This invention relates to tubular substrates having electrical conductors on an interior surface that are electrically connected through the tube wall to contacts on the tube exterior. Preferably, the conductors are concentric rings for a drift tube of an Ion Mobility Mass Spectrometer (IMS). This invention further relates to methods for producing such tubular substrates from flexible polymeric printed wiring board materials, ceramic materials and material compositions of glass and ceramic, commonly known as Low Temperature Co-Fired Ceramics (LTCC).
In the context of the present invention, LTCC is generally defined as a family of glass-ceramic dielectric substrate materials that are flexible and formable in the ‘green’ unfired state, and become rigid upon firing at temperatures below 1000° C. Such dielectric materials are widely used in the art and are supplied as flexible green sheets or tapes. Conductors, resistors, via fills, inductive and capacitive structures are incorporated in or printed on the LTCC dielectrics using compatible inks or pastes by processes well known in the art. These materials and recommended processing methods are well known and available commercially from Electro-Science Laboratories, INC, King of Prussia, Pa., the DuPont Company, Wilmington, Del. and Ferro Corporation of Cleveland, Ohio, among others.
An IMS is an analytical instrument that performs vapor phase compound speciation based on ion mobility in an atmospheric environment. Uses for an IMS include analyzing air samples for the presence of harmful substances in the form of toxic vapors, components of explosive materials, trace constituents of drugs, sampling of biological systems such as biogenic amines or fatty acid methyl esters, or other analytical chemistry applications. In a typical configuration, an IMS consists of a drift tube with drift gas inlet at one end, connected to an ionizing chamber at the opposed end, the ionizing chamber being provided with a sample gas inlet port. Gating grid electrodes are located between the drift tube and the ionizing region. An exhaust outlet for gases is provided for near the ionizing chamber and away from the gating electrodes. The drift gas, typically dry air, nitrogen or other inert gas, flows along the drift tube, past the sample inlet port, through the ionizing region and exits via the exhaust outlet. The sample to be analyzed is introduced along with a carrier gas, typically dry air, nitrogen or other inert gas, through the sample inlet port into the ionizing region where isotopic radiation, corona discharge sources, ultraviolet radiation or other known ionization techniques, ionize the constituents of the carrier and sample gases either by primary ionization of the analyte or secondary ionization by chemical reaction with a supplied dopant. Ions created in the ionizing region are attracted towards the entrance of the drift tube by the presence of an electric field. By applying a voltage pulse on gating grid electrodes separating the ionizing region from the drift tube, a controlled flow of ions is allowed into the drift tube, along which a generally linear potential gradient has been established. Ions within the drift tube are accelerated by the potential gradient and migrate against the drift gas flow, towards the ion detector. The rate or drift speed (Vd) at which ions migrate through the drift tube is controlled by their mobility (K) and the magnitude of the electric field (E) according to the following relationship Vd=KE. The ion's mobility is a generalized parameter that includes effects such as charge, collision cross-section, reduced mass of the ion-neutral collision pair, ion polarizability, temperature, and other variables. Chemical speciation is achieved by electronic circuits which monitor the ions collected on the detector, as a function of time passed since application of the voltage pulse to the gating electrodes. The resulting waveforms representing the number of ions collected versus time are well known to be indicative of the chemical species and their relative quantities, present within the gas sample being analyzed.
The construction of the drift tube, field and gating electrodes, ionizing region, gas inlet and exhaust port attachments, has significant impact in determining the size, cost, and performance of the IMS as a practical instrument. To achieve an optimized IMS, it is desired that the drift tube assembly be relatively small in size, airtight, constructed of non-contaminating materials, and of low cost to produce.
The following references teach several approaches for construction of the drift tube and it's associated components.
U.S. Pat. No. 4,390,784 to Browning et al discloses an ion accelerator for an ion mobility detector cell that is comprised of a ceramic tube coated inside with a thick film resistor composition across which a voltage potential difference is impressed to provide an ion accelerating electrical field gradient within the tube. One such tube is used to define the mobility detector reactant region and a second similar tube is used to define the drift region. Gating grid electrodes are provided by wire screens or mesh, contained in a separate mechanical assembly of many parts, placed inside the ceramic tube. This approach provides a functional system albeit one that is not amenable to miniaturization or low cost of manufacture.
U.S. Pat. No. 5,280,175 to Karl discloses a drift tube produced by stacking metal ring electrodes separated by insulating rings. The stack-up of conducting and insulating rings would be sealed with conventional o-rings, or brazed into an airtight assembly. To provide a voltage divider for creating a potential gradient along the drift tube, the ring electrodes would be interconnected with deposited or discrete resistor elements. The use of brazing to join the piece parts would produce a relatively inert, non-contaminating drift tube but requires a complicated assembly process.
U.S. Pat. No. 5,965,882 discloses a drift chamber created in the space between two printed wiring boards, separated by a Teflon™ spacer. Necessary electrodes are provided on the printed wiring boards and sealing of the drift chamber is accomplished by mechanical compression of the Teflon™ spacer. Systems constructed of such organic materials can be troubled with outgassing of contaminants from these materials, and may require extended flushing of the system to achieve optimum sensitivity.
U.S. Pat. No. 6,051,832 discloses a volume enclosure built up upon the surface of a printed wiring board by soldering a multiple of stamped metal assemblies onto it. A larger metal stamping is used to form the drift tube enclosure. Additional stampings are located within this volume and function as the electrode elements, interconnected by surface mounted discrete resistors. The joints within this structure are soldered to create an airtight enclosure. This system provides for integrating the electronics near the drift tube, but again requires a complex assembly process.
The applicants have described yet another approach to producing the drift tube assembly in the publication: “Applying New LTCC/LIGA Construction Techniques in Realizing a Miniature Ion Mobility Spectrometer”, presented at the conference on Packaging of MEMS and Related Micro Integrated Nano Systems, sponsored by the International Microelectronics and Packaging Society, Sep. 7, 2002, Denver, Colo. This publication discloses an approach to miniaturizing an IMS by constructing a drift tube of alternately stacked sapphire insulators each having a centrally located hole, with thin metal plates each having a centrally located hole or screen feature to function as an electrode. In this approach, the many alternating layers of insulator and metal electrode plates are joined with adhesives or metallurgically bonded through brazing or soldering, to produce an airtight assembly. Machined blocks of ceramic or similar material are bonded at each end of the drift tube to provide inlet and exhaust gas ports and provide for the ionizing and reaction regions. Manufacture of such a device proved successful, but was labor intensive and prone to leakage, as is typical for a structure with a large number of joints, each required to be airtight. A need exists for a simpler method for producing a structure usable as the drift region of an IMS, that preferably would entail non-contaminating materials and minimize the number of airtight joints required.
It is desired to provide a method of forming tubular substrates beginning with readily available planar sheets of ceramic, glass-ceramic or suitable polymeric materials. The following references teach several approaches for forming three-dimensional structures in ceramic materials.
U.S. Pat. No. 3,755,891 to Muckelroy et al discloses a method for producing three-dimensional circuit modules utilizing thick-film manufacturing processes applied to the inner and outer surfaces of a provided substrate in the form of a ceramic cylinder. Circuit networks are printed on the inside and outside of the cylindrical substrate, utilizing screen printers having similarly shaped cylindrical screens. After firing of the circuit networks, interconnection is effected by conductive clips extending from conductors on the inner surface of the cylinder to conductors on the outer surface. While a method as taught by Muckelroy et al might provide a basis for developing a drift chamber, the requirement to print networks on the interior of a tube is difficult to manufacture, and necessarily restricts the process to tubular structures with a large inner diameter, to accommodate the screen printing means.
U.S. Pat. No. 4,475,967 to Kanai et al teaches a method for producing a ceramic capacitor by rolling a sheet of green ceramic material about a core. A conductor pattern of alternating electrodes, separated by insulating gaps, is printed on one surface of the green ceramic sheet. By eliminating the necessity to maintain accurate alignment of two green ceramic sheets, problems attributed to miss-alignment of the sheets could be avoided, such as increasing the scatter of capacitance values produced or short-circuits developing between the electrode patterns. Kanai et al does not provide a method for interconnecting inner and outer electrodes as these ‘short-circuits’ would be deleterious to producing a capacitor, and is cited as a disadvantageous by-product of processes requiring accurate alignment of two green ceramic sheets.
U.S. Pat. No. 5,028,473 to Vitriol et al discloses forming an electrical circuit pattern on a glass-ceramic thermally fusible tape. The tape is heated to a temperature at which it becomes temporarily plastic, and is then bent into a desired non-planar shape. A multi-layer structure can be provided by laminating together plural layers of LTCC tape with respective circuit patterns formed thereon, and plastically bending the laminated structure into the non-planar shape during a heating step. Interconnection of circuit patterns on different tape layers is by means of electrical vias formed through a tape layer. By this method, a circuit structure including a desired edge connector can be formed into a non-planar shape. Examples of bending glass-ceramic tape by heating the tape and shaping or pressing the softened tape about a mold form are provided. While this method can produce a shaped substrate, this method requires handling of glass-ceramic substrates heated to their softening point. Having to form the substrate while in the heated state unnecessarily complicates the process and exposes external conductor and resistor networks to potential damage during handling.
U.S. Pat. No. 6,527,890 to Briscoe et al teaches a method for producing a textured channel in a plurality of green-sheet layers, which are then sintered together to form a substantially monolithic structure. Such a channel, filled with a porous phase for differentially adsorbing chemical components, can be used as the column for separation of gas species by gas chromatography. While this method can produce a channel in a planar substrate, ionizing of species and control of ion flow through appropriate application of an electric field gradient is not required for separation of gas species in Briscoe's disclosed method, and thus there is no provision for producing such.
Each of the above references describes an approach having unique qualities, but no reference on it's own satisfies all of the required characteristics. There remains a need in the art for a more advanced and efficient method of producing a tubular structure with the necessary electrode elements, as can be utilized as a drift tube in an IMS. It is therefore an object of this invention to provide a drift tube that is relatively small in size, airtight, constructed of non-contaminating materials, and of low cost to produce.
It is an object of this invention to provide a tubular substrate with electrodes on an internal surface that are electrically connected to the outer surface without the use of vias through the substrate.
To achieve the foregoing and other objects, and in accordance with the purpose of the present invention, as embodied and broadly described herein, the present invention comprises a tube formed from a rolled flexible substrate and having an interior, a lapped portion, and an exterior, the flexible substrate comprising a first surface and an opposed second surface extending from an interior end connecting the surfaces to an opposed exterior end. A second elongated electrode is affixed to the second surface and extends from the tube interior to the lapped portion; and a first elongated electrode is in direct electrical contact with the second elongated electrode at the lapped portion and extends along the first surface to the exterior of the tube. The substrate is preferably LTCC and the device is made by rolling a green substrate around a form for more than one revolution, restraining the rolled green substrate sheet on the form, applying a lamination pressure to set the green substrate to the form; and firing the rolled substrate sheet. The electrodes spiral through the wall of the tube from the tube interior to the tube exterior.
These and other objects of the present invention will become more fully apparent with reference to the following description and drawings, which relate to several preferred embodiments of the present invention.
The accompanying drawings, which are incorporated in and form part of the specification, illustrate several embodiments of the present invention and, together with the description, serve to explain the principles of the invention.
a shows a cross section of a first embodiment of a tube using the sheet of
b shows a cross section of a second embodiment of a tube using the sheet of
a and 3b show, respectively, opposite sides of a green sheet for use in making a drift tube.
a shows the tube of
b shows a cross section of the tube of
a and 7b show alternate layers of green sheets forming a second embodiment of the invention.
In accordance with a first embodiment of this invention,
It is useful to define some terms relative to tube (7). The ‘interior’ of tube (7) is the portion of surface (B) extending from interior end (i) for one revolution. The ‘lapped’ portion of tube (7) begins at end (i) and includes all portions of substrate (1) where surface (B) overlaps surface (A). The ‘exterior’ of tube (7) is that portion of surface (A) that is not covered by surface (B).
An object of this invention is to have an electrode on the interior of tube (7) that extends to the exterior of tube (7). This object may be accomplished by having an electrode spiral along the surface of substrate (1), as shown in
An internal electrode in the form of a ring is formed if a straight electrode (CB) extends around the interior of tube (7) perpendicular to axis (5) and if the length of electrode (CB) is greater than the circumference of mandrel (9) (which defines the internal circumference of tube (7).
As shown in
An alternate embodiment for connecting electrode (CB) to the outside of tube (7) is illustrated in
Although a tube (7) would most easily be formed by rolling a rectangular substrate around an axis (5) that lies perpendicular to one side of the rectangle, the invention may still be utilized if the axis (5) lies an acute angle to one side of the substrate. In that instance, the tube would extend along axis (5) with each revolution, but the electrodes may still be placed in accordance with the teaching herein. If the substrate is not of uniform width, the resulting tube will not be of uniform thickness, which may be desirable in some applications. Furthermore, there is no requirement that electrode CA follow the shortest possible path to the exterior of the tube. It could even be directed to the side of the substrate (the end of the tube), and be accessible if the substrate were cut so that no additional turns were placed above the electrode at the tube end. Such modifications will be apparent to those of ordinary skill in the art.
There are many known techniques for forming the flexible substrate into a coil or spiral as discussed above. For example, end (i) could be held against the mandrel while the mandrel is rotated at a fixed location. Also, the mandrel could be rolled along a flat surface holding the substrate. Or the substrate could be wrapped around the mandrel. The tube is most frequently described herein as being ‘rolled’, and it is intended that in this context, ‘roll’ means these and other known techniques for forming a substrate into a tube.
As shown in
In the preferred embodiment of the invention, a flexible substrate comprising one sheet of green LTCC tape, DuPont Type 951-AX Green Tape™, was used to produce a rolled tube. A flexible substrate thickness of about 0.010′ was used in this embodiment but thicker and thinner flexible substrates, or a multi-layer flexible substrate could be used as well. Illustrated in
It is preferred to take advantage of the fine line width and spacing capability of commercially available screen printer and micro-pen methods for forming the conductors. The width and spacing of the conductors is not critical to the invention, however a greater number of parallel spaced concentric conductor rings on the interior of a drift tube is preferred, as this will provide a more uniform electric field along the drift tube's length. In the present embodiment, 0.020′ wide gold conductors were printed with 0.010′ spacings on 0.030′ centers by well know screen printing processes using conductor materials compatible with DuPont 951 Green Tape™. In another embodiment of the invention, conductors as narrow as 0.004′ wide and spacings as fine as 0.004′ were produced on a flexible substrate by a well known micro-pen method.
As shown in
After conductor and resistor patterns are applied to the flexible substrate, the substrate is rolled around a mandrel as shown in
The rolled flexible substrate (1) is restrained on the mandrel by tightly wrapping the tube with a suitable polymer film (11) shown in
Co-firing, sintering or firing of the green ceramic are synonymous terms, where co-firing is commonly used to indicate the simultaneous firing of a green LTCC substrate with conductors, resistors, vias or other structures formed from compatible materials. For a typical firing profile, the green LTCC is first brought from room temperature, approximately 22° C., to 450° C. at a 3° C./minute thermal ramp rate. It is held at 450° C. for 2 hours and is then brought to 850° C. at a 2° C./minute ramp rate, and held at 850° C. for about 30 minutes and allowed to cool back to room temperature. At 450° C. organic material within the tape burns off. Had the tape been brought directly to 850° C., these organics would have formed carbonates, which degrade most of the LTCC's properties. Thus it is important that the firing profile allow sufficient time at 450° C. to completely burn off the organic materials within the tape. At 850° C., lower melting glass constituents within the LTCC soften and fuse the higher melting ceramic constituents into a dense body.
b shows a cross-section of a laminated and fired LTCC tube (17) where conductors (CB1 through CBn) form parallel spaced concentric rings on the interior of the tube. Each ring is electrically contacted to an exterior conductor (CA1 through CAn) by that portion of conductor CA which spirals through the body of the tube in the overlapping region (12). Since the individual layers of the green substrate are merged into one structure by the process, the conductors on the interior surface of a formed tube are clearly physically and electrically contacted to the conductors on the exterior surface of the tube by a process that does not require vias in the ceramic sheet. It is preferred to avoid the use of vias in the wall of the tube, as vias can lead to the formation of leakage paths that could impair the desired airtight quality of a drift tube. The length of the overlapped region (12) is not critical to the invention and can be adjusted as needed. For obtaining a reasonable mechanical strength in the fired tube while minimizing material requirements, it has been found that about two and one half complete wraps of the 0.010′ flexible LTCC substrate is preferable. More wraps of flexible LTCC can be used to build up the wall thickness of the tube for higher strength as might be needed to accommodate high pressure or vacuum applications. In the other extreme, the area of overlap may be reduced to zero resulting in a butt style joint in the sheet along the length of the ceramic tube.
It has been found that high quality, high aspect ratio tubes can be produced by this method without slumping of the green LTCC tube during the firing step. By this method, fired tubes having and inner diameter of from 0.238′ to 0.500 and from 1.5′ to 5.0′ in length have been produced with wall thicknesses from 0.020′ to 0.040′. These dimensions are not seen as limitations of the process, only exemplary of what has been done. After the firing step, the now sintered ceramic tube is trimmed to the desired length.
As shown in
Electrodes and gating grids for the drift tube can be provided by methods such as conventional wire mesh, mechanical stamping or photo-lithography of metal sheets, or LIGA (a German acronym that stands for Lithographic Galvonoformung Abformung, or the English translation, lithography, electroplating and molding). An excellent reference on LIGA processing is provided in: Chapter 18, “X-Ray-Based Fabrication” of ‘The MEMS Handbook’, CRC Press 2002.
An embodiment a drift tube produced by this method is shown in
The now essentially complete drift tube may be joined to an end cap structure to provide for carrier gas flow into the drift tube, a sample gas inlet structure and an ionizing source which additionally provides an exhaust port for gases to exit the instrument. These structures are simple mechanical structures well known in the art and may be produced by machining of traditional ceramics, firing of LTCC or other materials. The drift tube is mechanically attached to these components by traditional adhesive or metallurgical methods.
In another embodiment of the invention, a plurality of flexible green LTCC tape layers are provided with a through hole and are stacked to form a planar substrate with the through holes defining a tube extending through the stack. Alternate tape layers in the stack are provided with a conductor surrounding the through hole to form parallel spaced conductor rings on the interior surface of the tube. By this method multi-layer stacks of green LTCC sheets are fired to produce sub-sections of an eventual drift tube.
In this embodiment as shown in
In the present embodiment, 25 green LTCC sheets (40) according to
After firing the individual sub-sections are separated from the substrate by sawing along the dashed lines shown in
As shown in
The bonded sections (85) form an essentially complete drift tube, that may be joined to an end cap structure to provide for carrier gas flow into the drift tube, a sample gas inlet structure and an exhaust port, and ionizing source, constructed by methods well known in the art. The bonded drift tube can be mechanically attached to these components by traditional adhesive, metallurgical methods or by another application of fusible glass tape. The conductor pattern on the exterior of the drift tube provides electrical connection points (76) for interfacing to the IMS control electronics.
In another embodiment of the invention a tubular substrate is formed by lamination of two flexible green ceramic sheets, preferably comprising unfired LTCC, with a removable mandrel interposed between the two flexible sheets. As shown in
As shown in
The first and second flexible green ceramic sheets are restrained on the mandrel by means of vacuum bagging in a polymer film as is practiced in the art. Isostatic lamination conditions of about 3000 psi at about 68° C. and for about 15 minutes are applied to the restrained green ceramic sheets while on the mandrel, to conform the interior surfaces of the first and second green ceramic sheets to the mandrel and set the overlapping regions of the two sheets.
As shown in
Flexible printed wiring boards are available commercially and are widely manufactured by bonding, with or without an adhesive layer, ductile copper foil to a variety of dielectric sheet materials such as polyimide (Kapton™), polyester terephthalate (Mylar), and polytetrafluoroethylene (Teflon™ or PTFE). Preferred are dielectric's derived from polyimide and polytetrafluoroethylene as they are well known for their chemical inertness and stability at elevated temperatures. Dielectric thicknesses typically range from about 0.0005′ to 0.005′ with bonded copper conductor foil thickness ranging from about 0.0002′ to 0.020′. Adhesives are typically comprised of a wide range of materials including acrylics, epoxies, polyesters and phenolic butyrals and are known stable at temperatures of about 150° C. and can tolerate short term exposures to an elevated temperature of about 250° C. Conductors are formed from the bonded copper foil by photolithographic and etching techniques, or printed in conductive inks. Compatible polymeric resistor materials are commercially available to provide integrated resistor networks and multi-layer substrates can be formed by alternately bonding additional dielectric layers and conductor layers into a stacked arrangement. Electrical vias can also be provided to interconnect conductor patterns on differing layers in a multi-layer stack up.
In another embodiment of the invention as shown in
Additional objects, advantages, and novel features of the invention will become apparent to those skilled in the art upon examination of the following description or may be learned by practice of the invention. The objects and advantages of the invention may be realized and attained as particularly pointed out in the appended claims. It is intended that the scope of the invention be defined by the appended claims.
This application claims the benefit of U.S. Provisional Application No. 60/408,801, filed on Sep. 5, 2002.
The United States Government has rights in this invention pursuant to Department of Energy Contract No. DE-AC04-94AL85000 with Sandia Corporation.
Number | Name | Date | Kind |
---|---|---|---|
3755891 | Muckelroy et al. | Sep 1973 | A |
4390784 | Browning et al. | Jun 1983 | A |
4475967 | Kanai et al. | Oct 1984 | A |
5028473 | Vitriol et al. | Jul 1991 | A |
5280175 | Karl | Jan 1994 | A |
5814262 | Ketcham et al. | Sep 1998 | A |
5965882 | Megerle et al. | Oct 1999 | A |
6051832 | Bradshaw | Apr 2000 | A |
6369383 | Cornish et al. | Apr 2002 | B1 |
6527890 | Briscoe et al. | Mar 2003 | B1 |
6586885 | Coll et al. | Jul 2003 | B1 |
6607414 | Cornish et al. | Aug 2003 | B1 |
Number | Date | Country | |
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60408801 | Sep 2002 | US |