Patent Grant
7609135
This invention relates to high isolation microwave frequency switching devices where signal routing is achieved via mechanical movement of conducting elements connected by an insulator.
As electronics speed moves into the multi-gigahertz regime, component dimensions are shrinking commeasurably. This causes devices to be more sensitive to electrical over-stresses via accidental exposure to unintended voltages. When test and measurement instruments are of low bandwidth such as those state-of-the-art oscilloscopes from a few years ago, many ultra fast single incidence high voltage spikes are essentially undetectable and overlooked. Their presence however, may have caused mysterious unexplained device failures. As oscilloscope bandwidth continued to increase, those ultra fast single-incidence events can now be captured with relative ease. This has led to the discovery of many unexpected voltage spikes generated by some seemingly-harmless structures.
One such anomaly is an unexpected voltage-spiking problem common in 26 GHz mechanical relays. High bandwidth instruments often require signal routing with minimum distortion and insertion loss through different paths for various purposes such as, changing attenuation, filtering, gain controlling, time delaying, phase referencing, etc. Although solid-state switching devices have gained ground in signal switching applications, mechanical relays are still preferred for switching broadband microwave signals where minimum signal distortion, low on-state insertion loss, low off-state signal feed-through, and smooth impedance transitions throughout the signal rerouting are required. Such mechanical relays typically use a studded center (output) connector with as many moveable satellite strip lines as that relay's number of throws. Each of the satellite movable strip lines starts at its corresponding individual connector and ends at the center common connector, and is controlled by a push rod mechanism to place that strip line section, one-at-a-time, to complete the signal path between the center connector and the corresponding satellite connector. The entire strip line structure is completely contained in a fully enclosed Faraday cage.
An exemplary RF relay structure in the 26 GHz bandwidth range is represented by the DB Products (Carson, Calif.) model 2SE1T11JA relay. This relay has been found to produce up to ˜20V peak 200 ps negative pulses each time the relay toggles. This spike voltage does not change polarity as one switches the relay back and forth.
A switching apparatus has a conductive housing forming a chamber. The housing has an aperture enabling communication between the chamber and a housing exterior. A rod extends through the aperture, and has a first end within the chamber, and an opposed second end outside the chamber. The rod reciprocates over a range of motion between a first position in which a limited portion of the rod extends into the chamber, and a second position in which a greater portion of the rod extends into the chamber. The rod has a electrically insulative portion electrically isolating the first end from the second end, and has a conductive surface contacting the housing. A pair of electrical contacts are located in the chamber, and a shorting bar connected to the first end of the rod operates to bridge the contacts when the rod is in a selected position.
Within the chamber a pair of shorting bars 42A, 42B serve to close or open connections between the input and the outputs. Bar 42A has opposed ends registered respectively with an input contact 44 connected to input line 32, and an output contact 46A connected to output line 34A (all input and output lines being electrically isolated from the cage at the push rod down position.) The bar 42A moves between a first open position (up position) in which the bar is spaced apart from the contacts 44 and 46A and a closed position. In the open position, the bar is in electrical contact with the housing wall and thus electrically grounded as shown in
Each shorting bar is supported at its midsection by a respective cylindrical push-rod 50A, 50B. Each push rod is closely received in a respective circular aperture 52A, 52B in a major wall of the cage opposite the wall on which the contacts are mounted. Each pushrod is formed of a non-conductive dielectric material (except as detailed below) to prevent electrical continuity between the supported shorting bar and the rest of the supporting system. Each pushrod has a free end 54A, 54B extending away from the cage. A pivoting armature 56 pivots about an axis fixed with respect to the cage, with opposed ends registered with the free ends of the push rods through a leaf spring attached to it. The armature pivots about a point A to ensure that one and only one of the shorting bars is in the closed position at any time (except for momentary transitions.)
The armature is acted upon by a pair of solenoids 60A, 60B that each operate in response to an applied drive signal to bear on and pivot the armature to bear on and actuate a respective push rod to make a connection with the respective shorting bar.
In the prior art, the disclosed relay has entirely non-conductive pushrods, which leads to a problem addressed by the preferred embodiment. As the prior art push rods move up and down due to the pressure from the armature, negative triboelectricity static charges are generated from friction between the insulating push rod and the surrounding metals it contacts. This static charge on the push rod attracts positive charges on the originally neutral shorting bar as it departs from its open position and moves toward the contacts. Because of the initially neutral condition, the induced positive charge pushes the same amount negative charge to the opposite side of the shorting bar. As the shorting bar moves to contact the contact points, the equal potential law forces the net negative free charge out of the Faraday cage and a net negative charge spike is emitted through the contacts with which the shorting bar just made contact. Depending on which contact is established first, the majority of, or all of, the negative charge is dissipated through that connector and may be observable as a voltage spike. As the relay switches, the selected shorting bar to the open position, the shorting bar retracts to the top of the chamber and contacts the inner surface of the housing. Meanwhile, the corresponding push rod also retracts back into the chamber wall's through hole aperture where the flux lines emitted from its negative charges will now be terminated by the aperture wall instead of the shorting bar. The disappearance of the flux lines into the shorting bar releases those induced positive charges and transforms them into free charges. Upon the shorting bar's contact to the chamber wall, those positive charges again are immediately discharged to the chamber wall as the negative charges did to the contacts earlier and the process can repeat without attenuation.
The push rod 50 includes a metal sleeve 86 that closely encompasses the first cylindrical portion and is captured at its ends by shoulders 72 and 80, which have a larger diameter than the interior bore of the sleeve. The sleeve has a flange 90 at the end adjacent to the head 66, and the flange has a diameter greater that the cage bore 52 so that the flange can capture the upper end of a concentric coil spring that provides the restoring force to the push rod when its top surface 70 is not pressed down by the armature leaf spring (the shorting bar and contacts in the cage normally limit the range of motion). The sleeve may preferably include a slit 92 running from end-to-end. This not only facilitates assembly by allowing the sleeve to expand to be forced over the second shoulder portion 76, but is also useful to suppress a potential resonance mode that could absorb electrical energy from the passing microwave signals during operation at certain frequencies.
As shown in the right portion of
In the preferred embodiment, the dielectric spindle 62 is formed of PCTFE, has a length of 0.205 inch a head 66 diameter of 0.125 inch, a first cylindrical portion 74 length of 0.150 inch, a diameter of 0.067 inch, and a second shoulder portion diameter of 0.0725 inch.
The cage aperture 52 has a diameter of 0.093 inch. The sleeve is formed of brass, and has an overall length of 0.155 inch, an inside diameter of 0.07 inch, a flange diameter of 0.125 inch, and a wall thickness of 0.010 inch The switch is designed to avoid any contact between the plastic portions of the push rod and the cage, so that no charge can be accumulated due to friction. All contact between the push rod assembly and the cage is metal-to-metal. To relieve some friction between the metal sleeves and their corresponding barrel walls, and also to dissipate any static charges that might ever start to accumulate on the dielectric surfaces, an imperfectly insulating (slightly conducting) material such as Progold (from Caig Labs, Poway, Calif.) is applied to the exposed dielectric surface as well as to the metal sleeve exterior and interior. In addition to lubricating the sleeves as they travel up and down the barrels, this also allows any charge on the dielectric surface to be dissipated to the cage before any substantial charge amount can accumulate.
In alternative embodiments, the sleeve may be functionally replaced by plating the first cylindrical portion with a metal surface that prevents contact with the cage by anything but the conductive plating. To provide the slot 92, the plastic spindle may have a recessed groove so that thin film deposition can not fill that gap and, which effectively forms an electrical discontinuity for resonance suppression purpose. Also, the shoulder 72 facing the outer surface of the cage may preferably be plated, as may any shoulder or corner at the leading edge of the dielectric portion where the spindle transitions to a smaller diameter where the surface is unplated and rebated away from the cage aperture surface. In a further alternative embodiment, the cage aperture may have a larger diameter portion adjacent the interior of the cage to avoid possible contact with the unplated portion of the pushrod. In a further alternative embodiment, the spindle need not be dielectric material over its entire length. The sleeve portion may be a solid metal bushing, with a dielectric isolator mechanically connecting and electrically isolating the bushing from the shorting bar.
In a further alternative embodiment suited for applications seeking lower cost and complexity, and with less sensitivity to the electrical discharge concerns discussed above, the metal sleeve is omitted and the diameter of the dielectric section 74 is extended to a cross sectional profile comparable to the outside diameter of the metal sleeve 86 shown in
A transition shoulder 106 between the main and reduced portions is positioned a limited distance form the head 66, so that at the down stroke position (when the corresponding contacts are shorted by shorting bar 42) the shoulder remains within the bore 52, and does not extend into the chamber 40. Similarly, the main portion 102 remains at least slightly recessed within the bore in all conditions. The whole push rod assembly is then coated with an imperfect insulating material such as a thin coating of 5% Progold such as discussed above. In this arrangement, the dielectric rod section that will enter the Faraday cage not only will not have an opportunity to generate triboelectricity, but also will dissipate any surface charges that may have been there via the finite conductivity of the coated material.
Surface charge is also significantly reduced for the upper section of the dielectric rod that does come in contact with the aperture wall because of the enhanced conductivity provided by the Progold coating. Surface charge may still be present at the surface of the spindle that rubs against the cage bore wall. However, any accumulated charge does not enter the Faraday cage cavity. As a result, all field lines originating from such dielectric rod surface charges are terminated by the grounded barrel wall, and no electric flux lines enter the contact chamber. This eliminates induced charges on the shorting bar and thus eliminates the voltage spiking phenomenon during relay switching.
In another alternative embodiment, the dielectric rod is made of a low but finite conductivity material of low dielectric loss and dielectric constant. Similar to the above arguments, voltage spiking can also be effectively suppressed.
While the above is discussed in terms of preferred and alternative embodiments, the invention is not intended to be so limited.
The subject patent application claims priority from U.S. Provisional Patent Application Ser. No. 60/562,636, entitled, METHOD AND APPARATUS FOR ELIMINATION OF VOLTAGE TRANSIENT DURING SWITCHING OF AN RF RELAY (Yang) filed 14 Apr. 2004, and also from U.S. Provisional Patent Application Ser. No. 60/583,105, entitled, METHOD AND APPARATUS FOR ELIMINATION OF VOLTAGE TRANSIENT DURING SWITCHING OF AN RF RELAY (Yang) filed 24 Jun. 2004.
| Number | Name | Date | Kind |
|---|---|---|---|
| 4298847 | Hoffman | Nov 1981 | A |
| Number | Date | Country | |
|---|---|---|---|
| 20050231307 A1 | Oct 2005 | US |
| Number | Date | Country | |
|---|---|---|---|
| 60562636 | Apr 2004 | US | |
| 60583105 | Jun 2004 | US |
