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Military Radar Summit Smart Antennas 101 Frank Gross 2/25/15.

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Presentation on theme: "Military Radar Summit Smart Antennas 101 Frank Gross 2/25/15."— Presentation transcript:

1 Military Radar Summit Smart Antennas 101 Frank Gross 2/25/15

2 Relevant Books

3 Examples of “Smart Antennas”
Precision Acquisition Vehicle Entry Phased Array Warning System 450MHz: 1,792 Antennas, kW Detect and Track ICBMs PAVE PAWS

4 Very Large Array (VLA) – New Mexico
74 MHz to 50 GHz 13 mi 82’ 120o

5 HF Antennas/ HAARP Facility
High Frequency Active Auroral Research Program Gakona, Alaska HF: 2.8 – 10MHz / Antennas

6 Active Electronically Steered Array (AESA)
L-Band (1-2 GHz) X-Band (8-12 GHz) F-16

7 Definition of “Smart Antennas”
The term “Smart Antenna” refers to any antenna or array which can adjust or adapt its beam pattern according to a desired criteria. w1 wM w2 y Algorithm d + - Desired signal Suppressed Interference w1 wM w2 y “Dumb” Antenna “Smart/Cognitive” Antenna

8 Smart Antennas can encompass:
Smart Switched Beam Arrays – Butler Matrix, Rotman Lens, Plasma Array Smart Reconfigurable Antennas – Change electrical properties to steer beam Smart Surfaces/Metamaterials – Substrate change causes beam change Smart Vector Antennas – Direction finding with single antenna using polarization Smart Adaptive Arrays – Steer the beam to any direction of interest while simultaneously minimizing/nulling interfering signals

9 Switched Beam Array – Rotman Lens
True Time Delay = Large Bandwidth Beam Direction Feed Rotman Lens Feeding a Vivaldi Array 32 Ports/32 Beams Frontiers in Antennas, 2011 REMCOM Software Rotman Design

10 Applications for Smart Antennas
Beamsteering Jammer Nulling Adaptive Tracking Multipath Mitigation Active Electronically Steered Arrays (AESA)

11 Uniform Linear Antenna Array Modern Steering Vector:
Antenna Array Basics d 2d (N-1)d z Antennas, d  /2 N-Element Uniform Linear Antenna Array Uniform Weights Classic Array Factor: Modern Steering Vector:

12 Uniform Array Weights 30o Equal Gains Across Array Simple Array: Can’t manipulate sidelobes or nulls

13 Second Level of Control
By applying varying scalar weights (gains) to the array elements, we can suppress sidelobes Similar to windowing sampled data in the FFT world Window functions can be Bartlett Hanning Hamming Kaiser-Bessel Dolph-Chebyshev, etc… MATLAB has many of these window functions w1 w2 wM d/2 -d/2 3d/2 -3d/2 (2M-1)d/2 -(2M-1)d/2   

14 Scalar Weight Beamforming
Kaiser-Bessel weights , k = 0,1,... N/2,  > 1 15dB

15 Complex Weight Beamforming
Weights can also include amplitude and phase to allow us to steer the beam to a desired angle 0o o o d = spacing between antennas k = wavenumber = 2/ Beamsteering + Kaiser-Bessel

16 Propagation Over Water
Low flying threats Low grazing angle means highly correlated multipath AOA accuracy is exacerbated by low-angle multipath The evaporation duct can also contribute to multipath Let’s use Maximum Likelihood detection Find the projection of measured data onto a 2-D space of Gram-Schmidt orthonormalized steering vectors. Model glistening rough sea surface Various sea states (SS=0,…,5) Model direct path, specular path, & diffuse path, vertical and horizontal polarization, rms wave height, and rms facet slope. Include divergence factor for curved earth, specular scattering factor, and diffuse scattering factor for rough surfaces Use a vertical sparse array to find direct signal

17 Diffuse and Specular vs. Roughness

18 Like what you see when looking out over the ocean at sunset
Glistening Surface Like what you see when looking out over the ocean at sunset h2 Glistening Surface

19 Total received field The signal received at the kth antenna element is composed of the direct path, specular path, and diffuse path Direct Specular Scattering Diffuse Scattering Where, k= Classic Fresnel reflection coefficient wrt antenna element k D = divergence factor s= specular scattering factor d =.5*(1- s) diffuse scattering factor Rk = specular path length difference to element k Fm = Amplitude function over range of glistening surface m = phase function over range of glistening surface m = discrete glistening flash points

20 Multipath The direct path angle is positive relative to the horizon
Need algorithm to search simultaneously for positive angle direct paths and negative angle multipath direct diffuse specular + - Phased Array

21 Maximum Likelihood Solution to Multipath
Helps tackle highly correlated multipath N element array; D arriving angles kth time sample a = array steering vector

22 Maximum Likelihood Solution to Multipath
Now form the NxD signal matrix. We may now perform the Gram-Schmidt orthonormalization procedure to find D basis vectors sd where d = 1,2,…,D. The S matrix is given as: Where,

23 Maximum Likelihood Solution to Multipath
We define the likelihood function as: Where, We can form the L2-norm of the likelihood function to be

24 Example with 5 Element Array
SS = 5; Known direct angle = Estimated direct angle = 12.50 Maximum Likelihood Surface

25 Example 2: Highly Correlated Multipath
Three frequencies of 2GHz, 8GHz, and 14GHz. 5-element vertical array. Assume direct, specular, and diffuse angles

26 Adaptive Algorithms Adaptive algorithms attempt to minimize a “Cost Function” J(w) The cost function is derived based upon a specified criteria such as Maximum signal-to-interference ratio (SIR) Minimum variance distortionless response (MVDR) Minimum mean-square error (MSE) Constant modulus algorithm (CMA) Once the cost function is defined, various methods can be used to find the minimum either in closed form or by using a recursion relationship

27 Maximum Signal-to-Interference Ratio (SIR)
 0 1 x1(k) x2(k) xM(k) w1* s(k) y(k) w2* wM* N i1 (k) iN (k) ? Let us define the signal-to-interference ratio Power in desired received signal Power in undesired received signal Cost Function

28 Maximum Signal-to-Interference Ratio (SIR)
We can maximize the SIR by taking a derivative of the cost function with respect to the needed weights (amplitude and phase out of HPA) This leads to an eigenvector equation The largest eigenvalue gives the highest SIR The eigenvector solution yields the optimum weights

29 Example of maximum SIR M=10 elements, 0 =300, 1 =-300, 2 =-400, 3 =500 300 -400 500 -300

30 Minimum Variance Distortionless Response (MVDR)
If the array output: We can define the variance as: Where, s = undistorted desired output signal u = undesired interferers

31 Minimum Variance Distortionless Response (MVDR)
Minimizing the cost function we derive the optimum weights Where = covariance matrix of undesired signals +noise = steering vector for desired signal

32 Airborne Cantor Ring Array
3-D Example of MVDR Airborne Cantor Ring Array Nulled Interferers

33 High Altitude Constrained Beams

34 AESA Modern Active Electronically Steered Arrays (AESA) are filled arrays of wideband elements Vivaldi elements Fragmented patch elements The arrays have GaAs T/R modules for every antenna element The cost per element can be $40 to $500 depending on the power demands

35 Applied Radar, Inc. & UMASS
AESA Vivaldi Array Fragmented Patch Array GTRI Applied Radar, Inc. & UMASS Fragmented Aperture 33:1 Bandwidth Vivaldi Array 12:1 Bandwidth

36 Wideband Vivaldi Array
AESA MMIC T/R Modules Wideband Vivaldi Array High-Performance Composite Radome 12-Channel Dual-Pol T/R Module 36

37 Wideband Dual-Pol AESA Antenna
Vivaldi Array Backing Plate T/R Module Housings 3”

38 Low-Cost Phased Arrays
Applied Radar UMASS Design Vivaldi Elements Slant Left/Right Polarizations 24 8 192 elements

39 Low-Cost Phased Arrays
AESA arrays are filled arrays with large numbers of elements Wideband array elements cannot be removed because the inter-element coupling is crucial A template can be devised to thin the array and preserve performance requirements Thinned elements are terminated in dummy loads reducing T/R modules, power demands, heat, $$$

40 Low-Cost Phased Arrays
We can thin the number of active AESA elements? Resolution Uses fewer active elements Side Lobe Levels -15 to -20 dB Robust with 5 or 4-bit phase shifters Use same element phase centers Distinct “thinned” pattern 43% thinning 110 elements not 192

41 Low-Cost Phased Arrays
-13dB -16dB Elevation; 9 GHz; 5-bit phase Azimuth; 9 GHz; 5-bit phase -22dB Robust with 4 or 5-bit phase shifters (11o to 16o) 43% of elements eliminated 43% fewer elements means lower cost Requires ~ 2x HPA power for same ERP

42 AESA Summary Filled Vivaldi Array Challenges
NxM elements, cost, temperature gradients, cooling, weight Thinning is a viable option Array Thinning A novel new approach Uses 43% fewer elements for a 192 element array Reduces total # elements, weight, heat, etc… Performance Produces nearly the same beamwidths with lower sidelobes Thinned array can be weighted/tapered to suppress sidelobes Performs well with 5 bit phase and amplitude quantization

43 Questions?


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