Metal-Dielectric Radomes Windows SUMMARY Novel thick radomes loaded with periodic array of...
Transcript of Metal-Dielectric Radomes Windows SUMMARY Novel thick radomes loaded with periodic array of...
New Metal-Dielectric Window
The basic design is a thick dielectric slab with a central periodic array of conducting inclusions
Dielectric layer thickness is about 0.75
Array spacing and inclusion size are optimized for maximum transmission
Unit-cell of the Periodic Structure
Total thickness :
8.8 mm
Dielectric –polyimid
Eps=3.5
Tangent-loss=
0.0027
Unitcell d=3mm
Bandwidth Dependence on
Dielectric Constant
Typical bandwidth at -0.5db Transmission
loss :
=2.2 BW= 66%
=4.4 BW= 40%
=9.2 BW= 28%
Internal Grating Lobes
Unitcell size d< wavelength-in-air/2 to
avoid external grating lobes
But we must avoid unitcell size d<
wavelength-in-dielectric/2 to avoid internal
grating lobes that resonate
We check d=8mm, r=1.7mm
THz Window
Two layers of scatterers
Periodic grid of sub-resonant
scatterers
Dielectric constant – 2.94
Total thickness 0.762 mm
=> 1.5 wavelength at 0.35 THz
Metal via : diameter =0.11mm
height=0.127mm ,
periodicity= 0.2mm
Radome Performance
Radome size 54X54 unit-cells,
10.8X10.8 mm
The radome is in the quasi-far
-field of the horn
Horn aperture is about 2X2
Wavelengths
T_solver is used
14.2Mcells
Compensation of Thick Skins
Metal inclusions allow the use of thick
skins in a composite radome.
Ku radome design with 5mm foam core
and two skins (r=4.3) of thickness
t=1mm.
Radome with Thick Skins
- Geometry
d= 6mm
Skins 1mm thick
eps=4.3
Core 5mm thick
Eps=1.2
Printed circular patches
Metal-Dielectric Windows
SUMMARY
Novel thick radomes loaded with periodic array
of sub-resonant conducting inclusions are
presented.
The conducting inclusions allow the tuning of all
dielectric discontinuities.
The method offers many degrees of freedom in
the design.
This metal-dielectric technology is patented.