This application is a national stage (under 35 U.S.C. 371) of International Patent Application No. PCT/RU2014/000021, filed Jan. 16, 2015, which is herein incorporated by reference in its entirety.
The present invention relates generally to antennas, and more particularly to antennas for global navigation satellite systems.
Global navigation satellite systems (GNSSs) can determine positions with high accuracy. In a GNSS, a GNSS antenna receives electromagnetic signals transmitted from a constellation of GNSS satellites located within a line-of-sight of the antenna. The received electromagnetic signals are then processed by a GNSS receiver to determine the precise position of the GNSS antenna.
In an embodiment, an antenna includes a conductive cylindrical tube, a ground plane, a low-frequency radiator, and a high-frequency radiator. The conductive cylindrical tube has a longitudinal axis, an inner surface with a first inner diameter, and an outer surface with a first outer diameter. The ground plane has the geometry of a first annulus, in which the first circular inner periphery has a second inner diameter, and the first circular outer periphery has a second outer diameter. The ground plane is orthogonal to the longitudinal axis, and the first circular inner periphery is electrically connected to the outer surface of the conductive cylindrical tube.
The low-frequency radiator has the geometry of a second annulus, in which the second circular inner periphery has a third inner diameter, and the second circular outer periphery has a third outer diameter. The low-frequency radiator is orthogonal to the longitudinal axis, and the second circular inner periphery is electrically connected to the outer surface of the conductive cylindrical tube. The low-frequency radiator is spaced apart from the ground plane, and a low-frequency radiating gap is configured between the second circular outer periphery and the ground plane.
The high-frequency radiator has the geometry of a third annulus, in which the third circular inner periphery has a fourth inner diameter, and the third circular outer periphery has a fourth outer diameter. The high-frequency radiator is orthogonal to the longitudinal axis, and the high-frequency radiator is spaced apart from the low-frequency radiator such that the low-frequency radiator is disposed between the high-frequency radiator and the ground plane. The third circular outer periphery is electrically connected to the low-frequency radiator, and a high-frequency radiating gap is configured between the third circular inner periphery and the outer surface of the conductive cylindrical tube.
In an embodiment, the outer diameter of the conductive cylindrical tube has a value from about 28 mm to about 103 mm, and the inner diameter of the conductive cylindrical tube has a value from about 27 mm to about 102 mm. This range of inner diameters is sufficient to permit a post or pole to be inserted into the cylindrical tube.
These and other advantages of the invention will be apparent to those of ordinary skill in the art by reference to the following detailed description and the accompanying drawings.
In
To numerically characterize the capability of an antenna to mitigate the reflected signal, the following ratio is commonly used:
The parameter DU(θe) (down/up ratio) is equal to the ratio of the antenna pattern level F(−θe) in the backward hemisphere to the antenna pattern level F(θe) in the forward hemisphere at the mirror angle, where F represents a voltage level. Expressed in dB, the ratio is:
DU(θe) dB=20 logDU(θe). (E2)
A commonly used characteristic parameter is the down/up ratio at θe=+90 deg:
In a GNSS, the accuracy of position determination is improved as the antenna receives signals from a larger constellation of satellites; in particular, from low-elevation satellites (˜10- 15 deg above the horizon). A strong antenna pattern level over nearly the entire forward hemisphere is therefore desirable.
A major source of errors uncorrected by signal processing is multipath reception by the receiving antenna. In addition to receiving direct signals from the satellites, the antenna receives signals reflected from the environment around the antenna. The reflected signals are processed along with the direct signals and cause errors in time delay measurements and errors in carrier phase measurements. These errors subsequently cause errors in position determination. An antenna that strongly suppresses the reception of multipath signals is therefore desirable.
Each navigation satellite in a GNSS can transmit circularly-polarized signals on one or more frequency bands (for example, on the L1, L2, and L5 frequency bands). A single-band navigation receiver receives and processes signals on one frequency band (such as L1); a dual-band navigation receiver receives and processes signals on two frequency bands (such as L1 and L2); and a multi-band navigation receiver receives and processes signals on three or more frequency bands (such as L1, L2, and L5). A single-system navigation receiver receives and processes signals from a single GNSS [such as the US Global Positioning System (GPS)]; a dual-system navigation receiver receives and processes signals from two GNSSs (such as GPS and the Russian GLONASS); and a multi-system navigation receiver receives and processes signals from three or more systems (such as GPS, GLONASS, and the planned European GALILEO). The operational frequency bands can be different for different systems. An antenna that receives signals over the full frequency range assigned to GNSSs is therefore desirable. The full frequency range assigned to GNSSs is divided into two frequency bands: the low-frequency band (about 1165 to about 1300 MHz) and the high-frequency band (about 1525 to about 1605 MHz).
For portable navigation receivers, compact size and light weight are important design factors. Low-cost manufacture is usually an important factor for commercial products. For a GNSS navigation receiver, therefore, an antenna with the following design factors would be desirable: circular polarization; operating frequency over the low-frequency band (about 1165 to about 1300 MHz) and the high-frequency band (about 1525 to about 1605 MHz); strong antenna pattern level over most of the forward hemisphere; strong suppression of multipath signals; compact size; light weight; and low manufacturing cost.
In some applications, the antenna is mounted on a short post or on a long pole. In some instances, the antenna is mounted slightly above, but not in direct contact with, a surface, which can be planar (flat) or curved. In these instances, the antenna can be mounted to a short post, which in turn is mounted to the surface. In other instances, the antenna is mounted to a long pole; for example, the long pole can be a surveying pole or a mast on a vehicle. In an advantageous design, the antenna has an internal clear space (hollow core) through which the post or pole can be inserted. This configuration simplifies mounting of the antenna to the post or pole and allows a wide range of spacing between the antenna and a support surface; furthermore, the spacing can be readily adjusted by sliding the antenna along the post or pole.
In embodiments of antenna systems described herein, geometrical conditions are satisfied if they are satisfied within specified tolerances; that is, ideal mathematical conditions are not implied. The tolerances are specified, for example, by an antenna engineer. The tolerances are specified depending on various factors, such as available manufacturing tolerances and trade-offs between performance and cost. As examples, two lengths are equal if they are equal to within a specified tolerance, two planes are parallel if they are parallel within a specified tolerance, and two lines are orthogonal if the angle between them is equal to 90 deg within a specified tolerance. Similarly, geometrical shapes such as circles and cylinders have associated “out-of-round” tolerances.
For GNSS receivers, the antenna is operated in the receive mode (receive electromagnetic radiation or signals). Following standard antenna engineering practice, however, antenna performance characteristics are specified in the transmit mode (transmit electromagnetic radiation or signals). This practice is well accepted because, according to the well-known antenna reciprocity theorem, antenna performance characteristics in the receive mode correspond to antenna performance characteristics in the transmit mode.
The geometry of antenna systems is described with respect to the Cartesian coordinate system shown in
The coordinates of P can also be expressed in the spherical coordinate system and in the cylindrical coordinate system. In the spherical coordinate system, the coordinates of P are P(R,θ,φ), where R=|{right arrow over (R)}| is the radius, θ 223 is the polar angle measured from the x-y plane, and φ 225 is the azimuthal angle measured from the x-axis. In the cylindrical coordinate system, the coordinates of P are P(r,φ,h), where r=|{right arrow over (r)}| is the radius, φ is the azimuthal angle, and h=|{right arrow over (h)}| is the height measured parallel to the z-axis. In the cylindrical coordinate axis, the z-axis is referred to as the longitudinal axis. In geometrical configurations that are azimuthally symmetric about the z-axis, the z-axis is referred to as the longitudinal axis of symmetry, or simply the axis of symmetry if there is no other axis of symmetry under discussion.
The polar angle θ is more commonly measured down from the +z-axis (0≦θ≦π). Here, the polar angle θ 223 is measured from the x-y plane for the following reason. If the z-axis 207 refers to the z-axis of an antenna system, and the z-axis 207 is aligned with the geographic z-axis 105 in
In illustrating embodiments of antennas, various views are used in the figures. View B is a top (plan) view, sighted along the −z-axis. View C is a bottom view, sighted along the +z-axis. Other views are defined as needed.
In the dimensions described below, diameters are measured along the x-y plane; thicknesses, heights, and vertical spacings (also referred to as longitudinal spacings) are measured along the z-axis. The cylindrical tube 302 has an inner diameter 301, an outer diameter 303, and a height 311 (measured between the bottom end face 302B and the top end face 302T). The ground plane 304 has an outer diameter 309 and a thickness 321 (measured between the bottom surface 304B and the top surface 304T). The LF radiator 306 has an outer diameter 307 and a thickness 323 (measured between the bottom surface 306B and the top surface 306T). The HF radiator 308 has an outer diameter 305 and a thickness 325 (measured between the bottom surface 308B and the top surface 308T).
The vertical spacing between the bottom end face 302B of the cylindrical tube 302 and the bottom surface 304B of the ground plane 304 is the vertical spacing 313. The vertical spacing between the top surface 304T of the ground plane 304 and the bottom surface 306B of the LF radiator 306 is the vertical spacing 315. The vertical spacing between the top surface 306T of the LF radiator 306 and the bottom surface 308B of the HF radiator 308 is the vertical spacing 317. The vertical spacing between the top surface 308T of the HF radiator 308 and the top end face 302T of the cylindrical tube 302 is the vertical spacing 319.
In the prior-art antenna 300, the maximum value of the outer diameter 303 of the cylindrical tube 302 is 0.05λ, where λ is an operational wavelength of the antenna (the choice of λ is discussed in more detail below). Assuming that the cylindrical tube 302 has a thin wall [wall thickness of about 0.5 mm, where the wall thickness=(outer diameter 303−inner diameter 301)/2], the inner diameter 301 is equal to the outer diameter 303 (in mm)−1 mm. As discussed in more detail below, at GNSS frequencies, λ ranges from about 258 mm at the low end of the LF band to about 187 mm at the high end of the HF band. For λ=258 mm, 0.05λ corresponds to a value of 13 mm; for a value of λ=187 mm, 0.05λ corresponds to a value of 9 mm; therefore, the inner diameter corresponds to values of 12 mm to 9 mm. For some applications, discussed below, a larger inner diameter, corresponding to an outer diameter 303 in the range from about 0.15λ to about 0.4λ, is desired. In the prior-art antenna 300, if the outer diameter 303 of the cylindrical tube 302 is increased, then, to maintain the desired operational frequency range, the outer diameter 307 of the LF radiator 306 and the outer diameter 305 of the HF radiator 308 needs to be increased.
Increasing the outer diameter 307 and the outer diameter 305, however, degrades the antenna performance. Shown in
When the diameter of the radiating gap is increased (greater than about 0.4λ), the antenna pattern level at low elevation angles is decreased. As discussed above, a decrease of the antenna pattern level at low elevation angles is undesirable for GNSS antennas. Furthermore, the antenna pattern levels at other angles in the forward hemisphere can also drop, and the degree of multipath suppression decreases (the down/up ratio increases).
In the dimensions described below, diameters, wall thicknesses, and lengths are measured along the x-y plane; thicknesses, heights, and vertical spacings (also referred to as longitudinal spacings) are measured along the z-axis.
The cylindrical tube 402 has the outer surface (wall) 402O, the inner surface (wall) 402I, the top end face (also referred to as the first end face) 402T, and the bottom end face (also referred to as the second end face) 402B. The plane of the top end face and the plane of the bottom end face are each orthogonal to the longitudinal axis. Each of the inner surface and the outer surface is a cylindrical surface. The cylindrical tube 402 has an inner diameter 401, an outer diameter 403, and a height 411 (measured between the bottom end face 402B and the top end face 402T). In an embodiment, the outer diameter 403 has a value from about 0.15λref to about 0.4λref, where λref is a reference operational wavelength of the antenna (see below).
Wavelength is related to frequency by the well-known relationship λ=c/f, where λ is the wavelength, c is the speed of light, and f is the frequency. In free space, the following values are obtained:
In some embodiments, the antenna is tuned to operate over a narrower band than the full GNSS band. In general, in the frequency domain,
fLF,min≦fLF≦fLF,max, and
fHF,min≦fHF≦fHF,max;
where fLF is an operational frequency of the antenna in the LF band bounded by the minimum value fLF,min and the maximum value fLF,max, and fHF is an operational frequency of the antenna in the HF band bounded by the minimum value fHF,min and the maximum value fHF,max; the minimum and maximum values are specified, for example, by an antenna designer for the application of interest. Similarly, in the wavelength domain,
λLF,min≦λLF≦λLF,max, and
λHF,min≦λHF≦λHF,max;
where λLF is an operational wavelength of the antenna in the LF band bounded by the minimum value λLF,min and the maximum value λLF,max, and λHF is an operational wavelength of the antenna in the HF band bounded by the minimum value λHF,min and the maximum value λHF,max.
The reference operational wavelength λref is selected by the antenna designer as a single reference value at which to characterize the operational parameters of the antenna. Examples of λref include the value of λ corresponding to fLF,min, the value of λ corresponding to the central frequency in the LF band fLF,min≦fLF≦fLF,max, and the value of λ corresponding to the central frequency over the dual frequency band fLF,min≦f≦fHF,max. In some applications, two reference operational wavelengths are defined, one for the LF band (λLF,ref) and one for the HF band (λHF,ref); in each band, the reference wavelength, for example, can correspond to the minimum frequency, the central frequency, or the maximum frequency in the band.
The ground plane 404 has an outer diameter 413, an inner diameter 403, and a thickness 431 (measured between the bottom surface 404B and the top surface 404T). The LF radiator 406 has an outer diameter 407, an inner diameter 403, and a thickness 433 (measured between the bottom surface 406B and the top surface 406T). The HF radiator 408 has an outer diameter 407, an inner diameter 405, and a thickness 437 (measured between the bottom surface 408B and the top surface 408T). The HF radiator 408 is electrically connected to the LF radiator 406 by the conductive cylindrical tube 412, which has the outer wall 412O and the inner wall 412I; the wall thickness of the cylindrical tube 412 is the wall thickness 441.
The vertical spacing between the bottom end face 402B of the cylindrical tube 402 and the bottom surface 404B of the ground plane 404 is the vertical spacing 413. The vertical spacing between the top surface 404T of the ground plane 404 and the bottom surface 406B of the LF radiator 406 is the vertical spacing 415. The vertical spacing between the top surface 406T of the LF radiator 406 and the bottom surface 408B of the HF radiator 408 is the vertical spacing 417. The vertical spacing between the top surface 408T of the HF radiator 408 and the top end face 402T the cylindrical tube 402 is the vertical spacing 419.
In an embodiment, the vertical spacing 417 (also referred to as the height h1) has a value from about 0.02λHF,ref to about 0.1λHF,ref, where λHF,ref is a reference operational wavelength in the HF band. Similarly, the vertical spacing 415 (also referred to as the height h2) has a value from about 0.02λLF,ref to about 0.1λLF,ref, where λLF,ref is a reference operational wavelength in the LF band.
Refer to
The set of HF capacitive elements 460 is azimuthally spaced about the longitudinal axis and is bounded on the outer periphery by the reference circle 460O (with a diameter 461). In the embodiment shown in
In
The set of parasitic elements 420 is azimuthally spaced about the longitudinal axis and is bounded by the reference circle 410I (with a diameter 409) and the reference circle 410O (with a diameter 411). In the embodiment shown in
In the embodiment shown, each parasitic element includes a vertical segment and a horizontal segment. In other embodiments, each parasitic element has a vertical segment only (no horizontal segment). To representative parasitic elements are shown in
The cross-sectional geometry of a vertical segment is arbitrary. In one example, the vertical segment 414-7 is a cylindrical post with a diameter 443. The bottom end face of vertical segment 414-7 is electrically connected to the top surface 404T of the ground plane 404, and the top end face of the vertical segment 414-7 is electrically connected to the bottom surface 416B-7 of the horizontal segment 416-7. The vertical spacing between the top surface 404T of the ground plane 404 and the top surface 4161-7 of the horizontal segment 416-7 is the vertical spacing 421. In the embodiment shown, the vertical spacing 421 is equal to the vertical spacing 423 between the top surface 404T of the ground plane 404 and the top surface 408T of the HF radiator 408. In other embodiments, the vertical spacing 421 is not equal to the vertical spacing 423. The horizontal segment 416-7 has a thickness 435 (measured between the bottom surface 416B-7 and the top surface 416T-7)
Refer to
The set of parasitic elements 420 improves the antenna performance.
Return to
The LF radiator 506 is fabricated as a conductive annulus with a circular outer periphery 506O and a circular inner periphery 502I. In the embodiment shown, around the circular outer periphery 506O is a set of LF capacitive elements 526 aligned orthogonal to the plane of the LF radiator 506. In this example, the LF radiator 506 and the set of LF capacitive elements 526 are fabricated from a single piece of sheet metal. Notches are cut out from the outer periphery of the sheet, and the resulting tabs are bent 90 deg to form the set of LF capacitive elements 526. Other manufacturing techniques can be used; for example, the set of LF capacitive elements can be soldered or mechanically fastened to the LF radiator. The LF radiator 506 is supported above the PCB 524 by the set of dielectric standoffs 560. The set of LF capacitive elements 526, which provides capacitive coupling between the outer periphery 506O of the LF radiator 506 and the ground plane 504, serves as wave-slowing structures and permits the outer diameter of the LF radiator 506 to be reduced.
The printed circuit board (PCB) 528 has the geometry of an annulus with a circular outer periphery 528O and a circular inner periphery 528I. The PCB 528 has a top side 528T and a bottom side 528B. Refer to
Return to
Refer to
The set sidewall segments 512 are electrically connected to the HF radiator 566 fabricated on the bottom side 528B of the PCB 528. Refer to
Return to
Refer to
Refer to
Refer to
Return to
Principal features of the antenna system 500 are summarized in
The LF radiator 506 has a circular inner periphery 506I, a circular outer periphery 506O, a top surface 506T, and a bottom surface 506B. A circular set of LF capacitive elements 526 is configured around the circular outer periphery 506O. The circular set of LF capacitive elements 526 has an inner periphery 526I, an outer periphery 526O, a top end face 526T, and a bottom end face 526B. The circular set of LF capacitive elements 526 is aligned orthogonal to the plane of the LF radiator 506.
The support ring 516 includes the base plate 518 and the sidewall 512. The base plate 518 has a circular inner periphery 518I, a circular outer periphery 518O, a top surface 518T, and a bottom surface 518B. The sidewall 512 has an inner surface 512I, an outer surface 512O, a top end face 512T, and a bottom end face 512B (to simplify the drawing, details of the tabs are not shown).
The PCB 534 has an inner surface 534I, an outer surface 534O, a top end face 534T, and a bottom end face 534B. There is a circular set of conductive strips 514 fabricated on the outer surface 534O. Each conductive strip is aligned along the longitudinal axis.
The PCB 528 has a circular inner periphery 528I, a circular outer periphery 528O, a top side 528T, and a bottom side 528B. A first circular set of vias 560 passes through the PCB 528 from the top side 528T to the bottom side 528B. A second circular set of vias 562 passes through the PCB 528 from the top side 528T to the bottom side 528B. The HF radiator 566 is fabricated on the bottom side 528B. A set of HF capacitive elements 570 and a set of horizontal segments 510 is fabricated on the top side 528T. A portion of an excitation system is fabricated in the region 564 on the top side 528T.
The LF radiator 506 has an outer diameter 507, an inner diameter 503, and a thickness 533 (measured between the bottom surface 506B and the top surface 506T). The circular set of LF capacitive elements 526 has an outer diameter 507, a wall thickness 545 (measured between the inner surface 526I and the outer surface 526O), and a height 523 (measured between the bottom surface 506B of the LF radiator 506 and the bottom end face 526B of the circular set of LF capacitive elements 526).
The PCB 528 has an outer diameter 515, an inner diameter 503, and a thickness 535 (measured between the top side 528T and the bottom side 528B). The circular set of HF capacitive elements 570 is fabricated on the top side 528T (a representative HF capacitive element 570-J is labelled); the circular set of HF capacitive elements 570 has an outer diameter 571. The circular set of horizontal segments 510 is fabricated on the top side 528T (a representative horizontal segment 510-J is labelled); the circular set of horizontal segments 510 has an inner diameter 511. A portion of the excitation system is fabricated in the region 564 of the top side 528T.
The HF radiator 566 is fabricated on the bottom side 528B. The HF radiator 566 has an outer diameter 509 and an inner diameter 505. The support ring 516 includes the base plate 518 and the circular set of sidewall segments 512. The base plate 518 has an outer diameter 507, an inner diameter 503, and a thickness 537 (measured between the top surface 518T and the bottom surface 518B). The circular set of sidewall segments 512 has an outer diameter 507 and a wall thickness 541 (measured between the inner surface 512I and the outer surface 512O). The base plate 518 is electrically connected to the LF radiator 506, and the circular set of sidewall segments 512 is electrically connected to the HF radiator 566.
The PCB 534 has an outer diameter 513 and a wall thickness 543 (measured between the outer surface 534O and the inner surface 534I. A circular set of conductive strips 514 is fabricated on the outer surface 534O (a representative conductive strip 514-J is labelled). The circular set of conductive strips 514 electrically connects the circular set of horizontal segments 510 to the ground plane 504.
The vertical spacing between the bottom end face 502B of the cylindrical tube 502 and the bottom surface 524B of the PCB 524 is the vertical spacing 525. The vertical spacing between the top surface 524T of the PCB 524 and the bottom surface 506B of the LF radiator 506 is the vertical spacing 527. The vertical spacing between the top surface 518T of the base plate 518 and the bottom surface 528B of the PCB 528 is the vertical spacing 529. The vertical spacing between the top surface 524T of the PCB 524 and the bottom surface 528B of the PCB 528 is the vertical spacing 551. The vertical spacing between the top surface 528T of the PCB 528 and the top end face 502T of the cylindrical tube 502 is the vertical spacing 553.
The antenna system 500 is excited by a dual-band pin excitation system. Refer to
The LF excitation system 610 is shown schematically in
Return to the quadrature splitter 612. The output port 612-3 is electrically connected to the input port 616-1 of the −90 deg phase shifter 616. With respect to the signal at the input port 616-1, the signal at the output port 616-2 is phase shifted by −90 deg (net phase shift of −180 deg with respect to the signal at the input port 612-1 of the quadrature splitter 612). The output port 616-2 is electrically connected to the input port 618-1 of the quadrature splitter 618. With respect to the signal at the input port 618-1, the signal at the output port 618-2 is in-phase (0 deg phase shift), and the signal at the output port 618-3 is phase shifted by −90 deg.
Consequently, the output signals at port 614-2, port 614-3, port 618-2, and port 618-3 have net phase shifts of 0 deg, −90 deg, −180 deg, and −270 deg, respectively. These four ports are electrically connected to the LF exciter pin 540-1, the LF exciter pin 540-2, the LF exciter pin 540-3, and the LF exciter pin 540-4, respectively. Circularly-polarized radiation is therefore excited.
The HF excitation system 610 is shown schematically in
Return to the quadrature splitter 622. The output port 622-3 is electrically connected to the input port 626-1 of the −90 deg phase shifter 626. With respect to the signal at the input port 626-1, the signal at the output port 626-2 is phase shifted by −90 deg (net phase shift of −180 deg with respect to the signal at the input port 622-1 of the quadrature splitter 622). The output port 626-2 is electrically connected to the input port 628-1 of the quadrature splitter 628. With respect to the signal at the input port 628-1, the signal at the output port 628-2 is in-phase (0 deg phase shift), and the signal at the output port 628-3 is phase shifted by −90 deg.
Consequently, the output signals at port 624-2, port 624-3, port 628-2, and port 628-3 have net phase shifts of 0 deg, −90 deg, −180 deg, and −270 deg, respectively. These four ports are electrically connected to the HF exciter pin 542-1, the HF exciter pin 542-2, the HF exciter pin 542-3, and the HF exciter pin 542-4, respectively. Circularly-polarized radiation is therefore excited.
In an embodiment, the LF excitation system 610 is fabricated on the bottom side 524B of the PCB 524; and the LNA 630 is also mounted on the bottom side 524B, The HF excitation system 620 is fabricated on the top side 528T of the PCB 528. A signal cable (not shown) electrically connects the HF excitation system 620 to the LNA 630.
In the embodiments described above, the antennas have an overall approximately cylindrical geometry: the center tube has the geometry of a cylindrical tube, and the LF radiator and the HF radiator have the geometry of a circular annulus. In other embodiments, the cross-sectional geometry of the antenna (orthogonal to the longitudinal axis of the antenna) is non-circular. For example, the cross-sectional geometry of the center tube (inner wall and outer wall), LF radiator, HF radiator, and other components can be an n-sided regular polygon, where n is an integer greater than or equal to 4.
The foregoing Detailed Description is to be understood as being in every respect illustrative and exemplary, but not restrictive, and the scope of the invention disclosed herein is not to be determined from the Detailed Description, but rather from the claims as interpreted according to the full breadth permitted by the patent laws. It is to be understood that the embodiments shown and described herein are only illustrative of the principles of the present invention and that various modifications may be implemented by those skilled in the art without departing from the scope and spirit of the invention. Those skilled in the art could implement various other feature combinations without departing from the scope and spirit of the invention.
Filing Document | Filing Date | Country | Kind |
---|---|---|---|
PCT/RU2014/000021 | 1/16/2014 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2015/108436 | 7/23/2015 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
5220334 | Raguenet et al. | Jun 1993 | A |
7126538 | Sampo | Oct 2006 | B2 |
20020171595 | Schultze | Nov 2002 | A1 |
20080218418 | Gillette | Sep 2008 | A1 |
20140176386 | Rentz | Jun 2014 | A1 |
Number | Date | Country |
---|---|---|
2134923 | Aug 1999 | RU |
2258284 | Aug 2005 | RU |
Entry |
---|
International Search Report and Written Opinion mailed Feb. 5, 2015, in connection with International Patent Application No. PCT/RU2014/000021, 6 pgs. |
Number | Date | Country | |
---|---|---|---|
20160020521 A1 | Jan 2016 | US |