US3702979A

US3702979A - Rotary vane attenuator wherein rotor has orthogonally disposed resistive and dielectric cards

Info

Publication number: US3702979A
Application number: US193947A
Authority: US
Inventors: Charles T Stelzried; Tom Y Otoshi; David L Nixon; Robert W Beatty
Original assignee: National Aeronautics and Space Administration NASA
Current assignee: National Aeronautics and Space Administration NASA
Priority date: 1971-10-29
Filing date: 1971-10-29
Publication date: 1972-11-14
Anticipated expiration: 1989-11-14

Abstract

A rotary vane attenuator is described, comprising two stators and an intermediary rotor, each with a resistive card. The rotor, in addition to the resistive card, includes an orthogonally disposed card of dielectric material which has no resistive film thereon.

Description

United States Patent Fletcher et a].

[ 1 ROTARY VANE A'ITENUATOR WHEREIN ROTOR HAS ORTHOGONALLY DISPOSED RESISTIVE AND DIELECTRIC CARDS Inventors: James C. Fletcher, Administrator of the National Aeronautics and Space Administration with respect to an invention of; Charles T. Stelzried, La Crescenta; Tom Y. Otoshi, La Canada; David L. Nixon, Arcadia, all of Calif.; Robert W. Beatty, Boulder, Colo.

Filed: Oct. 29, 1971 Appl. No.: 193,947

US. Cl ..333/81 B, 333/98 R int. Cl. ..H0lp 1/22 [451 Nov. 14, 1972 [58] Field of Search ..333/81 B, 98 M [56] References Cited UNITED STATES PATENTS 2,542,185 2/1951 Fox ..333/81 B 2,603,710 7/l952 Bowen...... ..333/81 B Primary Examiner Paul L. Gensler AttorneyMonte F. Mott et a1.

[5 7] ABSTRACT A rotary vane attenuator is described, comprising two stators and an intermediary rotor, each with a resistive card. The rotor, in addition to the resistive card, includes an orthogonally disposed card of dielectric material which has no resistive film thereon.

4 Claims, 3 Drawing Eigures RESISTIVE PATENTEDNuv 14 I972 PRIOR ART E COS G Esme ecose E 0089 E C089 SING- CHARLES D. STELZRIED OTOSHI DAVID L. NIXON -ROBERT w. BEATTY INVENTORS 3O-DIELECTRIC W/Wg 5/ /J W ATTORNEYS ROTARY VANE ATTENUATOR WI-IEREIN ROTOR HAS ORTHOGONALLY DISPOSED RESISTIVE AND DIELECTRIC CARDS ORIGIN OF THE INVENTION The invention described herein was made in the performance of work under a NASA contract and is subject to the provisions of Section 305 of theNational Aeronautics and Space Act of 1958, Public Law 85- 568 (72 Stat. 435; 42 U.S.C. 2457).

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to attenuators and, more particularly, to a rotary vane attenuator of reduced size and weight and which exhibits small phase shift over the attenuators dynamic range.

2. Description of the Prior Art At present various attenuators for energy in the microwave range are well known. These include the rotary vane (RV) attenuator. Basically such an attenuator consists of three sections of a waveguide arranged in tandem. The two outer sections are fixed and are known as stators and the middle section, which is free to rotate axially with respect to the stators, is known as the rotor. The latter is generally a round or cylindrical guide of short length, while. each of the stators is generally a rectangular-to-round waveguide. In each section a resistive film card is placed across the guide. In the stators the resistive film cards are normal to the field of the applied wave. The construction is symmetrical and the device is bidirectional.

Two of the basic disadvantages of such an attenuator is its significant length and the phase shift which varies as a function of signal frequency. These two disadvantages greatly complicate attenuation calibration which is very undesirable whenever precise attenuation, as a function of rotor rotation angle, is required.

OBJECTS AND SUMMARY OF THE INVENTION It is a primary object of the present invention to provide a new improved rotary vane attenuator.

Another object is to provide a compact precision rotary vane attenuator.

A further object of the present invention is to provide a new rotary vane attenuator in which phase shift is substantially independent of signal frequency.

These and other objects of the invention are achieved by providing a rotor in which, in addition to the resistive card, a dielectric card is placed orthogonally with respect to the resistive film card. It should be stressed that the dielectric card does not have any resistive film, deposited thereon. It has been discovered that the addition of the dielectric card enables the reduction of the attenuator length, and the phase shift is substantially independent of frequency. That is, any phase shift which is experienced is substantially constant over a significant portion of the attenuators dynamic range.

The novel features of the invention are set forth with particularity in the appended claims. The invention will best be understood from the following description when read in conjunction with the accompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is an isometric view of a prior art rotary vane attenuator;

FIG. 2 is a diagram of E field vectors; and

FIG. 3 is an isometric view of the attenuator of the present invention.

DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 is an isometric view of one type of a conventional rotary vane attenuator 10, shown comprising

stators

12 and 13 between which a rotor 14 is positioned. The three sections are aligned along an axial axis 15. Positioned in each section is a resistive film card. The three cards in sections 12-14 are designated by

numerals

22, 23 and 24, respectively.

The operating principle of. this type attenuator may be described in conjunction with FIG. 2 wherein the E field vectors at the input and output of each section are shown. When all resistive film cards are aligned, the field of the applied wave is normal to the card. Thus no current flows in the resistive film and no attenuation occurs. If however, the rotor 14 is rotated so that card 24 forms an angle 0 with

cards

22 and 23, the E field can be considered as split between two components; E sin 0 in the plane of card 24 and E cos 0 at a right angle thereto. The Esin 0 component is absorbed in card 24 while the E cos 6 component passes unattenuated to stator 13. When it encounters card 23, the E cos 6 component is split into two components; E cos 6 sin 6 in the plane of card 23 and E cos 0 perpendicular thereto. Thus the E cos 0 sin 0 component is absorbed by the resistive film on card 23 and the E cos 6 emerges from stator 13 at the same orientation as the original wave which entered stator 12. Thus ideally attenuation is proportional only to angle 0 at which the center card 24 (or rotor 14) is rotated about axis 15 with respect to

stators

12 and 13. However, in practice it has been discovered that attenuation is frequency dependent due to the phase shift which is a function of frequency.

Phase shift and finite attenuation in' the rotor vane can be measured and accounted by the expression sin 0 cos 6+ sin 6 2 cos cos 0+- In situations where this is not possible, for example, in a precision rotary vane attenuator, where the highest accuracy is required or reduced weight and/or size is important, equation (1) is especially valuable. However, since (I: is frequency dependent, calibration of the rotary vane attenuator is very difficult.

It has been discovered that significant improvement in the attenuation is achieved by inserting an additional card in the rotor 14 which is orthogonally positioned with respect to the resistive film card 24. The added orthogonally positioned card however does not support a resistive film, as does card 24. Rather, the added card is of dielectric material without any conductive film thereon. Such an arrangement is shown in FIG. 3 in which the added card without a resistive film, is designated by numeral 30.

The incorporation of the dielectric card in the rotor has resulted in substantially constant phase shift with frequency, particularly with X-band attenuators. It has been discovered that with the knowledge of phase shift 1 and L in equation (1), the length of the attenuator need not be made great as is the case in the prior art. Thus, the overall size of the attenuator can be greatly reduced without sacrificing precision in attenuation. Also once the phase shift is known, the attenuator-can be easily calibrated for the entire dynamic range.

Although a particular embodiment of the invention has been described and illustrated herein, it is recognized that modification and variations may readily occur to those skilled in the art and consequently it is intended that the claims be interpreted to cover such modifications and equivalents.

What is claimed is:

1. In a rotary vane attenuator of the type including first, second and third waveguide sections aligned along a selected axis, with said first and third sections being stationary and said second center section being rotatable about said axis, with said first and third sections supporting electrically conductive means in a common plane extending through said axis and said second section supporting electrically conductive means in a plane extending through said axis, the improvement comprising:

dielectric means in said second section extending orthogonally to the electrically conductive means which is supported in said second section, in a plane which passes through said selected axis.

2. The arrangement as recited in claim 1 wherein the electrically conductive means in each of said sections is a flat card with a resistive film thereon, and said dielectric means in said second section is a card of dielectric material which is not coated by a resistive film.

3. The arrangement as recited in claim 2 wherein each of the cards extends the length of the section in which it is supported, and at least the second section is cylindrical with its longitudinal axis coinciding with said selected axis.

4. A rotary vane attenuator comprising:

a first waveguide section having a longitudinal axis extending along and coinciding with a preselected axis;

a first card with resistive film thereon, supported in said first waveguide section in a first plane which extends through said preselected axis, said first waveguide section being'fixedly positioned about said preselected axis;

a second waveguide section, spaced from said first section, and having a longitudinal axis extending along and coinciding with said preselected axis;

a second card with a resistive film thereon, supported in said second section in said first plane which extends throughsaid preselected axis; a third waveguide section between said first and second sections and having a longitudinal axis which extends along and coincides with said preselected axis, said third section being rotatable about said preselected axis;

a third card with a resistive film thereon, supported in said third section in a plane which extends through said preselected axis; and

a fourth card of dielectric material, which does not include a resistive film thereon, supported in said third section in a plane perpendicular to the plane in which the third card is supported, and which extends through said preselected axis.

Claims

1. In a rotary vane attenuator of the type including first, second and third waveguide sections aligned along a selected axis, with said first and third sections being stationary and said second center section being rotatable about said axis, with said first and third sections supporting electrically conductive means in a common plane extending through said axis and said second section supporting electrically conductive means in a plane extending through said axis, the improvement comprising: dielectric means in said second section extending orthogonally to the electrically conductive means which is supported in said second section, in a plane which passes through said selected axis.

4. A rotary vane attenuator comprising: a first waveguide section having a longitudinal axis extending along and coinciding with a preselected axis; a first card with resistive film thereon, supported in said first waveguide section in a first plane which extends through said preselected axis, said first waveguide section being fixedly positioned about said preselected axis; a second waveguide section, spaced from said first section, and having a longitudinal axis extending along and coinciding with said preselected axis; a second card with a resistive film thereon, supported in said second section in said first plane which extends through said preselected axis; a third waveguide section between said first and second sections and having a longitudinal axis which extends along and coincides with said preselected axis, said third section being rotatable about said preselected axis; a third card with a resistive film thereon, supported in said third section in a plane which extends through said preselected axis; and a fourth card of dielectric material, which does not include a resistive film thereon, supported in said third section in a plane perpendicular to the plane in which the third card is supported, and which extends through said preselected axis.