Planar coupling of spherical ferrites

Information

  • Patent Grant
  • 6504459
  • Patent Number
    6,504,459
  • Date Filed
    Thursday, June 21, 2001
    22 years ago
  • Date Issued
    Tuesday, January 7, 2003
    21 years ago
Abstract
A spherical resonator device includes a resonant sphere around which transducers for electrical coupling are metallized layers on a flat surface shaped to provide exposure of a sphere to a quasi constant field. In particular, the pattern comprises a transmission line of non-constant width in the region proximate to the sphere where a taper is provided which increases in width with distance from the sphere.
Description




BACKGROUND OF THE INVENTION




This invention relates to ferrite resonators and more particularly to coupling structures used with ferrite spheres.




A spherical ferrite is used as a resonator for building microwave tunable devices, such as oscillators, filters, limiters, and the like. In the past a complicated wire loop transducer is conventionally used to couple to the spherical ferrite resonator, which, in order to maximize coupling to the sphere, the transducer or transducers are in the shape of a half circle loop disposed around the sphere so that the wire is at roughly equal distance from the surface of the sphere. This configuration makes the assembly of these devices a time consuming task; making it almost impossible to implement an automated procedure for the purpose of high volume production of these components. What is needed is a configuration and structure to facilitate high volume manufacturability of spherical ferrite based devices.




BRIEF SUMMARY OF THE INVENTION




According to the invention, a spherical resonator device includes a resonant sphere around which transducers for electrical coupling are metallized layers on a flat surface shaped to provide exposure of the resonant sphere to a quasi constant field. In particular, the pattern comprises a transmission line of non-constant width in the region proximate to the sphere where a taper is provided which increases in width with distance from the sphere.




The invention will be better understood by reference to the following detailed description in connection with the accompanying drawings.











BRIEF DESCRIPTION OF THE DRAWINGS





FIG. 1

is a perspective view of a layout of a first coupling showing placement of a resonating sphere according to the invention.





FIG. 2

is a top view of the layout of the first coupling.





FIG. 3

is a top view of the layout of the first coupling showing placement of the resonating sphere.





FIG. 4

is a top view of a dual coupling showing orthogonal patterns on either side of a sphere.





FIG. 5

is a top view of a single coupling showing a secondary resonant feedback coupling.











DESCRIPTION OF SPECIFIC EMBODIMENTS




Reference is made to FIG.


1


. Note that planar substrates, physical support structures, and supporting rods are not always shown, but it is to be understood that a transducer


18


is mounted on a planar substrate


12


, which is supported by support structures


10


, and that a resonating sphere


14


is suspended by a support rod


16


over the transducer


18


. Alternatively, the resonating sphere may be mounted in an orifice between opposing sides of the planar substrate


12


.





FIG. 2

shows that the transducer


18


is a metallized layer having a non-constant width. The transducer


18


has a first region


20


having a minimum width, a second region


22


having a maximum width, and a third region


24


having a maximum width. A transition region


26


exists between the first region


20


and the second region


22


. In the transition region


26


, the width of the transducer


18


changes gradually from the minimum width of the first region


20


to the maximum width of the second region


22


. A transition region


28


exists between the first region


20


and the third region


24


. In the transition region


28


, the width of the transducer


18


changes gradually from the minimum width of the first region


20


to the maximum width of the third region


24


. The change of width in the transition regions


26


and


28


can resemble different mathematical function, including exponential functions.





FIG. 3

illustrates the placement of the resonating sphere


14


over the first region of the transducer


18


. Following the contour of the transition regions


26


and


28


, away from the resonating sphere


14


, the gradually increasing width of the transducer


18


, from the minimum width of the first region to the maximum widths of the second region


22


and the third region


24


, compensates for the gradual increase in distance of the boundary of the transition regions


26


and


28


from the resonating sphere


14


. The unique shape of the transducer


18


thus produces a quasi constant field to which the resonating sphere


14


is exposed.




Referring to

FIG. 4

, dual coupling is achieved by the placement of the resonating sphere


14


between orthogonally positioned transducers


42


and


44


. The transducers


42


and


44


are respectively mounted on separate planar substrates (not shown) that “sandwich” the resonant sphere


14


. This dual coupling structure produces, among other things, bandpass filters and special oscillators.





FIG. 5

shows a secondary resonant feedback coupling mechanism, which is achieved by mounting a trace


50


next to a transducer


52


, on the same planar substrate. The unique flat-surface shape of the transducer


52


allows the trace


50


to easily be incorporated in the same plane as the transducer


52


. The secondary resonant feedback coupling mechanism increases the operating bandwidth of the resonant sphere based device.




The invention has been explained with reference to specific embodiments. Other embodiments will be evident to those of ordinary skill in the art. It is therefore not intended that this invention be limited, except as indicated by the appended claims.



Claims
  • 1. A spherical resonator device comprising:a resonant sphere; at least one transducer for electromagnetic coupling to said resonant sphere, said transducer comprising a flat metallized layer having a finite width shaped to provide exposure of the sphere to a quasi constant field, wherein said at least one transducer comprises a first region having a first width and a second region having a second width and a transition region between said first region and said second region, said first region being adjacent said resonant sphere, said first width being at a minimum, said second region being displaced radially from said resonant sphere, said second width being at a maximum, said transition region bridging between said first region and second region.
  • 2. The device according to claim 1 wherein said transition region follows an exponential profile of increasing width from said first region to said second region, said profile being selected to compensate for decrease in field strength of coupling between said resonant sphere and said transducer and to enhance bandwidth of resonant coupling.
  • 3. The device according to claim 1 further including a second transducer disposed orthogonally to said first transducer and on an opposing side of said resonant sphere.
  • 4. The device according to claim 1 further including a secondary coupling comprising a trace disposed along said first transducer next to said first region and said second region.
  • 5. A spherical resonator device comprising:a resonant sphere; at least one transducer for electromagnetic coupling to said resonant sphere, said transducer comprising a flat metallized layer having a finite width shaped to provide exposure of the sphere to a quasi constant field, wherein said at least one transducer comprises a first region having a first width, a second region having a second width, a third region having a third width, a first transition region between said first region and said second region, a second transition region between said first region and said third region, said first region being adjacent said resonant sphere, said first width being at a minimum, said second region being displaced radially from said resonant sphere, said second width being at a maximum, said third region being displaced radially from said resonant sphere and opposite said second region, said second width being at a maximum, said first transition region bridging between said first region and second region, and said second transition region bridging between said first region and third region.
  • 6. The device according to claim 5 wherein said first transition region follows a first exponential profile of increasing width from said first region to said second region, said first exponential profile being selected to compensate for decrease in field strength of coupling between said resonant sphere and said transducer and to enhance bandwidth of resonant coupling, and wherein said second transition region follows a second exponential profile of increasing width from said first region to said third region, said second exponential profile being selected to compensate for decrease in field strength of coupling between said resonant sphere and said transducer and to enhance bandwidth of resonant coupling.
  • 7. The device according to claim 6 wherein said second width is substantially equal to said third width, and said first exponential profile is substantially equal to said second exponential profile.
  • 8. The device according to claim 5 wherein said second width is substantially equal to said third width.
  • 9. The device according to claim 5 further including a secondary coupling comprising a trace disposed along said first transducer next to said first region, said second region, and said third region.
US Referenced Citations (5)
Number Name Date Kind
4500858 Mezak Feb 1985 A
4543543 Blight et al. Sep 1985 A
4633205 Jones Dec 1986 A
6255918 Parrott et al. Jul 2001 B1
6348840 Ezura et al. Feb 2002 B2