Millimeter wavelength dielectric waveguide having increased power output and a method of making same

• US 4,665,660 A
• Filed: 06/19/1985
• Issued: 05/19/1987
• Est. Priority Date: 06/19/1985
• Status: Expired due to Fees

• Current Assignee: the united states of america as represented by the secretary of the navy
• Original Assignee: the united states of america as represented by the secretary of the navy
• Inventors: Jablonski, Daniel G., Krall, Albert D.
• Primary Examiner(s): Schmidt, Frederick R.
• Assistant Examiner(s): RACHUBA, MAURINA T
• Application Number:
  US06/746,483
• Time in Patent Office: 699 Days
• Field of Search: 51/281 R, 51/289 R, 51/290, 333/239, 333/240, 333/241, 333/242, 333/248, 29/600, 350/96.3
• US Class Current: 451/28
• CPC Class Codes: B24B 1/00 Processes of grinding or polishing; Use of auxiliary equipment in connection with such processes
• CPC Class Codes: H01P 3/16 Dielectric waveguides, i.e. without a longitudinal conductor
• CPC Class Codes: H01Q 1/002 Protection against seismic waves, thermal radiation or other disturbances, e.g. nuclear explosion; Arrangements for improving the power handling capability of an antenna
• CPC Class Codes: H01Q 13/24 constituted by a dielectric or ferromagnetic rod or pipe H01Q13/28 takes precedence
• CPC Class Codes: Y10T 29/49016 Antenna or wave energy "plumbing" making

Abstract

A millimeter wavelength solid dielectric waveguide having either an undulng or roughened outer surface is disclosed. As configured, and properly designed, for the wavelength of interest, the non-cylindrical surface will not have any deleterious effects on the electromagnetic properties of the dielectric waveguide. Moreover, the novel surface treatment will greatly increase the amount of heat energy that can be dissipated by radiation and convection from the dielectric waveguide thereby increasing its power handling capability.

Claims

1. A method of fabricating a solid dielectric waveguide configured to operate at a predetermined frequency within a predetermined range, so as to improve its power handling capability without deleteriously effecting its electromagnetic properties, comprising the steps of:

furnishing a cylindrical dielectric waveguide of a predetermined dielectric material, said cylindrical dielectric waveguide having a predetermined maximum diameter d, a length l and a smooth outer surface; and

modifying the smooth outer surface of said cylindrical dielectic waveguide to conform to an undulating outer surface characterized by ridges and valleys, said ridges and valleys increasing the effective surface area of the waveguide and providing means for increasing the heat energy that can be dissipated in the waveguide without adversely effecting the waveguides electromagnetic properties in the frequency range of interest, said ridges and/or valleys being spaced according to a predetermined surface wavelength λ

_s, and said ridges being at a predetermined maximum diameter d.

2. The method of claim 1 comprising the additional step of selecting the predetermined dielectric material from a group consisting of polytetraflouroethylene (PTFE), polystyrene and fused quartz.

3. The method of claim 2 comprising the additional step of choosing the predetermined maximum diameter d according to the inequality.

d<

d_c, where d_c is the critical diameter for dominant mode operation.

4. The method of claim 3 comprising the additional step of modifying the diameter of said cylindrical dielectric waveguide as a function of a position "z" along its length l according to the equation:

d(z)=d_avg +(Δ

d/2)(sin 2π

z/λ

_s), where d_avg is the average diameter of said cylindrical dielectric waveguide after modifying, and is d_avg =d-Δ

d/2, where d is the predetermined maximum diameter and Δ

d is the change in diameter between any one of said ridges and its adjacent valley, where π

is the number 3.1415 . . . , and λ

_s is the predetermined surface wavelength.

5. The method of claim 4 comprising the additional step of choosing the predetermined surface wavelength according to the inequality:

λ

_s <

(λ

/λ

₀)λ

₀ /[1+(λ

/λ

₀)], where λ

is the wavelength of a signal frequency f being propagated along said cylindrical dielectric waveguide, and λ

₀ is the wavelength of the same signal frequency in free-space.

6. The method of claim 5 wherein the predetemined frequency is in the range of 30 to 300 GHz.

7. The method of claim 1 wherein said modifying step is accomplished by machining.

8. The method of claim 1 wherein said modifying step is accomplished by rubbing the smooth outer surface of said cylindrical dielectric waveguide with an abrasive paper so as to create a roughened outer surface of random or psuedorandom variations.