CA2135703A1 - Ultra light weight thin membrane antenna reflector - Google Patents
Ultra light weight thin membrane antenna reflectorInfo
- Publication number
- CA2135703A1 CA2135703A1 CA 2135703 CA2135703A CA2135703A1 CA 2135703 A1 CA2135703 A1 CA 2135703A1 CA 2135703 CA2135703 CA 2135703 CA 2135703 A CA2135703 A CA 2135703A CA 2135703 A1 CA2135703 A1 CA 2135703A1
- Authority
- CA
- Canada
- Prior art keywords
- reflector
- fabric
- strands
- molded
- support
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Abandoned
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q15/00—Devices for reflection, refraction, diffraction or polarisation of waves radiated from an antenna, e.g. quasi-optical devices
- H01Q15/14—Reflecting surfaces; Equivalent structures
- H01Q15/141—Apparatus or processes specially adapted for manufacturing reflecting surfaces
- H01Q15/142—Apparatus or processes specially adapted for manufacturing reflecting surfaces using insulating material for supporting the reflecting surface
- H01Q15/144—Apparatus or processes specially adapted for manufacturing reflecting surfaces using insulating material for supporting the reflecting surface with a honeycomb, cellular or foamed sandwich structure
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q15/00—Devices for reflection, refraction, diffraction or polarisation of waves radiated from an antenna, e.g. quasi-optical devices
- H01Q15/14—Reflecting surfaces; Equivalent structures
- H01Q15/16—Reflecting surfaces; Equivalent structures curved in two dimensions, e.g. paraboloidal
- H01Q15/168—Mesh reflectors mounted on a non-collapsible frame
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Details Of Aerials (AREA)
- Aerials With Secondary Devices (AREA)
- Woven Fabrics (AREA)
Abstract
An ultra light weight reflector for a satellite application using an open weave fabric including a plurality of strands. The plurality of strands are oriented along distinct axis are intertwined with respect to each other.
The multi-axial fabric is at least tri-axial. A support, which is connected to the satellite, maintains the position of the fabric. The fabric is single ply, and as such the construction is resilient, lightweight, and relatively simple to produce. The fabric is typically formed as a membrane into either a standard shape (i.e.
flat, parabolic, hyperbolic, etc.), or more complex shaped surface using techniques known in the art.
The multi-axial fabric is at least tri-axial. A support, which is connected to the satellite, maintains the position of the fabric. The fabric is single ply, and as such the construction is resilient, lightweight, and relatively simple to produce. The fabric is typically formed as a membrane into either a standard shape (i.e.
flat, parabolic, hyperbolic, etc.), or more complex shaped surface using techniques known in the art.
Description
ULTRA LIGHT WEIGHT THIN MEMBRANE ANTENNA REFLECTOR
Field Of The TnVention s The present invention relates generally to light weight reflectors to be used with antennas, and more specifically to very light weight reflectors a6sociated with satellite antenna~ formed from a tri-axial fabric, which i6 capable of undergoing some deformations due to accelerations and minor contacts, and returning to the original configuration after the deformation.
Background of the Invention Reflector technology has always been an important consideration in antenna design. Since the cost of a launch is tied closely to the mass of the satellite, the weight of the antenna is at a premium. It is also important that the reflector be able to survive the extreme environment of launch and orbit conditions. These include high G-forces, acoustic noise and extreme temperature. So called "shaped" surfaces for reflectors are also highly desirable, in which reflector surfaces are intentionally di~torted during manufactur~ ~o that region~ o~ th~
radiation emanating from the reflector surface can be precisely controlled.
There have been a considerable number of reflector designs which have involved interwoven fahric of one type or other.
One example is illustrated in U.S. Patent No. 4,092,453, issued to Jonda on May 30, 1978. The interweaving of a plurality of the strands of the fabric is oriented perpendicularly to other strands (the weave i~ bi-axial).
While this interweaving process does provide for significant strength improvements over the prior art 2I~703 methods, the material of this patent suffers from having different strength characteristics when force is being applied to the fabric at different orientations. For example, when the force is being exerted parallel to the orientation of some of the strands of the fabric, the reflector will exhibit a greater resistance against deformation and deflection then when the force is being applied in the plane of the fabric, yet at some angle to the strands of the fabric.
Both U.S. Patent No. 4,868,580, issued September 19, 1989 to Wade and U.S. Patent No. 4,812,854, issued March 14, 1989 to Boan et al. illustrate different interweaving patterns for the fabric reflector from the perpendicular weave described in Jonda; both of these prior art weaves will under certain situations exert a greater resistance to applied stress, for a given weight than Jonda. These weaving configurations still exhibit different characteristics when a constant force is applied at different orientations to the fabric, within the general plane of the fabric.
Another reflector which utilizes interwoven fabric is illustrated in U.S. Patent No. 4,635,071, issued on January 6, 1987 to Gounder et al. The strands of fabric in each ply of fabric is oriented parallel to all of the other strands in that ply of fabric. There are multiple plies of fabric, each of the ply is oriented approximately~ sixty degrees to the other plies of fabric. The strands of fabric which are oriented in different directions are not intertwined. Also, utilizing fabric with more than one ply leads to extra material expense and manufacturing challenges.
From the above, it could be envisioned that the production of a multi-axial (at least tri-axial) intertwined fabric, which produces substantially constant resistance against 213~7~3 deflection when the forces are applied within the plane of the material, applicable to the production of a lightweight, resilient reflectors which are associated with antennas to be used in spacecraft and in other applications would be highly desirable.
SUMMARY OF THE INVENTION
The present invention relates to a fabric to be used in a reflector including a plurality of strands of fabric, in which a plurality of strands which are oriented along distinct axis are intertwined with respect to each other.
The multi-axial fabric is at least tri-axial.
BRIEF DESCRIPTION OF THE DRAWING FIGURES
Fig. 1 illustrates a perspective view of one embodiment of spacecraft (14) conta,ining an antenna (12) and an associated reflector (10) of the present invention;
Fig. 2 illustrates a side view of one embodiment of a reflector (10) of the present invention to be utilized in conjunction with the spacecraft (14) illustrated in Fig. l;
Fig. 3 illustrates a perspective view of the support (18) of the reflector of Fig. 2;-Fig. 4 illustrates a side view of the support (18) of Fig.30 3;
Fig. 5 illustrates an exploded view of one embodiment of ' the multi-axial fabric used in the reflector of Fig. 2; and Fig. 6 illustrates a similar view to Fig. 5 of a prior art bi-axial fabric weave.
DETAILED DESCRIPTION OF THE PRESENT INVENTION
While the present disclosure describes a reflector used on conjunction with a spacecraft, this application (and the specifla configuration of the reflector) and materials is intended to be illustrative and not limiting in scope. The present invention is meant to apply to any reflector which is to be utilized with any space or terrestrial application, whether it is associated with antennas or any other structure where reflectors are utilized. The present disclosure, however, is especially suited to spacecraft applications since it provides a very lightweight, durable, and resilient structure.
The present invention is concerned with an ultra-light weight thin membrane reflector 10, suitable for use with an antenna 12 on a spacecraft 14 (in the illustration, a satellite) as illustrated in Fig. 1. The spacecraft also has vanes 15 which do not form a part of the present invention. The thin membrane reflector 10, as illustrated in Fig. 2, comprises a support 18 including an outer ring 20 and an rear support portion 22. Also included in the thin membrane reflector 10 is a thin membrane 24 which is formed from a fabric 26 containing a multitude of strands, as described below. A typical size of the thin membrane reflector 10, when properly supported, is typically within the range of 1 to 3 meters, but may be any size which is desired, and applicable, and may be deployed.
Exploded perspective and side views of the support 18 are illustrated in Figs. 3 and 4, respectively. The support is formed from the outer ring 20 and the rear support portion 22. Both the outer ring and the internal support portion are configured to support the thin membrane 24 (illustrated in Fig. 1) in a planar, parabolic, hyperbolic, or any other geometric shape as is desired for the specific application.
The support is attached to the spacecraft utilizing any 213~703 well known and suitable type of fastener affixed to a connection portion 29. The outer ring 20 preferably has a core formed from a graphite honeycomb structure to provide a strong and lightweight structure and als~ provide a very low thermal expansion: even though any light weight material (usually synthetic) which has a very low coefficient of expansion may be used. Such synthetic materials may be formed using any well known manufacturing technique, but foam molds have been found to be appropriate.
The reason why the coefficient of thermal expansion is so critical in satellite applicat~ons is the intense temperature variation between the side of the reflector which is facing the sun compared to the side of the reflector which is in the shade. The spacecraft temperature variation ranges from 130 degrees centigrade in the sun to minus 180 degrees centigrade in the shade. With this temperature variation. It is essential that the coefficient of thermal expansion be approximately 1 part expansion per million parts for each variation of one degree centigrade, if the satellite reflector can be reliably used in communication applications. Larger or smaller coefficients of expansion may be required for satellite reflectors with different applications.
The thin membrane 24 is attached only to, and supported only by, the outer ring 20. The rear support portion 22 includes a plurality of support members 32 and an internal ring 33. The outer ring 20 is supported by the plurality of support members 32 (preferably at least six) which are also affixed to, and supported by, the internal ring 33.
The rear support portion consists of uni-directional and spread fabric formed preferably from a graphite composition which has a high modulus and low coefficient of thermal expansion. Such materials, and manufacturing techniques, as described previously relative to the outer ring 20 may also be applied to the internal ring 33 and the support members 32. The rear support portion 22 is formed from a minimal number of tubular integrated parts, being designed for a minimal weight. Multi-layer insulation may also be applied to protect all or part of the reflector and support structure from the thermal environments experienced in orbit. The front surface of the thin membrane 24 is left uncovered to avoid the thermal effects of paint, or other covering.
As illustrated in Fig. 5, the thin membrane 24 i5 a single ply membrane (in the approximate range from 0.010" to 0.040" thick) of high modulus (preferably graphite) fiber 40 applied as a tri-axial open weave fabric which is pre-impregnated with a toughened resin. Such membranedimensioning is usually applied to be reflective to radiation of the microwave spectrum. Even though the above membrane material dimension range is inapplicable in the visible light or other short wavelength electro-magnetic spectrum (the radiation would pass through the membrane and/or deflect at random angles off the individual fibers), the radiation from microwave radiation will interface with the 0.010" to 0.040" thick membrane as if it were a continual material. It is envisioned that the woven thin membrane of the present invention would therefore be most applied to microwave applications.
Even though this disclosure is directed towards a tri-axial weave, it is envisioned that any multi-axial weave may be used, as long as the multi-axial is at least tri-axial. In a tri-axial weave as illustrated in Fig. 5, for example, sets of fibers are oriented along three coplanar axes 42a, 42b, 42c with each axis forming an intersecting angle of approximately sixty degrees to each other axis.
The fibers oriented along each axis are interwoven with fibers which are not oriented in the same axis.
21~5703 The advantages of a multi-axial weave as illustrated in Fig. 5 is illustrated in comparison to a prior art bi-axial weave as illustrated in Fig. 6. The bi-axial weave will exhibit considerably higher deflection resistance when a distorting force Fl is applied in a direction substantially parallel to one of the axis 46, 48 as compared to when a distorting force F2 is applied at an angle 50a, SOb to both of the axis. The tri-axial weave of the present invention as illustrated in Fig. 6 will display a much more uniform deflection resistance when regardless of whether a distorting force F3 is applied substantially parallel to one of the axis 42a, 42b, 42c; or a distorting force F4 is applied at a non-zero angle 54a, 54b, 54c to each of the three axis 42a, 42b, 42c since the distorting force F4 usually is closer to parallel to one or more of the axes than F2 would be. This uniformity of deflection resistance (the material is quasi-isotropic in the plane of the fabric) not only ensures that the thin membrane will undergo a more constant deflection when a random force is applied to the fabric, but also ensures that the fabric will be able to resist the type of force which would likely cause permanent distortion to the thin membrane 24. The tri-axial weave also ensures that a desired resistance against a force applied from any direction can be met without providing a substantial increase in weight to the thin membrane 24.
The above configuration of thin membrane reflector 10 is ultra-light, and is suitable for use as an antenna reflector for the communications satellite 14. The fabric of the thin membrane 24 is very li~ht, thermally stable, durable, responsive and provides a reflective surface at radio frequencies (RF) and microwave frequencies. The fabric can be easily molded as a planar surface, a parabola, a hyperbola, or any other desired surface. The thin membrane 24 is deformable under the types of forces (either G-forces or contact forces) which the thin membrane 213~7~3 reflector 10 is likely to encounter when the spacecraft is being launched or deployed.
It is also possible that the thin membrane 24 may be formed in some peculiar configuration to form a ~o called "shaped" surface. Such shaped surfaces are configured such that radiation may be reflected off the surface of the membrane in a desired manner. For example, of the thin membrane reflector 10 is being used to apply radiation across a land-mass, it would be desired to confine the direction which the radiation is being directed to within the outlines of the landmass (which would usually be an irregular shape). It may be desirable to alter the configuration of the thin membrane 24 such that a higher percentage of the transmitted or received radiation is being directed to or from the desired location. "Shaping"
the membrane can assist in the above applications, among others. One advantage of the present invention compared to other more rigid reflectors relative to shaping is that the shape of the thin membrane 24 present system is easier to manufacture. Certain prior art reflectors, since they are thicker and relatively rigid, are typically more difficult to shape precisely.
Being able to produce a thin membrane 24 of only one ply improves the thermal stability both by lowering the thermal mass of the thin membrane reflector 24 and by lowering the coefficient of thermal expansion (CTE) to almost zero, and also simplifies the manufacturing process considerably. The open weave of the fabric permits acoustic vibrational forces (pressure exerted by sound waves) to be relieved through the membrane surface. The acoustic vibration environment experienced during the launch of the satellite 14 is a critical design constraint for large light weight surfaces such as the thin membrane reflectors 10.
Field Of The TnVention s The present invention relates generally to light weight reflectors to be used with antennas, and more specifically to very light weight reflectors a6sociated with satellite antenna~ formed from a tri-axial fabric, which i6 capable of undergoing some deformations due to accelerations and minor contacts, and returning to the original configuration after the deformation.
Background of the Invention Reflector technology has always been an important consideration in antenna design. Since the cost of a launch is tied closely to the mass of the satellite, the weight of the antenna is at a premium. It is also important that the reflector be able to survive the extreme environment of launch and orbit conditions. These include high G-forces, acoustic noise and extreme temperature. So called "shaped" surfaces for reflectors are also highly desirable, in which reflector surfaces are intentionally di~torted during manufactur~ ~o that region~ o~ th~
radiation emanating from the reflector surface can be precisely controlled.
There have been a considerable number of reflector designs which have involved interwoven fahric of one type or other.
One example is illustrated in U.S. Patent No. 4,092,453, issued to Jonda on May 30, 1978. The interweaving of a plurality of the strands of the fabric is oriented perpendicularly to other strands (the weave i~ bi-axial).
While this interweaving process does provide for significant strength improvements over the prior art 2I~703 methods, the material of this patent suffers from having different strength characteristics when force is being applied to the fabric at different orientations. For example, when the force is being exerted parallel to the orientation of some of the strands of the fabric, the reflector will exhibit a greater resistance against deformation and deflection then when the force is being applied in the plane of the fabric, yet at some angle to the strands of the fabric.
Both U.S. Patent No. 4,868,580, issued September 19, 1989 to Wade and U.S. Patent No. 4,812,854, issued March 14, 1989 to Boan et al. illustrate different interweaving patterns for the fabric reflector from the perpendicular weave described in Jonda; both of these prior art weaves will under certain situations exert a greater resistance to applied stress, for a given weight than Jonda. These weaving configurations still exhibit different characteristics when a constant force is applied at different orientations to the fabric, within the general plane of the fabric.
Another reflector which utilizes interwoven fabric is illustrated in U.S. Patent No. 4,635,071, issued on January 6, 1987 to Gounder et al. The strands of fabric in each ply of fabric is oriented parallel to all of the other strands in that ply of fabric. There are multiple plies of fabric, each of the ply is oriented approximately~ sixty degrees to the other plies of fabric. The strands of fabric which are oriented in different directions are not intertwined. Also, utilizing fabric with more than one ply leads to extra material expense and manufacturing challenges.
From the above, it could be envisioned that the production of a multi-axial (at least tri-axial) intertwined fabric, which produces substantially constant resistance against 213~7~3 deflection when the forces are applied within the plane of the material, applicable to the production of a lightweight, resilient reflectors which are associated with antennas to be used in spacecraft and in other applications would be highly desirable.
SUMMARY OF THE INVENTION
The present invention relates to a fabric to be used in a reflector including a plurality of strands of fabric, in which a plurality of strands which are oriented along distinct axis are intertwined with respect to each other.
The multi-axial fabric is at least tri-axial.
BRIEF DESCRIPTION OF THE DRAWING FIGURES
Fig. 1 illustrates a perspective view of one embodiment of spacecraft (14) conta,ining an antenna (12) and an associated reflector (10) of the present invention;
Fig. 2 illustrates a side view of one embodiment of a reflector (10) of the present invention to be utilized in conjunction with the spacecraft (14) illustrated in Fig. l;
Fig. 3 illustrates a perspective view of the support (18) of the reflector of Fig. 2;-Fig. 4 illustrates a side view of the support (18) of Fig.30 3;
Fig. 5 illustrates an exploded view of one embodiment of ' the multi-axial fabric used in the reflector of Fig. 2; and Fig. 6 illustrates a similar view to Fig. 5 of a prior art bi-axial fabric weave.
DETAILED DESCRIPTION OF THE PRESENT INVENTION
While the present disclosure describes a reflector used on conjunction with a spacecraft, this application (and the specifla configuration of the reflector) and materials is intended to be illustrative and not limiting in scope. The present invention is meant to apply to any reflector which is to be utilized with any space or terrestrial application, whether it is associated with antennas or any other structure where reflectors are utilized. The present disclosure, however, is especially suited to spacecraft applications since it provides a very lightweight, durable, and resilient structure.
The present invention is concerned with an ultra-light weight thin membrane reflector 10, suitable for use with an antenna 12 on a spacecraft 14 (in the illustration, a satellite) as illustrated in Fig. 1. The spacecraft also has vanes 15 which do not form a part of the present invention. The thin membrane reflector 10, as illustrated in Fig. 2, comprises a support 18 including an outer ring 20 and an rear support portion 22. Also included in the thin membrane reflector 10 is a thin membrane 24 which is formed from a fabric 26 containing a multitude of strands, as described below. A typical size of the thin membrane reflector 10, when properly supported, is typically within the range of 1 to 3 meters, but may be any size which is desired, and applicable, and may be deployed.
Exploded perspective and side views of the support 18 are illustrated in Figs. 3 and 4, respectively. The support is formed from the outer ring 20 and the rear support portion 22. Both the outer ring and the internal support portion are configured to support the thin membrane 24 (illustrated in Fig. 1) in a planar, parabolic, hyperbolic, or any other geometric shape as is desired for the specific application.
The support is attached to the spacecraft utilizing any 213~703 well known and suitable type of fastener affixed to a connection portion 29. The outer ring 20 preferably has a core formed from a graphite honeycomb structure to provide a strong and lightweight structure and als~ provide a very low thermal expansion: even though any light weight material (usually synthetic) which has a very low coefficient of expansion may be used. Such synthetic materials may be formed using any well known manufacturing technique, but foam molds have been found to be appropriate.
The reason why the coefficient of thermal expansion is so critical in satellite applicat~ons is the intense temperature variation between the side of the reflector which is facing the sun compared to the side of the reflector which is in the shade. The spacecraft temperature variation ranges from 130 degrees centigrade in the sun to minus 180 degrees centigrade in the shade. With this temperature variation. It is essential that the coefficient of thermal expansion be approximately 1 part expansion per million parts for each variation of one degree centigrade, if the satellite reflector can be reliably used in communication applications. Larger or smaller coefficients of expansion may be required for satellite reflectors with different applications.
The thin membrane 24 is attached only to, and supported only by, the outer ring 20. The rear support portion 22 includes a plurality of support members 32 and an internal ring 33. The outer ring 20 is supported by the plurality of support members 32 (preferably at least six) which are also affixed to, and supported by, the internal ring 33.
The rear support portion consists of uni-directional and spread fabric formed preferably from a graphite composition which has a high modulus and low coefficient of thermal expansion. Such materials, and manufacturing techniques, as described previously relative to the outer ring 20 may also be applied to the internal ring 33 and the support members 32. The rear support portion 22 is formed from a minimal number of tubular integrated parts, being designed for a minimal weight. Multi-layer insulation may also be applied to protect all or part of the reflector and support structure from the thermal environments experienced in orbit. The front surface of the thin membrane 24 is left uncovered to avoid the thermal effects of paint, or other covering.
As illustrated in Fig. 5, the thin membrane 24 i5 a single ply membrane (in the approximate range from 0.010" to 0.040" thick) of high modulus (preferably graphite) fiber 40 applied as a tri-axial open weave fabric which is pre-impregnated with a toughened resin. Such membranedimensioning is usually applied to be reflective to radiation of the microwave spectrum. Even though the above membrane material dimension range is inapplicable in the visible light or other short wavelength electro-magnetic spectrum (the radiation would pass through the membrane and/or deflect at random angles off the individual fibers), the radiation from microwave radiation will interface with the 0.010" to 0.040" thick membrane as if it were a continual material. It is envisioned that the woven thin membrane of the present invention would therefore be most applied to microwave applications.
Even though this disclosure is directed towards a tri-axial weave, it is envisioned that any multi-axial weave may be used, as long as the multi-axial is at least tri-axial. In a tri-axial weave as illustrated in Fig. 5, for example, sets of fibers are oriented along three coplanar axes 42a, 42b, 42c with each axis forming an intersecting angle of approximately sixty degrees to each other axis.
The fibers oriented along each axis are interwoven with fibers which are not oriented in the same axis.
21~5703 The advantages of a multi-axial weave as illustrated in Fig. 5 is illustrated in comparison to a prior art bi-axial weave as illustrated in Fig. 6. The bi-axial weave will exhibit considerably higher deflection resistance when a distorting force Fl is applied in a direction substantially parallel to one of the axis 46, 48 as compared to when a distorting force F2 is applied at an angle 50a, SOb to both of the axis. The tri-axial weave of the present invention as illustrated in Fig. 6 will display a much more uniform deflection resistance when regardless of whether a distorting force F3 is applied substantially parallel to one of the axis 42a, 42b, 42c; or a distorting force F4 is applied at a non-zero angle 54a, 54b, 54c to each of the three axis 42a, 42b, 42c since the distorting force F4 usually is closer to parallel to one or more of the axes than F2 would be. This uniformity of deflection resistance (the material is quasi-isotropic in the plane of the fabric) not only ensures that the thin membrane will undergo a more constant deflection when a random force is applied to the fabric, but also ensures that the fabric will be able to resist the type of force which would likely cause permanent distortion to the thin membrane 24. The tri-axial weave also ensures that a desired resistance against a force applied from any direction can be met without providing a substantial increase in weight to the thin membrane 24.
The above configuration of thin membrane reflector 10 is ultra-light, and is suitable for use as an antenna reflector for the communications satellite 14. The fabric of the thin membrane 24 is very li~ht, thermally stable, durable, responsive and provides a reflective surface at radio frequencies (RF) and microwave frequencies. The fabric can be easily molded as a planar surface, a parabola, a hyperbola, or any other desired surface. The thin membrane 24 is deformable under the types of forces (either G-forces or contact forces) which the thin membrane 213~7~3 reflector 10 is likely to encounter when the spacecraft is being launched or deployed.
It is also possible that the thin membrane 24 may be formed in some peculiar configuration to form a ~o called "shaped" surface. Such shaped surfaces are configured such that radiation may be reflected off the surface of the membrane in a desired manner. For example, of the thin membrane reflector 10 is being used to apply radiation across a land-mass, it would be desired to confine the direction which the radiation is being directed to within the outlines of the landmass (which would usually be an irregular shape). It may be desirable to alter the configuration of the thin membrane 24 such that a higher percentage of the transmitted or received radiation is being directed to or from the desired location. "Shaping"
the membrane can assist in the above applications, among others. One advantage of the present invention compared to other more rigid reflectors relative to shaping is that the shape of the thin membrane 24 present system is easier to manufacture. Certain prior art reflectors, since they are thicker and relatively rigid, are typically more difficult to shape precisely.
Being able to produce a thin membrane 24 of only one ply improves the thermal stability both by lowering the thermal mass of the thin membrane reflector 24 and by lowering the coefficient of thermal expansion (CTE) to almost zero, and also simplifies the manufacturing process considerably. The open weave of the fabric permits acoustic vibrational forces (pressure exerted by sound waves) to be relieved through the membrane surface. The acoustic vibration environment experienced during the launch of the satellite 14 is a critical design constraint for large light weight surfaces such as the thin membrane reflectors 10.
Claims (20)
1. A lightweight radiation reflector capable of being used with an antenna, comprising:
a multi-axis, singly-ply, lightweight, shaped fabric composed of a plurality of strands comprising at least three strands which are oriented along at least three distinct coplanar axes and are intertwined with respect to each other to form said fabric.
a multi-axis, singly-ply, lightweight, shaped fabric composed of a plurality of strands comprising at least three strands which are oriented along at least three distinct coplanar axes and are intertwined with respect to each other to form said fabric.
2. The reflector as defined in claim 1, further comprising a support capable of supporting said reflector.
3. The reflector as defined in claim 2 in which said support has a honeycomb structure.
4. The reflector as defined in claim 2, wherein the multi-axis fabric is molded into a geometric shape, and the support is affixed to the shaped fabric at a plurality of points.
5. The reflector as defined in claim 2, wherein said support comprises an outer ring member
6. The reflector as defined in claim 5, wherein the outer ring member is formed from graphite.
7. The reflector as defined in claim 5, wherein the outer ring member comprises a honeycomb structure.
8. The reflector as defined in claim 5, wherein the outer ring member comprises a material having a low thermal expansion.
9. The reflector as defined in claim 2 in which at least a portion of said support is molded.
10. The reflector as defined in claim 9, wherein said support is molded by means of a foam mold.
11. The reflector as defined in claim 1, wherein said fabric is molded in a parabolic shape.
12. The reflector as defined in claim 1, wherein said fabric is molded in a planar shape.
13. The reflector as defined in claim 1, wherein the reflector is molded in a hyperbolic shape.
14. The reflector as described in claim 1, wherein said strands comprise a high modulus graphite fiber.
15. The reflector as defined in claim 1 in which said intertwined strands are interwoven.
16. The reflector as described in claim 1, further comprising:
multi-layer insulation which is applied to protect all or part of the reflector from the thermal environments experienced in orbit.
multi-layer insulation which is applied to protect all or part of the reflector from the thermal environments experienced in orbit.
17. A lightweight, multi-axis fabric suitable for use in a radiation reflector comprising:
a single ply fabric composed of a plurality of strands of fiber comprising at least three strands which are oriented along at least three distinct axes and which are intertwined with respect to each other to form said fabric.
a single ply fabric composed of a plurality of strands of fiber comprising at least three strands which are oriented along at least three distinct axes and which are intertwined with respect to each other to form said fabric.
18. The fabric as described in claim 17, wherein the fiber comprises a high modulus graphite fiber.
19. The fabric as described in claim 17, molded into a geometric shape.
20. The fabric as described in claim 17 in which said intertwined strands are interwoven.
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US18919394A | 1994-01-31 | 1994-01-31 | |
| US08/189,193 | 1994-01-31 |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CA2135703A1 true CA2135703A1 (en) | 1995-08-01 |
Family
ID=22696327
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA 2135703 Abandoned CA2135703A1 (en) | 1994-01-31 | 1994-11-14 | Ultra light weight thin membrane antenna reflector |
Country Status (5)
| Country | Link |
|---|---|
| EP (1) | EP0665606B1 (en) |
| JP (1) | JPH07226619A (en) |
| CA (1) | CA2135703A1 (en) |
| DE (1) | DE69524796T2 (en) |
| ES (1) | ES2170125T3 (en) |
Families Citing this family (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5686930A (en) * | 1994-01-31 | 1997-11-11 | Brydon; Louis B. | Ultra lightweight thin membrane antenna reflector |
| JPH08130409A (en) * | 1994-10-28 | 1996-05-21 | Nec Aerospace Syst Ltd | Antenna |
| JP4189697B2 (en) * | 1997-09-18 | 2008-12-03 | サカセ・アドテック株式会社 | Reflective material for high frequency compatible antenna and method for setting design parameters of reflective material for high frequency compatible antenna |
| JP4141122B2 (en) * | 2000-11-06 | 2008-08-27 | サカセ・アドテック株式会社 | Inflatable structure, array antenna provided with inflatable structure, and method for deploying inflatable structure |
| JP5289098B2 (en) * | 2009-02-27 | 2013-09-11 | 三菱電機株式会社 | Grid reflector |
| FR2944155B1 (en) * | 2009-04-02 | 2016-05-13 | Astrium Sas | RADIOELECTRONIC ANTENNA WITH IMPROVED DECOUPLING CORNERS |
| US9685710B1 (en) | 2014-01-22 | 2017-06-20 | Space Systems/Loral, Llc | Reflective and permeable metalized laminate |
| CN113584682B (en) * | 2021-07-21 | 2023-03-24 | 航宸石家庄新材料科技有限公司 | Circular weaving machine for producing planar three-dimensional fabric |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE2447565C3 (en) * | 1974-10-05 | 1978-07-20 | Messerschmitt-Boelkow-Blohm Gmbh, 8000 Muenchen | Fine metal mesh structure with arched lattice bars |
| US4916459A (en) * | 1986-03-19 | 1990-04-10 | Hitachi, Ltd. | Parabolic antenna dish |
| JPH01148840A (en) * | 1987-11-30 | 1989-06-12 | Agency Of Ind Science & Technol | Three-dimensional shaped fabric and its production |
-
1994
- 1994-11-14 CA CA 2135703 patent/CA2135703A1/en not_active Abandoned
- 1994-12-27 JP JP6326029A patent/JPH07226619A/en active Pending
-
1995
- 1995-01-31 DE DE1995624796 patent/DE69524796T2/en not_active Expired - Fee Related
- 1995-01-31 EP EP19950300582 patent/EP0665606B1/en not_active Expired - Lifetime
- 1995-01-31 ES ES95300582T patent/ES2170125T3/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| ES2170125T3 (en) | 2002-08-01 |
| EP0665606B1 (en) | 2002-01-02 |
| EP0665606A1 (en) | 1995-08-02 |
| JPH07226619A (en) | 1995-08-22 |
| DE69524796D1 (en) | 2002-02-07 |
| DE69524796T2 (en) | 2002-08-14 |
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| EEER | Examination request | ||
| FZDE | Dead |