• Title/Summary/Keyword: HPS(Hongik Polarimetric Scatterometer)

Search Result 4, Processing Time 0.017 seconds

Design of a Full Polarimetric Scatterometer for X-Band (X-밴드용 완전 편파 Scatterometer 설계)

  • Hwang, Ji-Hwan;Lee, Kyung-Yup;Park, Seong-Min;Oh, Yi-Sok
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
    • /
    • v.20 no.12
    • /
    • pp.1308-1315
    • /
    • 2009
  • A full-polarimetric scatterometer(HPS: Hongik Polarimetric Scatterometer) for X-band is designed, fabricated, and verified using the theoretically well-known point-targets in this paper. The X-band full-polarimetric scatterometer consists of an OMT(Orthogonal-Mode Transducer)+horn antenna, the angle control part for the OMT+horn antenna, a transmitter/receiver with a network analyzer and a frequency-conversion circuitry, and a movable support of these parts. We use an inclinometer sensor to control the vertical and horizontal incidence angles. The full polarimetric data can be obtained because of the polarization switches and the OMT. The accuracy of the scatterometer system is verified by measuring the polarimetric RCS(Radar Cross Section) of one of the theoretically well-known point-targets, i.e., a corner reflector.

Verification of a Calibration Technique for a Full-Polarimetric Scatterometer System at C-band (C-밴드 완전 편파 측정용 스캐터미터 시스템 보정 기술 검증)

  • Park, Sin-Myeong;Go, Joo-Seoc;Joo, Jeong-Myeong;Kim, Hee-Young;Kim, Ju-Hui;Hwang, Ji-Hwan;Kwon, Soon-Gu;Shin, Jong-Chul;Oh, Yisok
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
    • /
    • v.23 no.10
    • /
    • pp.1196-1203
    • /
    • 2012
  • This paper presents a study on the calibration of a C-band HPS(Hongik Polarimetric Scatterometer) system using the DMMCT(Differential Mueller Matrix Calibration Technique). For calibration of the polarimetric scatterometer system, a fully-polarimetric antenna pattern(magnitudes and phase-differences) of the antenna main-beam is measured using a conducting sphere at anechoic chamber. The polarimetric scatterometer system could be accurately calibrated after retrieving its distortions using the DMMCT. Unlike a single-polarimetric system, in a fully-polarimetric system, not only backscattering coefficients but also phase differences are important parameters. This calibrated HPS system can be used to measure accurate Mueller matrices of bare soil surfaces, rice paddies, and vegetation fields. The phase-difference parameters as well as the backscattering coefficients for co- and cross-polarizations can then be obtained. The accuracy of calibration was verified by comparing the measured backscattering coefficients with a scattering model. The measured polarization response of a plowed bare field was also compared with the polarization response which was synthesized using a polarimetric scattering model for verifying the calibration technique.

Study on the Calibration of a Full-Polarimetric Scatterometer System at X-band (X-밴드 완전 편파 Scatterometer 시스템 보정에 관한 연구)

  • Hwang, Ji-Hwan;Park, Seong-Min;Kwon, Soon-Gu;Oh, Yi-Sok
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
    • /
    • v.21 no.4
    • /
    • pp.408-416
    • /
    • 2010
  • A study on the calibration of an X-band HPS(Hongik Polarimetric Scatterometer) system for ground-based operation is presented in this paper. In order to calibrate the scatterometer system, the degree of its distortions are analyzed by comparison between theoretical- and measured-values using the theoretically well-known calibration targets such as a metal sphere, a trihedral corner reflector(CR) and a metal cylinder. The calibration works in the field conditions depend on the precise and stable measurements of those calibration target. we present a measurement technique, so-called, an automatic 2-D target-scanning technique, using the incidence-angle(${\xi}-$ and ${\phi}-$ directions) control of HPS system. Then, we used STCT(Single-Target Calibration Technique) and GCT(General Calibration Technique) to calibrate a distortion of the scatterometer system, and measured the polarimetric RCS(Radar Cross Section) and phase-difference of a trihedral-CR as a test-target to verify the accuracy of the calibration technique. Then, three different types(i.e., 10, 20, 30 cm) of trihedral-CR were used. we obtained the error ranges about ${\pm}1.0$dB, ${\pm}0.5$ dB in a polarimetric RCS and about $-20^{\circ}{\sim}0^{\circ}$ and ${\pm}5^{\circ}$ in the co-polarized phase-difference by using the GCT and STCT, respectively.

Ground-Based Rotational SAR System for Field-Experiments (지상 운용 회전형 SAR 시험용 시스템 연구)

  • Hwang, Ji-Hwan;Kwon, Soon-Gu;Shin, Jong-Chul;Oh, Yi-Sok
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
    • /
    • v.22 no.11
    • /
    • pp.1092-1100
    • /
    • 2011
  • A C-band ground-based rotational SAR system is presented in this paper. The rotaional SAR system is a test-bed for future rotational SAR systems which can be deployed in space and on a tower. The test-bed system is designed for imaging the electromagnetic scattering from earth surfaces and buried targets. This paper also presents the examination results of the generated SAR images. This rotational SAR system is basically consisted of the network-analyzer based HPS(Hongik Polarimetric Scatterometer) and a horizontally rotating arm. Several SAR images were obtained using the rotational SAR system for various target areas. To verify this system, we simulated the SAR images for the rotational SAR using the FDTD algorithm and compared between the measured and simulated SAR images. The rotational SAR system is operated at the center frequency of 5 GHz and various frequency bandwidth within 0.5~2 GHz to change the resolution of SAR images.