Abstract:The inverse source problem has a number of applications in antenna analysis and synthesis. The properties of the radiation operator, connecting the source current to the far zone field, depends on the source geometry and can be analyzed by its singular value decomposition. Here, first, we present useful upper bounds about the number of degrees of freedom for some 2D source geometries (i.e. for elliptical and parabolic arc sources) and examine the role of two different representation variables. These results we… Show more
“…For UAV communications, the work done in [19] proposed conical conformal array at 9.8 GHz for point-to-point communications, while in [20], the cylindrical antenna arrays are combined with conical arrays to form "CYLCON" array using microstrip Yagi antennas to provide wide solid angle scanning. On the other hand, the recent work done in [30] discussed the radiation properties of different source geometries based on the inverse source problem. One of the most important achievements in [30] is the focused patterns for mainlobes at different angular directions, however, the tested structures have relatively high sidelobe levels.…”
Section: Background and Motivationmentioning
confidence: 99%
“…On the other hand, the recent work done in [30] discussed the radiation properties of different source geometries based on the inverse source problem. One of the most important achievements in [30] is the focused patterns for mainlobes at different angular directions, however, the tested structures have relatively high sidelobe levels. Additionally, spherical conformal arrays were proposed in [31] to compensate for the changing spherical surfaces using patch antenna structures.…”
In this paper, a new conformal array structure and beamforming technique are proposed to provide efficient communication performance for unmanned aerial vehicles (UAVs) and space vehicles. The proposed array is formed by conformally stacking cylindrical, conical, and concentric circular (CSC4) arrays which are all coaxially aligned with the same axis of the conformed body and with uniform interelement spacing. The array elements are then fed by a weighting vector that has an adaptive cosine tapered profile where the maximum amplitude coefficient is oriented with the mainlobe direction to improve the scanning capabilities of the array and increase the array effective area. In addition, for very large, conformed body structures such as space vehicles, a frontal mainlobe-oriented partial CSC4 array beamforming technique is proposed to efficiently utilize the large CSC4 structure, reduce the processing requirements for mainlobe electronic steering, and to provide very low sidelobe levels with reduced backlobe levels. Simulation results show that the proposed CSC4 design can provide wide scanning angles of up to ±70° angular range in the θ-direction with only ±1° change in the beamwidth, without increasing array size and with achievable sidelobe level of –45 dB and backlobe levels less than –10 dB.
“…For UAV communications, the work done in [19] proposed conical conformal array at 9.8 GHz for point-to-point communications, while in [20], the cylindrical antenna arrays are combined with conical arrays to form "CYLCON" array using microstrip Yagi antennas to provide wide solid angle scanning. On the other hand, the recent work done in [30] discussed the radiation properties of different source geometries based on the inverse source problem. One of the most important achievements in [30] is the focused patterns for mainlobes at different angular directions, however, the tested structures have relatively high sidelobe levels.…”
Section: Background and Motivationmentioning
confidence: 99%
“…On the other hand, the recent work done in [30] discussed the radiation properties of different source geometries based on the inverse source problem. One of the most important achievements in [30] is the focused patterns for mainlobes at different angular directions, however, the tested structures have relatively high sidelobe levels. Additionally, spherical conformal arrays were proposed in [31] to compensate for the changing spherical surfaces using patch antenna structures.…”
In this paper, a new conformal array structure and beamforming technique are proposed to provide efficient communication performance for unmanned aerial vehicles (UAVs) and space vehicles. The proposed array is formed by conformally stacking cylindrical, conical, and concentric circular (CSC4) arrays which are all coaxially aligned with the same axis of the conformed body and with uniform interelement spacing. The array elements are then fed by a weighting vector that has an adaptive cosine tapered profile where the maximum amplitude coefficient is oriented with the mainlobe direction to improve the scanning capabilities of the array and increase the array effective area. In addition, for very large, conformed body structures such as space vehicles, a frontal mainlobe-oriented partial CSC4 array beamforming technique is proposed to efficiently utilize the large CSC4 structure, reduce the processing requirements for mainlobe electronic steering, and to provide very low sidelobe levels with reduced backlobe levels. Simulation results show that the proposed CSC4 design can provide wide scanning angles of up to ±70° angular range in the θ-direction with only ±1° change in the beamwidth, without increasing array size and with achievable sidelobe level of –45 dB and backlobe levels less than –10 dB.
“…It is important to point out that, as shown in [9], the NDF of a conformal 2D curve source is related only to its electrical length. Therefore, it is apparent that also the directivity is proportional to it, as well known for the linear case.…”
Section: Ndf and Directivitymentioning
confidence: 99%
“…For an arc of circumference of radius , = , ( ) = , ‖ ′( ) ‖ = , = − , = in the integral operator (1), but, differently from the circumference case, no analytical results for the pertinent SVD are available in this case. Some asymptotic reasonings [9], [20] have led to an estimation of the NDF as…”
Section: Semi-circumferencementioning
confidence: 99%
“…In particular, the NDF defines the dimension of the space of the far field functions that can be radiated by a finite energy source, while the PSF is usually connected to the reconstruction of point-like sources. This approach has revealed itself useful in order to establish a way to compare the general radiation properties of some conformal source [9] before undertaking the synthesis procedure of a particular antenna with defined specifications [11].…”
<p>The<b>
</b>role of the source geometry in the the radiation of focusing beams by
conformal antennas is examined by the comparison of their directivity functions
at different maximum directions. An
inverse source problem approach is adopted, where solutions stable with respect
to data uncertainties are to be found by relying on the analysis of the
pertinent operator by the Singular Values Decomposition. This general framework
allows to connect the mean value of the mazimum directivity function to the
Number of Degrees of Freedom of the conformal source, which depends only on its
electrical length. For each source geometry the focusing far field ensuring the
maximum directivity for every pointing direction and the corresponding source
current are obtained. The comparison with the ones achieved by the usual phase
compensation technique of the source current reveals their optimal behavior.
The usefulness of the approach as a tool in antenna synthesis is shown by
comparing different geometries for those applications where identical beams are
required to be rdiated for the coverage of a larga angular domain.</p>
Terrestrial mapping is performed on the topographic surface, but control points are typically defined using a Projected Coordinate System (PCS). Using PCS directly as control points in terrestrial data processing can cause problems in final result. They must be corrected before, due to the discrepancies between the projection plane and the ellipsoid, and between the ellipsoid and the topographic surface. To address this, we propose an alternative approach that involves defining a custom ellipsoid that intersect with the topographic surface. In practice, this approach utilizes a control point whose coordinate is defined using PCS on the custom ellipsoid. To test this concept, we conducted a calculation of an open traverse survey spanning 10 km east-west and measuring an elevation of 1000 m above the reference ellipsoid. The traverse survey included two control points at the beginning and end, and two check points every 3 km. The traverse calculation was done using four different coordinate systems, including a combination of WGS84 and custom ellipsoid for the datums, and Universal Transverse Mercator zone 48 south (UTM48S) and Transverse Mercator (TM) with custom central meridian for the projections. After the calculation, we found that the lowest linear misclosure value was produced by the combination of custom datum-custom TM. The coordinate at the check point was then evaluated and the result showed that the total linear misclosure of the combination of custom datum-custom TM was not significantly different from WGS84-custom TM, with values of only differ by less than 1mm.While the difference of linear misclosure with standard data processing differ by 8 mm. Based on this result, we can conclude that the use of proper projection system in control point coordinate definition or combine with custom datum is the best option for open traverse without control at the end.
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