Test Antennas and Parameters
I. Test Antennas
a. High Gain: dish, reflector, array antenna etc.
b. Medium Gain: fan beam, panel, base station antenna etc.
c. Low Gain: dipole, patch, wireless antennas etc.
II. Test Parameters
a. VSWR
b. Far field radiation patterns
c. Gain
d. Side-lobe levels, cross polarization, axial ratio, point
angle, beamwidth, coverage area, etc.
e. Near field distributions on planar, spherical, and
cylindrical surfaces.[/vc_column_text][/vc_column][vc_column width=”1/2″][vc_single_image image=”821″ img_size=”medium” alignment=”center” style=”vc_box_shadow_3d” onclick=”img_link_large” img_link_target=”_blank” css=”.vc_custom_1715379138386{padding-top: 20% !important;}”][/vc_column][/vc_row][vc_row][vc_column][vc_separator border_width=”6″][/vc_column][/vc_row][vc_row top_margin=”0″ bottom_margin=”0″ el_id=”rcs-test”][vc_column width=”1/2″ css=”.vc_custom_1715378978619{padding-left: 20% !important;}”][vc_custom_heading text=”RCS TEST SERVICES” font_container=”tag:h2|font_size:35px|text_align:left|color:%23353535|line_height:35px” google_fonts=”font_family:Oswald%3A300%2Cregular%2C700|font_style:300%20light%20regular%3A300%3Anormal”][vc_column_text]A. Test Facilities
I. RCS Test Chambers
Three anechoic test chambers are currently under
development and construction at ALLWAVE, the
schedule for completion is set on May 31, 2008
II. RCS Test Systems
a. Near-Field Test Systems
b. Far-Field Test Systems
c. Near-Field & Far-Field Test Systems
III. RF Equipment
a. Frequency Domain: Network Analyzer
b. Time Domain: Pulse Generator & Sampler
B. Test Parameters
I. RCS: Radar Cross Section
II. ISAR: Inverse Synthetic Aperture Radar[/vc_column_text][/vc_column][vc_column width=”1/2″][vc_single_image image=”661″ img_size=”medium” alignment=”center” style=”vc_box_shadow_3d” onclick=”img_link_large” img_link_target=”_blank” css=”.vc_custom_1715379329019{padding-top: 20% !important;}”][/vc_column][/vc_row][vc_row][vc_column]
a) The receiver comprises 2D square RF sensors that meticulously measure the amplitude and phase of the electric field at each grid point.
b) During the imaging process, a cell phone is actively engaged in a call and positioned atop the receiver.
c) Utilizing the collected near-field data grid, a three-dimensional depiction of the electromagnetic waves is subsequently generated via our proprietary FMA algorithm. This intricate 3D image not only illustrates the progression of the waves over time but also reveals the geometric intricacies of their propagation.[/vc_column_text][/vc_column][vc_column width=”1/2″][vc_single_image image=”1015″ img_size=”medium” alignment=”center” style=”vc_box_shadow_3d” onclick=”img_link_large” img_link_target=”_blank” css=”.vc_custom_1715379353410{padding-top: 20% !important;}”][/vc_column][/vc_row]