are
labelled MXCLIN elements. “X,” which can range from 3 to 16,
represents the number of parallel edge-coupled microstrip lines.
Figure.7 shows AWR MXCLIN with 8 coupled lines.
Fig 7: AWR MXCLIN advanced numerical element model
where X=8.
5.5 Electromagnetic Model:
At frequency greater than 3GHz it is compulsory for any
microstrip design to undergo EM simulation. EM simulation
considers all the dielectric effect so the response of the
schematic will lose some of its characteristics and as the
frequency goes higher and higher these responses may vary
enormously. So at the higher frequency the EM Simulation is
very necessary simultaneously it is difficulty to meet the
specification. To increase the length of all resonators by
connecting a multiple coupled line in between the two halves.
The multiple coupled lines can come from a good circuit theory
model, or it can be generated from an EM analysis. Increase the
length of the added line to decrease the center frequency of the
filter. To shorten all the resonators, connect a negative length
line. While not physical, circuit theory and EM analysis
programs both have no trouble doing this just connect a multiple
coupled line in between the two halves. No need to repeat the
entire EM analysis. Tune up your layout with circuit theory, do
one more EM analysis to confirm the changes, and then
fabricate. Design closure, quick and easy: a tunable EM
analysis.
Fig 8: EM sight filter.
EM sight is designed using EM layer= 2, a perfect conductor
material, drawing layer of top copper conductor, input port of
impedance 50ohms and reference plane distance= 30mil, and
output port of impedance 50ohms and reference plane distance=
34mil.
Fig 9: Three dimensional EM Structure design with enclosure
box
An EM simulation is recommended to confirm the design
accuracy fig 9 shows the simulation of planar 3D structures
containing multiple metallization and dielectric layers. The
structures can have interconnecting vias between layers or to
ground. EMSight uses the Galerkin Method of Moments (MoM)
in the spectral domain, an extremely accurate method for
analyzing micro strip, this technique can provide accurate
simulation results up to 100 GHz and beyond.
6. RESULT AND ANALYSIS:
Insertion loss plot of lumped element low pass filter is shown in
figure 10. Here the insertion loss at 18.14GHz is -2.999dB.
Fig 10: Insertion loss of Lumped design.
Return loss of lumped element low pass filter is shown in fig 11.
Here the return loss at 18.011GHz is -16.029dB.
W1
W2
W3
W4
W5
W6
W7
W8
1 2 3 4 5 6 7 8
9 10 11 12 13 14 15 16
M8CLIN
ID=TL1
W1=W2 mil
W2=W4 mil
W3=W6 mil
W4=W6 mil
W5=W6 mil
W6=W6 mil
W7=W4 mil
W8=W2 mil
S1=L3 mil
S2=L5 mil
S3=L7 mil
S4=L9 mil
S5=L7 mil
S6=L5 mil
S7=L3 mil
L=24 mil
Acc=1
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 03 Issue: 05 | May-2014, Available @ http://www.ijret.org 316
Fig 11: Return loss of Lumped design
Insertion loss of Basic low pass filter design is shown in fig 12.
Here the insertion loss at 18.95GHz is -1.0869dB.
Fig 12: Insertion loss of Basic low pass filter.
Return loss of basic low pass filter is shown in fig 13. Here the
return loss at 18GHz is -42.441dB.
Fig 13: Return loss of basic low pass filter.
Insertion loss of advanced low pass filter is shown in fig 14.
Here the insertion loss at 18.498GHz is -3.019dB.
Fig 14: Insertion loss of advanced low pass filter.
Return loss of advanced low pass filter is shown in fig 15. Here
the return loss at 18GHz is -10.001dB.
Fig 15: Return loss of advanced low pass filter.
Insertion loss of EM sight low pass filter is shown in fig 16.
Here the insertion loss at 18.586GHz is -3.039dB.
Fig 16: Insertion loss of EM sight low pass filter.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 03 Issue: 05 | May-2014, Available @ http://www.ijret.org 317
Return loss of EM sight low pass filter is shown in fig 17. Here
the return loss at 18.124GHz is -20dB.
Fig 17: Return loss of EM sight low pass filter.
VSWR comparison between iFilter, basic LPF, advanced LPF
and EM sight design is shown in fig 18. The advanced design
and EM sight design having very good VSWR value. Variation
of VSWR curve is crazy in Lumped design which is shown in
fig 19.
Fig 18: VSWR comparison.
Fig 19: Variation of VSWR in lumped design.
7. SUMMARY
Table 2: Characteristics Comparison of all design types
Table 3: Parameters Comparison with previous designs
8. CONCLUSIONS
This paper shows the design of 18GHz printed micro strip low
pass filter on 15 mil Alumina substrate and simulation shows the
comparison between lumped , basic , advanced and EM sight
design successfully. The "LPF EMSight” shows the filter in the
EMSight 2.5D electromagnetic simulator, which is viewed in
three dimensions. This compares very closely to measured data.
The "LPF Advanced" schematic makes use of advanced X-
Models (EM-based models), coupled lines and other linear
schematic elements, including a substrate definition. This too
gives excellent correlation. The "LPF Basic" indicates potential
errors in schematic entry with the associated errors in results. A
good comparison is achieved among all four designs and
validated through circuits and EM sight in AWR MWO
Environment, furthermore particular design can be chosen based
on tradeoffs.
The design will be useful for Satellite and PTP Communications
Links, Marine and Pleasure Craft Radar, Port Vessel Traffic
Services etc…
Design Frequen
cy
Insertio
n loss
Return
loss
VSW
R
Lumped
design
18.14GH
z
-2.996dB -
16.067d
B
1.5
Measured
filter
18.659G
Hz
-
3.0573d
B
-
18.458d
B
10.24
Basic design 18.95GH
z
-
1.0869d
B
-
42.441d
B
1.029
Advanced
design
18.498G
Hz
-
3.0195d
B
-
10.001d
B
1.826
EM sight
design
18.586G
Hz
-3.039dB -
20.001d
B
1.081
References [2] [7] [10] This
work
Order of the
filter
5 4 3 7
Cut-off
frequency
2 &
3GHz
7.7GHz 1990MHz 18.95GHz
Insertion-
loss
-0.6dB 18dB <0.6dB -
1.0869dB
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 03 Issue: 05 | May-2014, Available @ http://www.ijret.org 318
REFERENCES
[1] “A novel design of Narrowband Band pass filters
onPTFE laminate using Radial stubs” Pramod, K.B. ;
Shyam, S.S. ; Kumaraswamy, H.V. ;Praveen, K.B.
Informatics, Electronics & Vision (ICIEV), 2013
International Conference on Digital Object
Identifier:10.1109/ICIEV.2013.6572584 Publication
Year: 2013 , Page(s): 1 - 6
[2] “Design and Simulation of RF MEMS Switchable Low
Pass Filter” M. Jeya Rani, M. Anitha, M. Arul Jothi and
S. Kanthamani MEMS Design Center, Department of
ECE, Thiagarajar College of Engineering, Madurai,
Tamil Nadu ,INDIA. 978-1-4673-1515-9/12/$31.00
©2012 IEEE
[3] “Design and Development of High Gain Wideband
Microstrip Antenna and DGS Filters”,by Adel Bedair
Abdel-Mooty Abdel-Rahman, IEEE AP-S 2008
[4] “Design Of Compact Microstrip Low-Pass Filter With
Ultra-Wide Stopband Using Sirs” L. Wang, H.C.Yang
and Y.Li, School of Physical Electronics, UESTC
Chengdu, China Vol. 18, 179-186, 2010
[5] “An 880 / 1760 MHz Tunable Bandwidth Active RC
Low-pass Filter using High Gain Amplifier” Kijin Kim,
Electrical Engineering Department, KAIST 978-1-4673-
2990-3/12/©2012 IEEE
[6] “A very linear low pass filter with automatic frequency
tuning”, by J. Galán, M. Pedro, T. Sánchez-Rodríguez,
F. Muñoz, R. G. Carvajal, and A. López-Martín IEEE
TRANSACTIONS ON VERY LARGE SCALE
INTEGRATION (VLSI) SYSTEMS, VOL. 21, NO. 1,
JANUARY 2013
[7] “A DC to 6 GHz Balanced Elliptic Low-Pass Filter in
CMOS 130nm Technology”, by Mohammad S. Mahani,
Ramesh Abhari Electrical and Computer Engineering
Department, McGill University, Montreal, Quebec,
Canada 978-1-4577-1318-7/12/$26.00 © 2012 IEEE.
[8] ” A Miniaturized High Out-band Suppression Low-pass
Filter Based on the Lumped Circuit Model Using LTCC
Technology”, by Xiaoshi Huo and Peng Wang Research
Institute of Electronic Science and Technology
University of Electronic Science and Technology of
China Chengdu China 978-1-4673-1697-2/12/$31.00 ©
2012 IEEE.
[9] John T. Taylor and Qiuting Huang. CRC handbook of
electrical filters. CRC publisher, 1997.
[10] “Development of UWB HTS Bandpass Filters With
Microstrip Stubs-Loaded Three-Mode Resonator“, by
Hiroyuki Ishii, Toru Kimura, Naotaka Kobayashi,
Atsushi Saito, Zhewang Ma, and Shigetoshi Ohshima
IEEE TRANSACTIONS ON APPLIED
SUPERCONDUCTIVITY, VOL. 23, NO. 3, JUNE 2013
1051-8223/$31.00 © 2012 IEEE
[11] Cornelis Jan Kikkert, “A Design Technique for
Microstrip Filters”. Electrical and Computer
Engineering James Cook University Townsville,
Queensland, Australia.
[12] J. S. Hong and M. J. Lancaster, “Theory and experiment
of novel microstrip slow-wave open-loop resonator
filters,” IEEE Trans. Microwave Theory Tech., vol. 45,
pp. 2358–2365, 1997.

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Design and simulation of printed micro strip low pass filter based on the electromagnetic models 18 ghz printed microstrip lowpass filter using x models

  • 1. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 03 Issue: 05 | May-2014, Available @ http://www.ijret.org 312 DESIGN AND SIMULATION OF PRINTED MICRO STRIP LOW PASS FILTER BASED ON THE ELECTROMAGNETIC MODELS 18GHZ PRINTED MICROSTRIP LOWPASS FILTER USING X-MODELS Arfiya Kouser1 , Pramod K B2 , Kumaraswamy H.V3 , Jayaraj N4 1 Department of Electronics and Communication Engineering, The Oxford College of Engineering, Bangalore, Karnataka, India 2 Department of Electronics Engineering, Jain University, Bangalore, Karnataka, India 3 Department of Telecommunication, R. V. College of Engineering, Bangalore, India 4 Department of Electronics and Communication Engineering, The Oxford College of Engineering, Bangalore, India Abstract This paper presents the Design, Simulation and characterization of Printed Micro strip Low Pass Filter based on 15 mil Alumina substrate. Simulations show a comparison between a pure EM simulation with EM Sight and a more efficient hybrid approach that combines EM analysis (using X-Models) with conventional circuit simulations and both approaches match the measured data. Furthermore, the proposed paper has four different low pass filter designs, lumped design; basic designs uses only micro strip lines; advanced design uses multiple edge coupled micro strip lines, EM sight design provides a very sharp cut-off frequency response with low insertion loss, results having great agreement with excellent correlation. Tuning and Optimization of the design is carried out using AWR Microwave office tool. Keywords— EM sight, AWR, MMIC, X-Models, I-Filter ----------------------------------------------------------------------***-------------------------------------------------------------------- 1. INTRODUCTION A low-pass filter (LPF) offers easy passage to low-frequency signals and difficult passage to high-frequency signals. It is highly demanded in modern microwave communication systems, especially in wireless and mobile communications in order to suppress harmonics and spurious signals [1]. The amount of insertion loss and phase shift encountered by a signal passing through the filter and the amount of rejection of an undesired signal is a function of the filter design. Filters are networks that process signals in a frequency-dependent manner and they can be explained by examining the frequency dependent nature of the impedance of capacitors and inductors. With the advent of printed-circuit board (PCB) technology, microwave system also develop a strip line components and system with a technique of integrated circuit, called MMIC. It is a type of Integrated circuit device that operates at microwave frequencies (300MHz - 300GHz). Inputs and outputs on MMIC devices are frequently matched to a characteristic impedance of 50 ohms. In advanced filter design, micro strip edge-coupled filters are used, they have advantages such as easy design procedures and simple integration into circuits. A general structure of parallel-coupled (or edge-coupled) micro strip filters that use half-wavelength line resonators. They are positioned so that adjacent resonators are parallel to each other along half of their length. This parallel arrangement gives relatively large coupling for a given spacing between resonators, therefore this filter structure is particularly convenient for constructing filters having a wider bandwidth as compared to the structure for the end coupled microstrip filters. For the creation of EM waves we need specific structures with time-varying charges and currents. At high frequencies hollow waveguides are used to transmit energy because they do not radiate at any frequency. There are new design methodologies for EM analysis such as topological partitioning, functional partitioning, and tuning methodology. In this filter design topological partitioning method is applied since it has advantage of gain in speed and also one can make certain changes very quickly. This paper deals with the designing and fabrication of microstrip low pass filters. The designing is done using AWR Microwave Office simulation program developed by Applied Wave Research USA. This is a user-friendly software with all of the capabilities necessary for the accurate modelling and design of microwave components. It contains a linear, harmonic-balance, time domain, EM simulation, physical layout and includes linear and nonlinear noise analysis and can model nonlinear behavior existing in microwave devices. 2. I-FILTER I-Filter is specifically developed for synthesis of lumped element and distributed filters, it brings useful filter synthesis to the integrated desktop. The module plugs directly into the
  • 2. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 03 Issue: 05 | May-2014, Available @ http://www.ijret.org 313 Microwave Office design environment and is integrated as a wizard within the AWR Design Environment (AWRDE), it is completely integrated into AWRDE and easily accessible. Limits for minimum line width and minimum line spacing are specified in iFilter - which are typical dimensions for modern printed circuit board processes. I-Filter also provides the ability to adjust secondary parameters in real time and see the results, in the case of hairpin filters, includes adjustment of the filter’s nominal impedance. The short connecting lines between the resonators (in the U-turns), will have this impedance and the resonator lines will share this line width. If the area is assumed to be limited to 0.36 x 0.30 inches, the nominal impedance of the resonators can be adjusted to examine the effects of line width on performance and required area. Additionally, I-Filter performs accurate synthesis through electromagnetic verification with for instance, AWR’s AXIEM 3D planar EM simulator. This is especially important when designing distributed filters. Fig 1: Schematic showing ifilter design 2.1 Features:  Simplicity.  Power – ideal or real, lumped or distributed, wide variety  Ease-of-use.  Integrated – works directly with AWR layout, EM, and optimization.  Upgradeable – options for your design needs. 3. MICROSTRIP Microstrip line consists of thin strip conductor suspended over ground plane by a low-loss dielectric material. Waves traveling in microstrip line not only travels in the dielectric medium they also travel in the air media above the microstrip line. Thus they don’t support pure TEM waves, rather it supports quasi TEM approximation. Fig 2: A basic Microstrip structure The effective dielectric constant in terms of W (width of the Microstrip), h (height of the substrate) and εr (relative dielectric constant) given by Hammerstad and Jensen [11] is: εre = εr + 1 2 + εr − 1 2 1 1 + 12h W 1 Characteristic impedance of the microstrip line is given by Zc = 1 c CaCd (2) Where c is the velocity of electromagnetic waves in free space c=2.99x108 m/s. The accuracy of Zc√εre is better than 0.01 %. 4. INITIAL LUMPED DESIGN: Insertion loss method is used in designing lumped element filter. It provides ways to shape pass band and stop band of the filter, although its design theory is much more complex. The order N of a filter can be found as follows: 𝑁 = cosh−1 (100.1×𝐼𝐿 − 1)/(100.1×𝛼 − 1) cosh−1(𝜔/𝜔𝑐) (3) The filter design specification has cut-off frequency of 18GHz. From the above equation order of the filter is found to be 7. For this design prototype parameters are as follows: g0 = g8 = 1 g1 = g7 = 1.3722 g2 = g6 = 1.3781 g3 = g5 = 2.2756 g4 = 1.5001 5. IMPLEMENTATION: 5.1 Basic Design: Basic filter is designed using microstrip lines such as MLIN, MLEF and MTEE$ microstrips which are available in AWR tool. Input/Output ports are matched to 50ohms, these are also available in AWR tool. Microstrip has relative dielectric constant, ɛᵣ=9.8, substrate thickness H=15mil, conductor
  • 3. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 03 Issue: 05 | May-2014, Available @ http://www.ijret.org 314 thickness T=0.3mil, metal bulk resistivity normalized to gold ρ=2 and loss tangent dielectric, Tand=0.002. Basic filter design has insertion-loss of -1.0896dB and return loss of -42.441dB at 18.95GHz. Fig 3: Basic schematic of LPF 5.2 Advanced Filter Design: Advanced filter is designed using edge coupled microstrip line. The following figure shows the cross section of a coupled line. They support two modes of excitation, even and odd mode. Fig 4: A Coupled Line Structure. 5.3 Even Mode: In even mode excitation both the microstrip coupled lines have the same voltage potential resulting in a magnetic wall at the symmetry plane. Fig 5: Quasi-TEM, Even Mode of a Pair of Coupled Microstrip Lines The Odd mode Impedances can be calculated using the following formulae (𝑍 𝑜𝑒 )𝑗 ,𝑗+1 = 1 𝑌0 1 + 𝐽01 𝑌0 + 𝐽01 𝑌0 2 (4) Where, 𝐽01 𝑌0 = 𝜋∆ 2𝑔0 𝑔1 (5) Jj.j+1 Y0 j=1 to n−1 = 𝜋∆ 2ω1 ′ 2𝑔𝑗 𝑔𝑗 +1 (6) 𝐽𝑛,𝑛+1 𝑌0 = 𝜋∆ 2𝑔 𝑛 𝑔 𝑛+1 (7) 5.4 Odd Mode In odd mode the coupled microstrip line possess opposite potential. This results into an electric wall at the symmetry. The following cross section diagram shows the same. Fig 6: Quasi-TEM, Odd Mode of a Pair of Coupled Microstrip Lines The Odd mode impedances can be calculated as same as Even mode impedances using the following formulae. (𝑍 𝑜𝑜 )𝑗,𝑗+1 = 1 𝑌0 1 − 𝐽01 𝑌0 + 𝐽01 𝑌0 2 (8) Where, 𝐽01 𝑌0 = 𝜋∆ 2𝑔0 𝑔1 (9) Jj.j+1 Y0 j=1 to n−1 = 𝜋∆ 2ω1 ′ 2𝑔𝑗 𝑔𝑗+1 (10) 𝐽𝑛,𝑛+1 𝑌0 = 𝜋∆ 2𝑔 𝑛 𝑔 𝑛+1 11 Table 1: Odd and Even Impedances values obtained from the admittance inverter parameters J Even – mode impedance (Zoe)j , j+1 Odd – mode impedance (Zoo)j , j+1 Characteristic Impedance Zo Zo2  (Zoe)(Zoo) 0 78.777 37.9177 54.6514 1 59.7244 43.0544 50.7089 2 57.3072 44.3672 50.4238 3 56.9688 44.5688 50.3888
  • 4. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 03 Issue: 05 | May-2014, Available @ http://www.ijret.org 315 Applied Wave Research has developed accurate advanced numerical models for microstrip edge coupled lines, which are labelled MXCLIN elements. “X,” which can range from 3 to 16, represents the number of parallel edge-coupled microstrip lines. Figure.7 shows AWR MXCLIN with 8 coupled lines. Fig 7: AWR MXCLIN advanced numerical element model where X=8. 5.5 Electromagnetic Model: At frequency greater than 3GHz it is compulsory for any microstrip design to undergo EM simulation. EM simulation considers all the dielectric effect so the response of the schematic will lose some of its characteristics and as the frequency goes higher and higher these responses may vary enormously. So at the higher frequency the EM Simulation is very necessary simultaneously it is difficulty to meet the specification. To increase the length of all resonators by connecting a multiple coupled line in between the two halves. The multiple coupled lines can come from a good circuit theory model, or it can be generated from an EM analysis. Increase the length of the added line to decrease the center frequency of the filter. To shorten all the resonators, connect a negative length line. While not physical, circuit theory and EM analysis programs both have no trouble doing this just connect a multiple coupled line in between the two halves. No need to repeat the entire EM analysis. Tune up your layout with circuit theory, do one more EM analysis to confirm the changes, and then fabricate. Design closure, quick and easy: a tunable EM analysis. Fig 8: EM sight filter. EM sight is designed using EM layer= 2, a perfect conductor material, drawing layer of top copper conductor, input port of impedance 50ohms and reference plane distance= 30mil, and output port of impedance 50ohms and reference plane distance= 34mil. Fig 9: Three dimensional EM Structure design with enclosure box An EM simulation is recommended to confirm the design accuracy fig 9 shows the simulation of planar 3D structures containing multiple metallization and dielectric layers. The structures can have interconnecting vias between layers or to ground. EMSight uses the Galerkin Method of Moments (MoM) in the spectral domain, an extremely accurate method for analyzing micro strip, this technique can provide accurate simulation results up to 100 GHz and beyond. 6. RESULT AND ANALYSIS: Insertion loss plot of lumped element low pass filter is shown in figure 10. Here the insertion loss at 18.14GHz is -2.999dB. Fig 10: Insertion loss of Lumped design. Return loss of lumped element low pass filter is shown in fig 11. Here the return loss at 18.011GHz is -16.029dB. W1 W2 W3 W4 W5 W6 W7 W8 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 M8CLIN ID=TL1 W1=W2 mil W2=W4 mil W3=W6 mil W4=W6 mil W5=W6 mil W6=W6 mil W7=W4 mil W8=W2 mil S1=L3 mil S2=L5 mil S3=L7 mil S4=L9 mil S5=L7 mil S6=L5 mil S7=L3 mil L=24 mil Acc=1
  • 5. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 03 Issue: 05 | May-2014, Available @ http://www.ijret.org 316 Fig 11: Return loss of Lumped design Insertion loss of Basic low pass filter design is shown in fig 12. Here the insertion loss at 18.95GHz is -1.0869dB. Fig 12: Insertion loss of Basic low pass filter. Return loss of basic low pass filter is shown in fig 13. Here the return loss at 18GHz is -42.441dB. Fig 13: Return loss of basic low pass filter. Insertion loss of advanced low pass filter is shown in fig 14. Here the insertion loss at 18.498GHz is -3.019dB. Fig 14: Insertion loss of advanced low pass filter. Return loss of advanced low pass filter is shown in fig 15. Here the return loss at 18GHz is -10.001dB. Fig 15: Return loss of advanced low pass filter. Insertion loss of EM sight low pass filter is shown in fig 16. Here the insertion loss at 18.586GHz is -3.039dB. Fig 16: Insertion loss of EM sight low pass filter.
  • 6. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 03 Issue: 05 | May-2014, Available @ http://www.ijret.org 317 Return loss of EM sight low pass filter is shown in fig 17. Here the return loss at 18.124GHz is -20dB. Fig 17: Return loss of EM sight low pass filter. VSWR comparison between iFilter, basic LPF, advanced LPF and EM sight design is shown in fig 18. The advanced design and EM sight design having very good VSWR value. Variation of VSWR curve is crazy in Lumped design which is shown in fig 19. Fig 18: VSWR comparison. Fig 19: Variation of VSWR in lumped design. 7. SUMMARY Table 2: Characteristics Comparison of all design types Table 3: Parameters Comparison with previous designs 8. CONCLUSIONS This paper shows the design of 18GHz printed micro strip low pass filter on 15 mil Alumina substrate and simulation shows the comparison between lumped , basic , advanced and EM sight design successfully. The "LPF EMSight” shows the filter in the EMSight 2.5D electromagnetic simulator, which is viewed in three dimensions. This compares very closely to measured data. The "LPF Advanced" schematic makes use of advanced X- Models (EM-based models), coupled lines and other linear schematic elements, including a substrate definition. This too gives excellent correlation. The "LPF Basic" indicates potential errors in schematic entry with the associated errors in results. A good comparison is achieved among all four designs and validated through circuits and EM sight in AWR MWO Environment, furthermore particular design can be chosen based on tradeoffs. The design will be useful for Satellite and PTP Communications Links, Marine and Pleasure Craft Radar, Port Vessel Traffic Services etc… Design Frequen cy Insertio n loss Return loss VSW R Lumped design 18.14GH z -2.996dB - 16.067d B 1.5 Measured filter 18.659G Hz - 3.0573d B - 18.458d B 10.24 Basic design 18.95GH z - 1.0869d B - 42.441d B 1.029 Advanced design 18.498G Hz - 3.0195d B - 10.001d B 1.826 EM sight design 18.586G Hz -3.039dB - 20.001d B 1.081 References [2] [7] [10] This work Order of the filter 5 4 3 7 Cut-off frequency 2 & 3GHz 7.7GHz 1990MHz 18.95GHz Insertion- loss -0.6dB 18dB <0.6dB - 1.0869dB
  • 7. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 03 Issue: 05 | May-2014, Available @ http://www.ijret.org 318 REFERENCES [1] “A novel design of Narrowband Band pass filters onPTFE laminate using Radial stubs” Pramod, K.B. ; Shyam, S.S. ; Kumaraswamy, H.V. ;Praveen, K.B. Informatics, Electronics & Vision (ICIEV), 2013 International Conference on Digital Object Identifier:10.1109/ICIEV.2013.6572584 Publication Year: 2013 , Page(s): 1 - 6 [2] “Design and Simulation of RF MEMS Switchable Low Pass Filter” M. Jeya Rani, M. Anitha, M. Arul Jothi and S. Kanthamani MEMS Design Center, Department of ECE, Thiagarajar College of Engineering, Madurai, Tamil Nadu ,INDIA. 978-1-4673-1515-9/12/$31.00 ©2012 IEEE [3] “Design and Development of High Gain Wideband Microstrip Antenna and DGS Filters”,by Adel Bedair Abdel-Mooty Abdel-Rahman, IEEE AP-S 2008 [4] “Design Of Compact Microstrip Low-Pass Filter With Ultra-Wide Stopband Using Sirs” L. Wang, H.C.Yang and Y.Li, School of Physical Electronics, UESTC Chengdu, China Vol. 18, 179-186, 2010 [5] “An 880 / 1760 MHz Tunable Bandwidth Active RC Low-pass Filter using High Gain Amplifier” Kijin Kim, Electrical Engineering Department, KAIST 978-1-4673- 2990-3/12/©2012 IEEE [6] “A very linear low pass filter with automatic frequency tuning”, by J. Galán, M. Pedro, T. Sánchez-Rodríguez, F. Muñoz, R. G. Carvajal, and A. López-Martín IEEE TRANSACTIONS ON VERY LARGE SCALE INTEGRATION (VLSI) SYSTEMS, VOL. 21, NO. 1, JANUARY 2013 [7] “A DC to 6 GHz Balanced Elliptic Low-Pass Filter in CMOS 130nm Technology”, by Mohammad S. Mahani, Ramesh Abhari Electrical and Computer Engineering Department, McGill University, Montreal, Quebec, Canada 978-1-4577-1318-7/12/$26.00 © 2012 IEEE. [8] ” A Miniaturized High Out-band Suppression Low-pass Filter Based on the Lumped Circuit Model Using LTCC Technology”, by Xiaoshi Huo and Peng Wang Research Institute of Electronic Science and Technology University of Electronic Science and Technology of China Chengdu China 978-1-4673-1697-2/12/$31.00 © 2012 IEEE. [9] John T. Taylor and Qiuting Huang. CRC handbook of electrical filters. CRC publisher, 1997. [10] “Development of UWB HTS Bandpass Filters With Microstrip Stubs-Loaded Three-Mode Resonator“, by Hiroyuki Ishii, Toru Kimura, Naotaka Kobayashi, Atsushi Saito, Zhewang Ma, and Shigetoshi Ohshima IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, VOL. 23, NO. 3, JUNE 2013 1051-8223/$31.00 © 2012 IEEE [11] Cornelis Jan Kikkert, “A Design Technique for Microstrip Filters”. Electrical and Computer Engineering James Cook University Townsville, Queensland, Australia. [12] J. S. Hong and M. J. Lancaster, “Theory and experiment of novel microstrip slow-wave open-loop resonator filters,” IEEE Trans. Microwave Theory Tech., vol. 45, pp. 2358–2365, 1997.