Waveguide transitions and method of forming components

• US 7,893,789 B2
• Filed: 12/12/2006
• Issued: 02/22/2011
• Est. Priority Date: 12/12/2006
• Status: Expired due to Fees

• Current Assignee: CommScope Technologies, LLC (CommScope Holding Company, Inc.)
• Original Assignee: Andrew LLC (CommScope Holding Company, Inc.)
• Inventors: Paynter, Jeffrey
• Primary Examiner(s): CHO, JAMES HYONCHOL
• Application Number:
  US11/637,478
• Publication Number:
  US 20080136565A1
• Time in Patent Office: 1,533 Days
• Field of Search: 333/21.R, 333 33- 34, 333/248
• US Class Current: 333/21.00R
• CPC Class Codes: B22D 17/007 Semi-solid pressure die casting
• CPC Class Codes: H01P 1/162 absorbing spurious or unwanted modes of propagation
• CPC Class Codes: H01P 5/082 Transitions between hollow waveguides of different shape, e.g. between a rectangular and a circular waveguide

Abstract

A waveguide transition for transitioning from an overmoded waveguide to another waveguide is provided, where one end of the waveguide is configured to connect to a rectangular waveguide and the other end is configured to connect to an elliptical waveguide. The transition has an internal shape having top and bottom walls and two side walls. The top and bottom walls are shaped to join smoothly with waveguides at each end of the transition, while the side walls diminish in height along the length of the transition. The waveguide transition may employ mode filtering to suppress unwanted higher modes. A method of forming waveguide components is also disclosed, involving thixoforming of components in single pieces, the components having internal shapes configured for mold core removal.

Claims

1. A waveguide transition for transitioning from a rectangular waveguide to an elliptical waveguide, at least one of the waveguides being an overmoded waveguide, the transition having a transition passage, said transition passage including:

i. a rectangular end having a rectangular cross-section and an elliptical end having an elliptical cross-section, at least one of the rectangular and elliptical ends having a cross-section dimensioned to support overmoded transmission; and

ii. internal top, bottom and side walls connecting the rectangular end and the elliptical end;

wherein;

a. the cross-sectional shape of the top and bottom walls varies continuously between straight at the rectangular end and semi-elliptical at the elliptical end;

b. the top and bottom walls are shaped to join smoothly with a passage of rectangular cross-section at the rectangular end and with a passage of elliptical cross-section at the elliptical end;

c. the cross-sectional shape of the side walls is straight or convex at all points between the rectangular end and the elliptical end, the height of the side walls diminishing continuously along the length of the transition, being larger at the rectangular end than at the elliptical end;

d. the side walls are shaped to join smoothly with a passage of rectangular cross-section at the rectangular end; and

e. the transition passage is configured to support a mode filter by further including one or more slots formed in the internal walls.

2. A waveguide transition as claimed in claim 1 wherein a slot is formed in each internal side wall, the slots being configured to receive a mode filter and retain it in the H plane.

3. A waveguide transition as claimed in claim 1 wherein the slots open onto the elliptical end, allowing a mode filter to be slid into the slots from the elliptical end.

4. A waveguide transition as claimed in claim 1, wherein:

each of the top and bottom walls defines a smooth curve in the E plane between the rectangular end and the elliptical end, the curve being capable of definition by an equation of lateral displacement from the axis of the transition as a function of displacement along the length of the transition; and

the first derivative of that equation is zero at each end of the transition and the second derivative of that equation changes sign along the length of the transition.

5. A waveguide transition as claimed in claim 4 wherein the equation is given by:

D=(B/2)cos²(π

z/2L)+b sin²(π

z/2L)

where D is the lateral displacement of the top or bottom wall from the transition axis in the E plane, B is the height at the rectangular end, b is the semi-minor axis at the elliptical end, z is the displacement along the length of the transition from the rectangular end, and L is the total length of the transition.

6. A waveguide transition as claimed in claim 5 wherein the cross-sectional shape of each of the top and bottom walls at any point between the rectangular and elliptical ends is substantially that of an elliptical arc, the arc satisfying the elliptical equation:

(x²/C²)+(y²/D²)=1

where C=a/[sin(π

z/2L)], and a is the semi-major axis at the elliptical end.

7. A waveguide transition as claimed in claim 1, wherein:

each of the side walls defines a smooth curve in the H plane between the rectangular end and the elliptical end, the curve being capable of definition by an equation of lateral displacement from the axis of the transition as a function of displacement along the length of the transition; and

the first derivative of that equation is zero at the rectangular end of the transition.

8. A waveguide transition as claimed in claim 7 wherein the equation is given by:

X=a−

(a−

A/2)cos[(π

z/2L)]

where X is the lateral displacement of the side wall from the transition axis in the H plane, a is the semi-major axis at the elliptical end, A is the width of the rectangular end, z is the displacement along the length of the transition from the rectangular end, and L is the total length of the transition.

9. A waveguide transition as claimed in claim 1 wherein the cross-sectional shape of each of the top and bottom walls at any point between the rectangular and elliptical ends is substantially that of an elliptical arc, the eccentricity of the elliptical arc diminishing along the length of the transition.

10. A waveguide transition as claimed in claim 1 for transitioning from a rectangular dominant mode waveguide to an elliptical overmoded waveguide, the rectangular end having a cross-section dimensioned to support dominant mode transmissions in a frequency range and the elliptical end having a cross-section dimensioned to support overmoded transmissions in the frequency range.

11. A waveguide transition as claimed in claim 1 wherein the height of the side walls diminishes substantially to zero at the elliptical end.

12. A manufacturing method comprising:

i. casting the waveguide transition of claim 1 by employing a thixoforming process; and

ii. establishing a mode filter within the transition passage.

13. A waveguide system including:

i. a dominant mode input;

ii. a dominant mode output;

iii. a length of overmoded waveguide between the dominant mode input and the dominant mode output;

iv. a first waveguide transition transitioning from the dominant mode input to the overmoded waveguide; and

v. a second waveguide transition transitioning from the overmoded waveguide to the dominant mode output;

wherein at least one of the first and second waveguide transitions is a waveguide transition as claimed in claim 1.

14. A waveguide transition comprising:

i. a casting defining an internal passage extending therethrough having a first end of rectangular cross-section and a second end of non-rectangular cross-section, the cross-section of said passage at one of the first and second ends being shaped and dimensioned to support dominant mode transmissions at a signal frequency, and the cross-section of said passage at the other of the first and second ends being shaped and dimensioned to support overmoded transmissions at the signal frequency; and

ii. a metallic mode filter mounted within said passage and configured and positioned to suppress unwanted higher modes more than signals at the signal frequency.

15. The waveguide transition of claim 14 wherein the metallic mode filter is a mode filter card longitudinally mounted to bisect said passage.

16. The waveguide transition of claim 15 wherein the metallic mode filter card comprises a metallic coating formed on a substrate.

17. The waveguide transition of claim 14, wherein the waveguide transition further comprises thixoformed material for low cost and lightweight, said internal passage having walls of such smoothness as to minimize creation of surface-induced mode conversions in the passage.

18. A waveguide transition of claim 14 in the form of a one-piece casting having slots on opposed sides of said passage located and configured to receive said mode filter.

19. The waveguide transition of claim 18 wherein the slots are formed in opposing internal walls of the transition without penetrating to the exterior through those walls.

20. The waveguide transition of claim 14 wherein said passage transitions between rectangular cross-section at the first end and elliptical cross-section at the second end, and wherein opposed first and second passage walls are concave and characterized by a first derivative being substantially zero at the first and second ends of the passage, and by a second derivative changing sign between the first and second ends of the passage.

21. The waveguide transition of claim 14 wherein said passage transitions between rectangular cross-section at the first end and elliptical cross-section at the second end, and wherein opposed third and fourth passage walls are characterized by a first derivative being substantially zero at the first end of the passage, and by said third and fourth walls flaring out from the first end to the second end of the passage and reducing in height substantially to zero at the second end of the passage.

22. The waveguide transition of claim 14, wherein the waveguide transition further comprises a one-piece casting of thixoformed material for low cost and light weight, said passage having walls of such smoothness as to minimize creation of surface-induced mode conversions in the passage and having slots on opposed sides thereof located and configured to receive said mode filter.

23. The waveguide transition of claim 22 wherein said passage transitions between rectangular cross-section at the first end and elliptical cross-section at the second end, and wherein opposed first and second passage walls are concave and characterized by a first derivative being substantially zero at the first and second ends of the passage, and by a second derivative changing sign between the first and second ends of the passage.

24. The waveguide transition of claim 23 wherein said passage transitions between rectangular cross-section at the first end and elliptical cross-section at the second end, and wherein opposed third and fourth passage walls are characterized by a first derivative being substantially zero at the first end of the passage, and by said third and fourth walls flaring out from the first end to the second end of the passage and reducing in height substantially to zero at the second end of the passage.

25. The waveguide transition of claim 22 wherein the transition is tapered from a narrow end to a wide end and wherein the slots open onto the wide end of the transition, the internal shape formed thereby being configured for removal of a mold core.

26. The waveguide transition of claim 14 wherein the metallic mode filter extends along a portion of the internal passage in which unwanted higher modes are able to exist.

27. The waveguide transition of claim 26 wherein the metallic mode filter card extends along about 75% of the length of the transition, from the end shaped and dimensioned to support overmoded transmissions.

28. A waveguide system including:

i. a dominant mode input;

ii. a dominant mode output;

iii. a length of overmoded waveguide between the dominant mode input and the dominant mode output;

iv. a first waveguide transition transitioning from the dominant mode input to the overmoded waveguide; and

v. a second waveguide transition transitioning from the overmoded waveguide to the dominant mode output;

wherein at least one of the first and second waveguide transitions is a waveguide transition as claimed in claim 14.