Invention Grant
US07656342B2 Double-sideband suppressed-carrier radar to null near-field reflections from a first interface between media layers
失效
双边带抑制载波雷达从媒体层之间的第一接口进行无效近场反射
- Patent Title: Double-sideband suppressed-carrier radar to null near-field reflections from a first interface between media layers
- Patent Title (中): 双边带抑制载波雷达从媒体层之间的第一接口进行无效近场反射
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Application No.: US11877655Application Date: 2007-10-23
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Publication No.: US07656342B2Publication Date: 2010-02-02
- Inventor: Larry G. Stolarczyk , Igor Bausov , Richard B. Main
- Applicant: Larry G. Stolarczyk , Igor Bausov , Richard B. Main
- Applicant Address: US NM Raton
- Assignee: Stolar, Inc.
- Current Assignee: Stolar, Inc.
- Current Assignee Address: US NM Raton
- Agent Richard B. Main
- Main IPC: G01V3/12
- IPC: G01V3/12 ; G01S13/89 ; G01S13/32

Abstract:
A ground-penetrating radar comprises a software-definable transmitter for launching pairs of widely separated and coherent continuous waves. Each pair is separated by a constant or variable different amount double-sideband suppressed carrier modulation such as 10 MHz, 20 MHz, and 30 MHz Processing suppresses the larger first interface reflection and emphasizes the smaller second, third, etc. reflections. Processing determines the electrical parameter of the natural medium adjacent to the antenna.The modulation process may be the variable or constant frequency difference between pairs of frequencies. If a variable frequency is used in modulation, pairs of tunable resonant microstrip patch antennas (resonant microstrip patch antenna) can be used in the antenna design. If a constant frequency difference is used in the software-defined transceiver, a wide-bandwidth antenna design is used featuring a swept or stepped-frequency continuous-wave (SFCW) radar design.The received modulation signal has a phase range that starts at 0-degrees at the transmitter antenna, which is near the first interface surface. After coherent demodulation, the first reflection is suppressed. The pair of antennas may increase suppression. Then the modulation signal phase is changed by 90-degrees and the first interface signal is measured to determine the in situ electrical parameters of the natural medium.Deep reflections at 90-degrees and 270-degrees create maximum reflection and will be illuminated with modulation signal peaks. Quadrature detection, mixing, and down-conversion result in 0-degree and 180-degree reflections effectively dropping out in demodulation.
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