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MULTI-FREQUENCY AND ULTRA-WIDEBAND ANTENNA RADOMES

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MULTI-FREQUENCY AND ULTRA-WIDEBAND ANTENNA RADOMES Dr. D .J. Kozakoff Marietta, GA, USA * Approach 3: Pyramidal inner walls Bandwidth of 10:1 or greater potential. – PowerPoint PPT presentation

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Title: MULTI-FREQUENCY AND ULTRA-WIDEBAND ANTENNA RADOMES


1
MULTI-FREQUENCY AND ULTRA-WIDEBAND ANTENNA RADOMES
  • Dr. D .J. Kozakoff
  • Marietta, GA, USA

2
Radome
  • A dielectric (RF transparent) cover placed over
    an antenna in order to protect it from the
    environment
  • A technology spin off of WWII

3
Reasons for its Development
  • The maximum speed of an aircraft is limited to
    the speed at which external antennas are able to
    survive.
  • In WWII a plastic cover over a B18 bombers radar
    antenna was the first known application
  • Today, in what applications are radomes used?

4
Maritime Applications
  • Ocean Liners
  • Small Craft

5
Telecon Applications
  • Parabolic Reflector Antennas
  • Hog Horn Antennas

6
Radar and SATCOM Applications
  • Air Traffic Control
  • SATCOM

7
Aircraft and Missile Applications
8
Vehicular Applications
9
Cell Telephone Tower Antennas
10
As a Structure to Conceal an Enclosed Microwave
Communications Antenna
  • Antenna Within Structure
  • External view

Concealfab Corp.
11
As a Structure to Conceal an Enclosed SATCOM
Antenna
Concealfab Corp.
12
Revise the last Question
  • Are there applications where radomes not used?
  • Not many!!!

13
Bottlenecks to Consider
  • Within a radome, the system bandwidth is limited
    by the radomes bandwidth.
  • The noise floor (system noise temperature) cannot
    be less than radome noise temperature
  • (in the order of 10o K for every 0.1 dB
    loss.)
  • The radome depolarization limits the dynamic
    range in a frequency reuse application.

14
Reciprocity
What a Radome does in the transmitting mode, it
does exactly the same thing in the receiving mode
(For instance, if a radome had 1 dB of
transmission signal loss, it would also attenuate
the received signal by 1 dB.
15
Parameters that Impact Broadband Performance
  • Wall thickness (thin is generally better)
  • Wall design number of layers, thickness,
  • and permittivity of each layer (more layers
  • is better.)
  • Shape (flatness is desirable)
  • Selection of low loss materials (small loss
  • tangent is required).

16
Definition of Walls Types
e1
e1
e2
e1
e1
e1
e2
e2
Monolithic
A or B
C
B-Sandwich e1 lt
A-Sandwich e1 gt e2
C-Sandwich e1 gt e2
17
Radome Wall Details
18
Multifrequency or Ultrabroadband Approaches in
Current Use Thin Wall Radomes
19
Monolithic Walls
  • Walls that are any multiple of a half wave must
    be precluded because these are narrow band.
  • Any wall that is thin in terms of wavelength is
    ultrabroadband but
  • - generally has poor mechanical strength.
  • - has a loss almost entirely due to
    reflection (loss tangent value is of little
    importance)

20
Approximate loss versus thickness
21
Inflatable Thin Wall Radome Example
22
Multifrequency or Ultrabroadband Approaches in
Current Use Computer OptimizedMultilayer Wall
Designs
23
Computer optimization of multi-wall radomes
considerations
  • Iterate all possible layer thicknesses in half
    ply
  • (6 mil) increments
  • Coarse search followed by a fine search and use
  • of convergence algorithms was important when
  • computers were slow (4 MHz)
  • Brute force search through all combinations is
  • feasible with todays high speed PC computers
  • (2 GHz )
  • Optimized solutions are not unique, that is
    various
  • combinations of wall thicknesses may suffice

24
Multilayer Computer Optimization Procedure
  • Describe wall type and max and min thicknesses of
    each layer
  • Input layer dielectric constants and loss
    tangents
  • Define performance desired in each frequency
    range
  • Iterate radome transmission calculations until
    acceptable performance is achieved.

25
Multifrequency or Ultrabroadband Approaches in
Research or Development
26
Approach 1 Matched Materials Wave Impedance of
a Radome Material
  • Where
  • Relative permeability
  • Relative permittivity

27
Approach 1 Matched Materials
  • If the relative permittivity of a radome
    material is equal to its relative permeability
    then the intrinsic impedance is the same as the
    intrinsic impedance of free space and there is no
    radome reflection loss.
  • Materials with a relative permeability greater
    than one do not yet exist above about 1 GHz
  • (above 1 GHz the only practical matched
    material approach is a radome material both
    relative permittivity and relative permeability
    close to 1).

28
Approach 1 Structual Foam SATCOM Radome Example
29
Summary for Matched Materials Approach
  • Materials development needed to find a material
    with a relative permeability greater than 1 above
    1 GHz. (This could be incorporated with a
    standard dielectric using dielectric mix formulas
    in order to achieve a matched material).

30
Approach 2 Metamaterials
  • Metamaterials are periodic structures that
  • Exhibit a negative refractive index
  • Microwave metamaterials are usually
  • constructed as arrays of electrically conductive
  • elements which have suitable reactance
  • characteristics.
  • Passive circuits.
  • (Note metamaterial core
  • could replace standard
  • Honeycomb core in an A
  • Sandwich radome.)

31
Metamaterial Radome Features
  • A dielectric layer and adjacent to a suitable
  • metamaterial used as a radome.
  • The structure may be non-reciprocal for
  • incoming and outgoing waves.
  • Metamaterial radomes can improved power
  • Transmission over a broad range of antenna
  • scan angles.

32
Metamaterial Radome Features
  • Metamaterial radomes can enhance out of
  • band signal rejection.
  • Commercial metamaterial radomes are not
  • yet state-of-the-art.
  • Metamaterials are useful for multi-band
  • Radomes.
  • Metamaterials ultra wideband radomes (TBD).

33
Metamaterial References
  • Use of conjugate dielectric and metamaterial
    slabs as
  • radomes, Microwaves, Antennas Propagation
  • IET, ISSN 1751-8725, pp.1751-8725, Feb 2007
  • Oraizi, H. and M.Afsahi, Design of Metamaterial
  • Multilayer Structures as Frequency Selective
  • Surfaces, Progress in Electromagnetics Research
    C,
  • Vol.6, pp.115-126, 2009
  • Wu, C., H. Lin and J.Chen, A novel low profile
    dual
  • Polarization metamaterial antenna radome design
    for
  • 2.6 GHz WiMAX, 3rd International Congress on
    Advanced
  • EM Materials and Optics, 2009

34
Approach 3 Pyramidal inner walls
  • Bandwidth of 101 or greater potential.
  • Performance demonstrated in lab tests over 0 to
    60 deg angle of incidence.
  • Excellent circular pol. characteristics.
  • This approach has not yet known to have been used
    in any commercial application.

35
Pyramidal inner walls reference
Bassett,H. L., D.G.Bodnar, G.K.Huddleston and
J.M.Newton, Broadband Radome Techniques,
AD0920772, Engineering Experiment Station,
Georgia Institute of Technology, Atlanta, GA, 1974
36
Approach 4 Active Radomes
  • Reconfigurable frequency pass bands and frequency
    reject bands.
  • Lightweight and low loss.
  • An outgrowth of meta-materials technology.

37
Summary
  • Current technology thin wall radomes meet
    electrical requirements for ultra wideband
    transmission, but not necessarily meet mechanical
    requirements.
  • Current technology computer optimized multi-wall
    radomes using state of the art materials are
    realizable but very expensive.
  • Matched material (Approach 1) requires material
    development break thru to use above 1 Ghz.

38
Summary (continued)
  • Approach 2 (Pyramidal surface matching) has been
    demonstrated in the lab but not yet been
    commercialized.
  • Approach 3 (Meta-materials radomes) are passive
    and are in current research.
  • Active radomes (Approach 4) are envisioned as a
    future development offering enhanced features and
    capabilities.

39
Thank you for your time in listening to this
presentation. Have a good day.
D.J.Kozakoff dr.kozakoff_at_usdigicomm.com
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