antenna systems Search Results


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Metawave Communications Corp narrow-beam smart antenna system
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Menlo Systems emitter antenna tera 15-tx-fc
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Trimble Navigation real-time kinematic gps system trimble rtk 5700 with zephyr geodetic antenna
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TOPTICA Photonics ingaas-based emitter antenna
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Morishita Jintan folded antenna system
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Geophysical Survey Systems Inc 1.5 ghz antenna model
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SAS institute shared antenna system
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Geophysical Survey Systems Inc 400 mhz antenna (type: 50400s)
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Electro-Optics Technology Inc optical system/antenna
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Nearfield Systems Inc array antennas
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Advanced Telemetry Systems Inc yagi directional antennas
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Nearfield Systems Inc srr antennas
The effect of rotation on the reflection coefficient measured by the monopole interaction <t>with</t> <t>nearfield</t> <t>SRR</t> antenna. The x-axis is parallel to the monopole, with the outer split upward and in plane of the SRR at θ x = 0 , θ y = 0 , a n d θ z = 0 —see . Spectra from a 433 MHz antenna design when rotated ( a ) about the x-axis θ x ( θ y = 0 , θ z = 0 ) and ( b ) the peak reflection coefficient rotated about θ x . ( c ) Spectra when rotated about the y-axis θ y ( θ x = 0 , θ z = 0 ) and ( d ) the peak reflection rotated about θ y . ( e ) The peak reflection value rotated about θ z ( θ x = 0 , θ y = 0 ) with the xy-plane aligned to the monopole (z-axis normal to the monopole). The general fit is overlaid as a dash line.
Srr Antennas, supplied by Nearfield Systems Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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Image Search Results


The effect of rotation on the reflection coefficient measured by the monopole interaction with nearfield SRR antenna. The x-axis is parallel to the monopole, with the outer split upward and in plane of the SRR at θ x = 0 , θ y = 0 , a n d θ z = 0 —see . Spectra from a 433 MHz antenna design when rotated ( a ) about the x-axis θ x ( θ y = 0 , θ z = 0 ) and ( b ) the peak reflection coefficient rotated about θ x . ( c ) Spectra when rotated about the y-axis θ y ( θ x = 0 , θ z = 0 ) and ( d ) the peak reflection rotated about θ y . ( e ) The peak reflection value rotated about θ z ( θ x = 0 , θ y = 0 ) with the xy-plane aligned to the monopole (z-axis normal to the monopole). The general fit is overlaid as a dash line.

Journal: Sensors (Basel, Switzerland)

Article Title: Small Split-Ring Resonators as Efficient Antennas for Remote LoRa IOT Systems—A Path to Reduce Physical Interference

doi: 10.3390/s21237779

Figure Lengend Snippet: The effect of rotation on the reflection coefficient measured by the monopole interaction with nearfield SRR antenna. The x-axis is parallel to the monopole, with the outer split upward and in plane of the SRR at θ x = 0 , θ y = 0 , a n d θ z = 0 —see . Spectra from a 433 MHz antenna design when rotated ( a ) about the x-axis θ x ( θ y = 0 , θ z = 0 ) and ( b ) the peak reflection coefficient rotated about θ x . ( c ) Spectra when rotated about the y-axis θ y ( θ x = 0 , θ z = 0 ) and ( d ) the peak reflection rotated about θ y . ( e ) The peak reflection value rotated about θ z ( θ x = 0 , θ y = 0 ) with the xy-plane aligned to the monopole (z-axis normal to the monopole). The general fit is overlaid as a dash line.

Article Snippet: The angular dependence of SRR antennas from nearfield measurements above a ground plane was also measured in the current work to compliment the findings of the farfield range tests, which did not include a ground plane.

Techniques: