ebook img

A J Gasiewski remote sensing course notes lecture21 PDF

33 Pages·00.794 MB·English
Save to my drive
Quick download
Download
Most books are stored in the elastic cloud where traffic is expensive. For this reason, we have a limit on daily download.

Preview A J Gasiewski remote sensing course notes lecture21

ECEN 5254 Remote Sensing Signals and Systems Professor Albin J. Gasiewski Lecture #21 – April 3, 2012 ECOT 246 303-492-9688 (O) [email protected] Classes: ECCS 1B14 TR 9:30-10:45 AM 1 ECEN 5254 Remote Sensing Signals & Systems Spring 2012 University of Colorado at Boulder Administration • HW4 solutions posted on D2L • HW5 posted on D2L, due April 10 • Reading: – RSSS slides – Skolnik Chapters 10,11 (on D2L) – Additional references on D2L • Term Paper: – ~10 pages + figures, references – Slide presentations in standard conference format held on Friday, May 4 at end of semester. Schedule to be arranged. – Term paper and slide presentation templates on D2L • Final Exam: Saturday May 5, 7:30-10:00 PM in ECCS 1B14 2 Last Lecture • Sampling, resolution, fringe washing • Noise • Aperture thinning • Intensity correlation (Hanbury-Brown- Twiss Experiment) 3 ECEN 5254 Remote Sensing Signals & Systems Spring 2012 University of Colorado at Boulder Today’s Lecture • Radar principles • Radar cross section • Doppler effect • Correlation receiver • Matched filter • Ambiguity 4 ECEN 5254 Remote Sensing Signals & Systems Spring 2012 University of Colorado at Boulder Radar Principles 5 Received Power - Point Scatterer P G ^ ^ σ(k ,k ) General bistatic T T ^ s i R , k ~ T i radar system: ^ G R ,k R R s P R Received power in steady state: ^ ^ σ(k ,k ) is bistatic s i radar scattering cross section: Depends on λ, size, orientation, and polarization 6 Received Power - Point Scatterer P G ^ ^ σ(-k ,k ) Monostatic T ^ i i R , k ~ i radar system: P R Received power in steady state: ^ ^ σ(-k ,k ) is back- i i scattering cross section: Depends on λ, size, orientation, and P varies as R-4 , G2 : polarization R 7 Radar Cross Section 8 Radar Cross Section Typical RCS values for λ ~ 3 cm wavelength (X-band): ^ ^ σ(-k ,k ) i i RCS increased by:  sharp edges  flat and normal surfaces  high dielectric contrast and/or low loss materials 0.01-0.0002  resonant structures (e.g, λ/2 wires) RCS ~ f 4D6 for electrically small objects, ~(area) for large objects 9 Scattering Coefficients of Hydrometeors f 4a6 Ice Liquid (parameters are sphere radii a in mm) 10

See more

The list of books you might like

Most books are stored in the elastic cloud where traffic is expensive. For this reason, we have a limit on daily download.