1206 IEEE ANTENNAS AND WIRELESS PROPAGATION LETTERS, VOL. 11, 2012
The Effect of Electromagnetic Waves on Multilayer
Orthogonal Microstrip Lines With and Without
Defected Microstrip Structure
Mohammad Ali Salari, Seyyedpayam Abbasiniazare, and Omid Manoochehri
Abstract—A method for analysis of multilayer coupled trans-
mission lines with and without defected microstrip structure
(DMS) excited by an external electromagnetic wave is presented.
The structure is first decomposed into coupled transmission-line
sections and crosstalk regions, then a lumped circuit model for the
crosstalk region and the DMS section is presented, and the forced
terms associated with the incident wave are calculated. Finally,
by using the modal decoupling method, the unknown modal
coefficients and subsequently voltages and currents are obtained.
The validity of the method is verified by comparison between the
analytical and the simulated results of HFSS full-wave simulator.
Index Terms—Electromagnetic coupling, incident fields, multi-
layered media, orthogonal microstrip lines.
I. INTRODUCTION
O
RTHOGONAL interconnections can be seen in many
multilayered circuits. This orthogonality decreases the
crosstalk between the interconnections of two adjacent layers.
There exists a vast amount of papers about the coupling of
external electromagnetic waves into transmission lines [1], [2].
A transmission-line method is used in this letter to calculate
the effect of external electromagnetic waves on a multilayer
coupled microstrip lines. The modeling and analysis of the
structure results in practical points that could be exploited in
order to reduce the effect of external electromagnetic waves
at the terminals, e.g., by adjusting the length of the line or the
orientation of the circuit with respect to the source of interfer-
ence (when the source is known for us). Moreover, a method of
analysis is introduced, when there is a defect on the strip like
DMS. The method can be generalized to the other defects like
gap or transverse slit in the microstrip line.
This letter is organized as follows. In Section II, the forced
terms due to an external wave are obtained by primary-sec-
ondary field idea. In Section III, a lumped circuit model for the
crosstalk region and the defected microstrip structure (DMS)
is presented, then the entire structure will be modeled, and the
Manuscript received August 16, 2012; accepted September 25, 2012. Date of
publication October 02, 2012; date of current version October 25, 2012.
M. A. Salari is with the Department of Mathematics, University of Bonn,
Bonn 53115, Germany (e-mail: s6mosala@uni-bonn.de).
S. Abbasiniazare and O. Manoochehri are with the Department of Electrical
and Computer Engineering, Tarbiat Modares University, Tehran, Iran.
Color versions of one or more of the figures in this letter are available online
at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/LAWP.2012.2221453
Fig. 1. Dimensional parameters of a double-layer structure illuminated by a
uniform plane electromagnetic wave. A DMS is placed in the middle of the
lower strip.
matrix equation that relates the crosstalk region’s voltages and
currents is obtained. Finally, the matrix equation that incorpo-
rates all the boundary conditions is given. Section IV describes
the solution of the obtained matrix equation by modal decou-
pling method. In Section V, some examples for normal
incidence are presented.
II. FORCED TERMS DERIVATION
For lossless or low-loss layers, the quasi-TEM assumption
can be applied when the distance between the conductors is
much smaller than the smallest wavelength of propagating
fields. The system in Fig. 1 is assumed to be externally excited
by a uniform plane wave of time dependence . For
simplicity, we assume the following.
1) The principal propagation mode of the lines is quasi-TEM.
2) The strips and ground plane are perfect electric conductors,
the substrate is lossless, and also the thickness of the inter-
connections is assumed to be negligible.
3) The incident electromagnetic (EM) field only excites the
quasi-TEM dominant mode.
4) The ground plane is infinite.
5) The effect of higher-order modes in discontinuities of the
microstrip transmission lines is negligible with respect to
the dominant TEM mode.
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