Title: Omid Sotoudeh
1Innovative solutions for Multibeam antenna feeds
- Omid Sotoudeh
- omid.sotoudeh_at_chalmers.se
- Antenna group
2- Overview
- Examiner Prof. Per-Simon Kildal, Chalmers, Head
of Antenna Group - Industrial supervisor Dr. Per Ingvarson, Chief
Engineer Antennas, Saab Ericsson Space - ESA/ESTEC project Innovative solutions for
muti-beam antenna feeds - August 2002 September 2003
- Principal investigator Omid Sotoudeh
- Supervisors Per-Simon Kildal (Chalmers)
- Per Ingvarson (SES)
- Contacts from ESTEC
- Antoine Roederer, Head of Electromagnetics
Division - Cyril Magenot, Head of Antenna and
Sub-Millimeter Wave Section - Arturo Martin-Polegre, Antenna and
Sub-Millimeter Wave Section - Teknisk Licentiat
- O. Sotoudeh, Hard horns for cluster-fed
multi-beam antennas, National Graduate School of
Space Engineering Chalmers University of
Technology, Sweden, February 2004. - Final work in analysis, optimization and design
of single and multi-mode hard horns for cluster
fed multi-beam antennas.
3Ka band multimedia satellites
- New generation of satellite networks
- operating in the Ka-band (20/30 GHz)
- Two way high-speed communications
- A broad range of voice, data and video
communications - Large coverage area (ex Europe, Asia)
- Low Cost
Source  EuroSkyWay program http//www.euroskywa
y.it
4- Cluster-fed multi-beam antennas for Ka-band
- 4 reflector system
- 17.7 20.2 GHz downlink
- 27.5 30.0 GHz Uplink
One of four antennas
Hard horns proposed as feed
20 GHz
Footprint
30 GHz
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5Coverage 4 reflector system
Beam isolation 4 cell reuse scheme
?? 1?
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?d4 2?
- Directivity and directive gain at the weakest
point of the footprint (EOC) - Minimum directive gain level
- Max relative co- and x-pol. between the
neighboring beams - Max x-pol. in own beam
6System requirementsgiven by ESTEC
7Tools used for the analysis and design of horns
- Theoretical formulas based on modes
- Rotational symmetric problems
- Very fast solution
- Rather accurate for design of single mode horns
- Mode-Matching technique
- 2D solver rotational symmetric problems
- Very accurate and fast
- Used for design of horns traditionally
- Commercial 3D SWs (FDTD)
- Slow and demanding
- Accurate
- Used for verification
8Hard horns as feeds in CF-MBA
Horn types and their radiation patterns at center
frequency
d 5? at 30 GHz
Hard horns Dielectric in the corrugations, er
2.44 Wall thickness 0.21?
9Potter/dual mode horns
Smooth walled horns
- TE11 TM11 modes
- Equal E - and H planes Low X - pol
- Low efficiency
- Narrow bandwidth
- TE11 mode
- Difference in E- and H-plane
- High X-pol
- Medium efficiency
- Wide bandwidth
R.H. Turrin, 1966
Potter
10High efficiency horns
- Multimode
- Complex step geometry
- High efficiency (ex. 90 )
- Low X - pol
- Narrow bandwidth
Bhattacharyya et al 2002
11Hard and Soft surfaces
Soft surface Stops field propagation
Hard surface Enhances field propagation
More on these surfaces I recommend P-S, Kildal,
Artificially soft and hard surfaces in
Electromagnetics, IEEE transactions on Antennas
and Propagations, Vol. 38, No. 10, Oct. 1990.
12The hard horn using longitudinal corrugations
- High efficiency
- Low X pol
- Wide bandwidth
- Complex geometry
Conductor (blue region)
Corrugations filled with dielectric
direction of propagation
13Single and multimode hard horns
- Single mode horn with corrugations of constant
depth - Single mode horn with linearly increasing
thickness - Multimode horn with hard wall in an outer section
- Multimode horn combined with a step-shaped mode
exciter to improve the performance at high
frequencies
14Simple single mode hard hornsAnalysed using
asymptotic models
15Study of hard horns Analysis tools
Classical-type model Dominant TEz mode field
distribution
Example d 5? at 30 GHz er 2.5 fTEM
30 GHz
The corrugation period p ltlt ?
1 0
0.6 0
16Multimode hard horns Initial studies Based on
simple manufacturing very simple geometry
Smaller D/t gives shorter L1 Possible for small
radii lt 4-5? Larger apertures need a long PEC
section
- Direct transition from PEC to hard surface
Cylindrical or slightly conical hard surface
Only part of the horn is corrugated
17Dual band multimode hornDesigned using
parametric studiesand Genetic algorithm
optimizationEM solver Mode-matchingTested
with FDTD QW-V2D and QW3D
18Calculated at 19 GHz Tx band
Calculated at 29 GHz Rx band
19Horn performance 2D simulations
Aperture efficiency ()
Return-loss (dB)
Max cross-polar level (dB)
Frequency (GHz)
Frequency (GHz)
Frequency (GHz)
20Total antenna performance in BOR reflector
Directive gain
Co polar BI
Max rel. cross pol in own beam
Cross polar BI
21Hard horn measurements at SES
22Horn performance measurements and MM ? High
sidelobes in E-plane
23Horn performance measurements and MM and 3D
FDTD(40 corrugations)?The 3D simulations agree
with the measurements
24Horn performance measurements and MM and 3D
FDTDN 40 and 80 corrugations?The 3D
simulations of N 40 agree with the
measurements? N 80 and tooth thickness 0.4 mm
agrees with asymptotic design
25Comparison of designs
Best single mode design Ltot 47 cm, corrugated
Lcorr 47 cm
Best multi-mode design Ltot 30 cm, corrugated
Lcorr 22 cm
26Conclusions
- Studies of hard walled horn antennas
- The hard walls may be used in horn antennas in
order to enhance their performance. - They can be designed as single mode hard horns or
multimode hard horns. - A dual band multi-mode hard horn has been built
and measured for 20/30 GHz Ka-band operation. - Horn designed using fast Mode-Matching.
- Present design is smaller than previous single
mode horns and much more simple to manufacture. - Discrepancies with measurements have been
explained. - For present design we need more than 40
corrugations and lt 0.5 mm corrugation tooth
thickness. - We can use the fast mode-matching codes in the
future for design of these horns. - Future work More on the effect of corrugations
on the hard horn performance and their optimal
dimensions for our hard horn design is being
studied at the moment.
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28Horn parameters
29BOR reflector model
- Rotationally symmetric reflector, and neglected
feed blockage (offset reflectors) - Horns in the focal point of reflector
- Aperture integration method
- Short computational time
- Very fast for parametric studies
- Quite accurate and relevant results
30Theory of BOR, Body of revolution
Aperture fields vertical polarization
Total
BOR1 component
31Theory of BOR, Body of revolution
Far-fields vertical polarization
Total
BOR1 component
32Theory of BOR, Body of revolution
BOR1 relations for RHCP Far-field functions
Aperture field functions
(see e.g. Kildals textbook, Foundations of
Antennas)
33Hard horn analysis Performance as a function of
frequency
Ex d 5?TEM, LH 15 ?TEM, fTEM 31.8 GHz
TE11
TE11
er 5, t 1.2 mm
er 5, t 1.2 mm
er 2.5, t 1.9 mm
er 2.5, t 1.9 mm
eap ()
er 1.5, t 3.2 mm
er 1.5, t 3.2 mm
Max xp level (dB)
er 1.25, t 4.5 mm
er 1.25, t 4.5 mm
Frequency (GHz)
Frequency (GHz)
Frequency (GHz)
34Hard horn analysis Performance as a function of
length
Ex d 5?TEM, f fTEM 31.8 GHz
TE11
er 5, t 1.2 mm
er 1.5, t 3.2 mm
er 1.25, t 4.5 mm
er 2.5, t 1.9 mm
TE11
er 1.5, t 3.2 mm
eap ()
er 1.25, t 4.5 mm
er 2.5, t 1.9 mm
Max xp level (dB)
er 5, t 1.2 mm
Length (mm)
Length (mm)
35Comparison mode-matching classical-type er
1.25, d 5? at 17.7 GHz, fTEM 30.5 GHz LH
25? at 17.7 GHz 424 mm LE 376 mm
Ideal design
Realizable design
36Optimum D 1.25 m, F 1.86 m, subtended semi
angle 19
Horn patterns
Reflector patterns