Near-Field Antenna Measurement Theory II Cylindrical
AMTA EDUCATIONAL SEMINAR 2002
Publication: AMTA 2002
Copyright Owner: NSI-MI Technologies
Cylindrical coordinate systems
Brief summary of rigorous derivation of transmission equation
Development of transmission equation using measurement approach
Comparison to planar transmission equation
Translation of centers for probe receiving coefficients
Far-field quantities
Probe correction
Probe coefficients from far-field pattern
Sample measurements and probe correction data
Near-Field Antenna Measurement Theory III Spherical
AMTA EDUCATIONAL SEMINAR 2002
Publication: AMTA 2002
Copyright Owner: NSI-MI Technologies
Spherical Coordinate Systems
Spherical Modes
Development Of Transmission Equation
Comparison To Planar And Cylindrical
Translation Of Centers For Probe Receiving Coefficients
Far-field Quantities
Probe Correction
Sample Data
Using a Tracking Laser Interferometer to Characterize the Planarity of a Planar Near-Field Scanner
Authors: Paul R. Rousseau, William C. Wysock, Carlos M. Turano, John R. Proctor
Publication: AMTA 2002
Copyright Owner: NSI-MI Technologies
This paper describes the experience of using a tracking
laser interferometer to align and characterize the planarity
of a planar near-field scanner. Last year, The Aerospace
Corporation moved their planar near-field antenna range
into a new larger room with improved environmental
controls. After this move, the near-field scanner required
careful alignment and characterization. The quality of the
scanner is judged by how accurately the probe scans over
a planar surface. The initial effort to align the scanner
used a large granite block as a planarity reference surface
and cumbersome mechanical probe measurements.
However, a tracking laser interferometer was used for the
final alignment and characterization.
The laser interferometer was included as part of an
alignment service purchased from MI Technologies. The
tracking laser interferometer emits a laser beam to a
mirrored target called an SMR (Spherically Mounted
Retroreflector). Encoders in the tracker measure the
horizontal and vertical angles while the laser
interferometer measures the distance. From these
measurements, the three-dimensional SMR location is
determined. The laser has the ability to very accurately
(within about 0.001 inch) measure the location of the
scanning near-field probe.
This paper includes a description of the mechanical
alignment of the scanner, the tracking laser interferometer
measurements, and the final planarity characterization.
Wireless Antenna Measurements
Author: Dr. Donald G. Bodnar
Publication: (MPD) Microwave Product Digest
Copyright Owner: NSI-MI Technologies
We are witnessing an explosive expansion of RF transmitting and receiving products
due to consumer demand for wireless voice and data connectivity and the
availability of cost-effective technology to produce such products and services.
Developers of these new products are keenly interested in the pattern, gain and
polarization of their products. Traditional antenna measurement equipment can
provide the needed information but usually at a prohibitively high price since such
test equipment was designed for general purpose, very high precision aerospace
applications. Many of the features needed in aerospace antenna measurements are
not required in wireless applications. For example, aerospace measurements are
often made at 35 or 95 GHz while wireless communication devices often work at
800 or 1,900 MHz. In addition, phase and amplitude measurements are made in
the aerospace applications while wireless measurements usually only require
amplitude information.
Estimating Z-Position Errors in Planar Near-Field Measurements From RF Measurements
Authors: Allen C. Newell, Jeff Way
Publication: AMTA 2002
Copyright Owner: NSI-MI Technologies
Z-position errors are generally the largest contributor to the uncertainty in sidelobe levels that are measured on a planar near-field range. The position errors result from imperfections in the mechanical rails that guide the motion of the measurement probe and cause it to deviate from an ideal plane. The deviations (,)zxyδcan be measured with precise optical and/or laser alignment tools and this is generally done during installation and maintenance checks to verify the scanner alignment. If the measurements are made to a very small fraction of a wavelength in Z and at intervals in X and Y approximating one half wavelength, the sidelobe uncertainty can be estimated with high confidence and is usually very small. For Z-error maps with lower resolution the resulting error estimates are generally larger or have lower confidence.
This paper describes a method for estimating the Z-position error from a series of planar near-field measurements using the antenna under test. Measurements are made on one or more planes close to the antenna and on other planes a few wavelengths farther away. The Z-distance between the close and far planes should be as large as the probe transport will allow. The difference between the holograms calculated from the close and far measurements gives an estimate of the Z-position errors. This approach has the advantage of using the actual AUT and frequency of interest and does not require specialized measurement equipment.