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Effect of slow wave structures on scan angles in microstrip Leaky-Wave Antennas The 36th PIERS - 2015 Prague, Czech Republic Semnan University Semnan, I. R. Iran BY: S. Mohammadpour Jaghargh, P. Rezaei, J. S. Meiguni E-MAIL: [email protected] Forum for Electromagnetic Research Methods and Application Technologies (FERMAT) *This use of this work is restricted solely for academic purposes. The author of this work owns the copyright and no reproduction in any form is permitted without written permission by the author. *

Semnan University The 36th PIERS - 2015 Prague, Czech Republic … · 2017. 1. 16. · leaky-wave antenna with metamaterial unit cell and slow-wave structure,” 1st national conf

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  • Effect of slow wave structures on scan angles in microstrip

    Leaky-Wave Antennas

    The 36th PIERS - 2015

    Prague, Czech RepublicSemnan University

    Semnan, I. R. Iran

    BY:

    S. Mohammadpour Jaghargh, P. Rezaei, J. S. MeiguniE-MAIL: [email protected]

    Forum for Electromagnetic Research Methods and Application Technologies (FERMAT)

    *This use of this work is restricted solely for academic purposes. The author of this work owns the copyright and no reproduction in any form ispermitted without written permission by the author. *

  • Abstract

    2

    This paper presents two miniaturized slow wave structures in

    microstrip leaky-wave antennas (MLWAs) which operate about 8

    GHz. The effects of these structures on the scan angles have been

    compared in the paper. The designed interdigital capacitors and

    folded-back line have been investigated with ADS Momentum

    software. It has been shown that the interdigital capacitors (IDCs)

    yield to a broad scan angles from +53 to -74 degree, while the folded-

    back line inductor scans only the positive angles.

    Index Terms—leaky-wave antenna (LWA), scan angle, slow

    wave structure, periodic structure.

  • Contents• Introduction

    • History

    • Classification

    • Recent attention

    • Introduction to Slow wave structure

    • Topologies of proposed LWAs

    • Properties of proposed LWAs

    • Effects of slow wave structure on scan angles and Results

    • Conclusion

    • References

    The 36th PIERS - 2015

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    3

  • IntroductionDefinition of Leaky Wave Antennas (LWA)

    LWA is guiding structure that supports wave propagation along it.

    Waves are leaking along it continuously.

    Application: light and speedy vehicle, missile, plane and automotive Radar.

    LWA is travelling wave and non-resonant antenna.

    The 36th PIERS - 2015

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    4

  • IntroductionAdvantages of LWAs

    High directivity.

    Simple and cheap structure.

    Not-complicated feed network.

    Ideally suits for frequency beam scanning applications (Beam scans with frequency inherently).

    So popular in Microwave and millimeter bands.

    Semnan University

    Semnan, Iran

    5

  • Narrow pattern beam width ≈ (1% to 10%).

    So, not appropriate for Point-to-Point

    communication.

    IntroductionDisadvantages of LWAs

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    6

  • History of LWAs• Started at 1940s.

    • Introducing as slotted rectangular waveguide.

    • Some prototype LWA structures, See below!

    Honey LWA-1959

    Dimensions: 46-61 cm

    7-13 GHz

    Transverse resonance method

    Φ(f)

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    7

  • LWA

    2-Dimension 1-Dimension

    Uniform /

    Quasi-uniformPeriodic

    Classification of LWAs

    LWA

    Unidirectional case

    (Feed at one side)

    Bidirectional case

    (Feed at center)

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    • Classification based on feed location (Right chart)

    • Classification based on wave propagating (Left chart)

    8

  • Classification of LWAsBased on feed location

    Figure (a): Unidirectional case (Feed at one side)

    Figure (b): Bidirectional case (Feed at center): So useful because of creating beam at broadside.

    9

    Semnan University

    Semnan, Iran

  • Classification of LWAsBased on wave propagating

    1D: Wave is guided in 1 directional.1) Uniform (or Quasi-uniform): Guiding structure is uniform along length

    (support fast waves, 0< β < k0 ).

    2) Periodic: Non-radiating changes to radiating by periodic

    structures (support slow wave, β > k0).

    2D: Wave is propagated on 2D guiding

    surface.10

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  • Recent Attention on LWA

    Full space scanning continuously.Means: full-space continuous beam scanning, from backfire to endfire, including the broadside direction.

    Create broadside beam by bidirectional LWA.

    Overcoming the “open stop band” problem.

    Power recycling to avoid wasting non-radiated power.

    LWA for curved surface.

    11

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  • Slow wave structures (SWSs)

    • Controlling and handle the wave

    velocity in certain direction.

    • SWS is non-resonant circuit.

    • SWS is designed for producing large

    gain antennas.

    12

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  • Some slow wave structures• Zigzag line

    • Corrugated waveguide

    • Helical line

    • Folded-back line inductor

    • Interdigital capacitor (IDC)

    13

    The 36th PIERS - 2015

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    Interdigital Capacitor (typical IDC) Folded back line inductor

    Effects of them on scan angles in

    LWA will be investigated.

  • Unit cell of each proposed LWAs

    143D view of proposed LWA with periodic folded-back line.

    3D view of proposed LWA with periodic IDC.

    Unit cell of folded-back line

    Unit cell of IDC

    Zoom in

    Zoom in

  • 3D view of 16-cell periodic LWAs

    15

    3D view of LWA with IDCs formed by 16 cells. 3D view of LWA with folded-back line formed by 16

    cells.

  • Properties of proposed LWAs

    16

    Property LWA with IDCs LWA with folded back

    Type of LWA CRLH RH

    Fabrication Technology Microstrip Microstrip

    Number of cells 16 16

    Frequency band analyzing X-band X-band

    Dimensions of unit cell 4.5mm * 4mm 4.5mm * 4mm

    Dimensions of 16-cell 4.5mm * 64mm 4.5mm * 64mm

    Substrate and height Rogers 5880, h = 0.508mm Rogers 5880, h = 0.508mm

    Ԑr of substrate 10.2 10.2

    Semnan University

    Semnan, Iran

  • Results of radiation pattern and scan

    angles for both MLWAs

    17

    -100 -80 -60 -40 -20 0 20 40 60 80 100-100

    -80

    -60

    -40

    -20

    0

    20

    Theta (degree)

    Ga

    in (

    dB

    )

    Pattern at 8GHz

    Max gain at 9.285GHz

    Pattern at 10.363GHz

    13.393 dB 12.066 dB

    +53-18-74

    17.647 dB

    -100 -80 -60 -40 -20 0 20 40 60 80 100-100

    -80

    -60

    -40

    -20

    0

    20

    Theta (deg)

    Ga

    in (

    dB

    )

    Pattern at 8GHz

    Pattern,Max gain at 8.714GHz

    +3 +54

    11.236 dB

    2.106 dB

    Radiation pattern of LWA with IDC Radiation pattern of LWA with folded back

  • Other Results

    18

    7.5 8 8.5 9 9.5 10 10.5

    -80

    -60

    -40

    -20

    0

    20

    40

    60

    Frequency (GHz)

    Sc

    an

    an

    gle

    (d

    eg

    ree

    )

    LWA with Folded back line

    LWA with Interdigital

    -77 deg

    +53 deg +54 deg

    +3 deg

    Scan Intervalfor Foldedback line

    Scan Interval for Interdigital

    8.714 7.5 8 8.5 9 9.5 10 10.5-10

    -5

    0

    5

    10

    15

    20

    Frequency (GHz)

    Ga

    in (

    dB

    )

    LWA with Folded back line

    LWA with Interdigital

    Average for Interdigital

    Average for Folded back line

    5.93 dB

    14 dB

    Details of scan angles in both proposed

    LWAs when frequency changes.

    Details of magnitude of the gain in both

    proposed LWAs when frequency changes

    and the average of gains in interval of scan.

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  • Magnitude of S-parameter

    19

    8 8.5 9 9.5 10 10.5 11-30

    -25

    -20

    -15

    -10

    -5

    0

    Frequency (GHz)

    Ma

    gn

    itu

    de

    of

    S-p

    ara

    me

    ter

    (dB

    )

    S11 of IDC S12 of IDC S12 of Folded back S11 of Folded back

    Red lines: S-Parameter for LWA with IDCs

    Blue lines: S-Parameter for LWA with folded-back line

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  • Comparative results and conclusion

    Replacing an Interdigital capacitor with a folded back line inductor in this letter.

    LWA with Folded back line scans only positive angles (Forward radiation).

    20

    Name of

    antenna

    Scan Freq

    (GHz)

    Scan angles

    (deg) in Φ= 0̊

    plane

    Max gain

    (dB)

    Forward /

    backward

    radiation

    descriptions

    LWA with

    IDC8 to 10.36 -74 to +53 17.64 Yes / Yes CRLH

    LWA with

    folded back8 to 8.71 +3 to +54 11.23 Yes / No RH

  • References

    [1] D. R. Jackson and A. A. Oliner, Leaky-wave antennas in modern antenna handbook, New York: Wiley, 2008.

    [2] C. Caloz, D. R. Jackson, and T. Itoh, “Leaky-wave antennas,” IEEE Trans. Antennas Propag., vol. 100, no.7, pp.

    2194-2206, July 2012.

    [3] V. Nguyen, A. Parsa, and C. Caloz, “Power-recycling feedback system for maximization of leaky-wave antennas

    radiation efficiency,” IEEE Trans. Microw.Theory Tech., vol. 58, no. 7, pp. 1641-1650, July 2010.

    [4] R. C. Honey, “A flush-mounted leaky wave antenna with predictable patterns,” IRE Trans. Antennas Propag., vol. 7,

    pp. 320-329, Oct. 1959.

    [5] S. Y. Liao, Microwave devices and circuits, New Jersey: Prentice Hall, 1990.

    [6] S. S. Gevorgian, T. Martinsson, P. L. J. Linner and E. L. Kollberg, “CAD models for multilayered substrate

    interdigital capacitor,” IEEE Trans. Microw. Theory Tech., vol. 44, no. 6, pp. 896-904, June 1996.

    [7] N. Amani, M. Kamyab, A. Jafargholi, A. Hosseinbeig and J.S. Meiguni, “Compact tri-band metamaterial-inspired

    antenna based on CRLH resonant structures,” Electronic Letts., vol. 50, no. 12, pp. 847-848, June 2014.

    [8] S. Mohammadpour Jaghargh, P. Rezaei and J. S. Meiguni, “Simulation and design of a novel K-band microstrip

    leaky-wave antenna with metamaterial unit cell and slow-wave structure,” 1st national conf. Development of civil

    eng. Archetecture, electricity and mechanichal in Iran., Gorgan, Iran, Dec 2014.21

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  • References

    [9] G. F. Cheng and C. K. C. Tzuang, “Closely coupled half-width leakywave antenna array,” 6th European Conf. Antennas and Propag., pp. 957-960, 2012.

    [10] J. Liu, D. R. Jackson, and Y. Long, ”Substrate integrated waveguide (SIW) leaky-wave antenna with transverse slots,” IEEE Trans. Antennas Propag., vol. 60, no. 1, pp. 20-29, Jan. 2012.

    [11] C. Calm, T.Itoh, and A.Renning, “CRLH metamaterial leaky-wave and resonant antennas,” IEEE Antennas Propag. Mag., vol. 50, no.5, pp. 25-39, Oct. 2008.

    [12] Y. Li, Q. Xue, H.z. Tan, and Y. Long, “The half-width microstrip leaky wave antenna with the periodic short circuits,” IEEE Trans. Antennas Propag., vol. 9, no. 9, pp. 3421-3423, Sept. 2011.

    [13] A. Pourghorban Saghati, M. Mirsalehi and M.H. Neshati, “A HMSIW circularly polarized leaky-wave antenna with backward, broadside, and forward radiation,” IEEE Antennas and Wireless Propag Letts., vol. 13, pp. 451-454, Mar. 2014.

    [14] S. Paulotto, P. Baccarelli, F. Frezza1 and D. R. Jackson, “A microstrip periodic leaky-wave antenna optimized for broadside scanning,” Antennas and Propag. Society International Symposium IEEE, pp. 5789-5792, 2007.

    [15] A. Sutinjo, M. Okoniewski and R. H. Johnston, “Radiation from fast and slow traveling waves,” IEEE Antennas Propag. Mag., vol. 50, no. 4, pp. 175-181, Aug. 2008.

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