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| United States Patent | 3969731 |
| Link to this page | http://www.wikipatents.com/3969731.html |
| Inventor(s) | Jenkins; Robert K. (Huntington Beach, CA);
Keller; Leon B. (Palos Verdes Peninsula, CA);
Cover, Jr.; John H. (Woodland Hills, CA) |
| Abstract | A mesh article, such as a reflector for radio frequencies, comprises glassy
base fibers of high tensile strength, low elongation properties and low
coefficient of expansion, the fibers being coated with a thin layer of
metal. In a typical embodiment, the fibers are quartz coated with
aluminum. The fibers are not interwoven and are bonded together at their
intersections and to a peripheral ring support. These articles are
lightweight, flexible and foldable and possess a "shape memory." |
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Title Information  |
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Drawing from US Patent 3969731 |
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Mesh articles particularly for use as reflectors of radio waves |
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| Publication Date |
July 13, 1976 |
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| Filing Date |
February 19, 1974 |
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| Parent Case |
BACKGROUND OF THE INVENTION
This is a continuation of application Ser. No. 9,132 filed Feb. 11, 1970,
now abandoned, which in turn is a continuation of application Ser. No.
590,571 filed Oct. 31, 1966, now abandoned. |
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Title Information  |
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Description  |
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This invention relates to electrically conductive mesh articles
characterized by being flexible yet thermally stable. More particularly,
but not necessarily exclusively, the invention relates to radio wave
reflective articles and materials in mesh form which are electrically
conductive and of exceptional light weight, flexibility, and dimensional
and thermal stability. Such articles and materials may be readily formed
and maintained in extremely accurate shapes.
The articles and materials of the present invention are especially useful
for lightweight radar antennas and particularly where such antennas are to
be used in space as on space satellites or celestial bodies (i.e., the
moon). Heretofore it has been customary to utilize solid metal surfaces
for the reflection of radio waves in such applications. Such solid
reflective articles have been produced from sheet metal, metal foil, or
metal-coated substrates. Such space applications require radio wave
reflectors to possess many diverse properties which often are incongruous
and usually not achievable in solid structures. Thus, large size and low
weight are usually required as well as flexibility and dimensional and
structural rigidity, especially to environmental and maneuvering
conditions. At the same time, the ability to be packaged in a small
volume, as during transit to a space station, and the ability to be
deployed thereat into the correct shape, are desirable features.
Heretofore some of these properties have been sought in approaches
utilizing umbrella-like structures consisting of spokes and mesh,
metallized polymeric films reinforced with plastic or foam capable of
being hardened in space, or petaloid structures made of a large number of
electroformed metal (i.e., nickel) segments which are mechanically
unfurled. It will be appreciated that these various constructions have
possessed disadvantages such as high weight per unit area of reflective
surface (i.e., 0.1 to 0.3 lb./sq. ft. of deployed surface), mechanical
complexity, poor dimensional accuracy, and low reliability. Perforated or
expanded metal reflectors, or woven and/or welded wire grids have also
been used with a sacrifice in lightness, flexibility, and foldability. In
contrast, the conductive mesh articles and materials of the invention are
lighter by several orders of magnitude with respect to comparable prior
art constructions and exhibit flexibility and foldability prior to
deployment into shape as well as being more dimensionally precise.
Constructions achieved according to the present invention, for example,
weigh from 0.001 to 0.003 lb./sq. ft. of deployed surface. In the case of
a 120-foot diameter paraboloid design made according to the invention,
deviation from the true paraboloid was estimated to be .+-. 0.125 inch
compared to a predicted deviation of .+-. 1.0 to .+-. 3.0 inch for such
paraboloids fabricated according to the prior art. It is also possible to
make articles according to the invention which possess a smooth, doubly
curved shape without gaps, laps, seams, or discontinuities.
It is therefore an object of the present invention to provide an improved
electrically conductive mesh article of prescribed shape and which is
dimensionally accurate and stable.
Another object of the invention is to provide an improved mesh article of
prescribed shape suitable for use as a reflector of radio waves.
Another object of the invention is to provide an improved electrically
conductive mesh article of prescribed shape, which is dimensionally
accurate and stable, of light weight, which is flexible, and capable of
being folded into a small volume prior to deployment into the prescribed
shape.
Still another object of the invention is to provide an improved mesh
reflector for radio waves wherein the mesh-forming elements and spaces may
be precisely established and maintained.
These and other objects and advantages of the invention are realized by
providing mesh-forming material or elements comprising glassy base fibers
of high tensile strength, low elongation properties, and low coefficient
of expansion which fibers are coated with a thin layer of metal. By
forming such fibers of appropriate diameters and by maintaining the
prescribed spacing therebetween when formed into a mesh article, an
excellent reflector of radio waves for a particular frequency thereof may
be provided. Such mesh articles are lightweight, flexible and foldable.
The mesh configuration is achieved by bonding the fibers together at their
intersections. It was discovered that such mesh articles appear to possess
what may be called a "shape memory" that aids considerably in deployment
of the article to the desired shape after it has been folded.
The invention will be described in greater detail by reference to the
drawings in which:
FIG. 1 is a perspective view partly in section of a mesh structure
according to the invention;
FIG. 2 is an elevational view partly in section of a pair of intersecting
fibers showing the same in greater detail; and
FIG. 3 is a perspective view of mesh radio wave reflector according to the
invention.
Mesh articles according to the invention are formed by threads or fibers
having high tensile strength, low elongation, and a low coefficient of
expansion. Suitable fibers are available from inorganic materials such as
fused quartz, other various glasses formed of fused metal oxides and/or
metal silicates which may be drawn from the molten state into continuous
fibers. Such fibers are referred to hereinafter as "glassy". The term
"quartz" as used herein refers to the material of chemical formula
SiO.sub.2, usually found in crystalline form in nature as well as to
noncrystalline or vitreous materials. These fibers 2 are coated with a
thin layer 4 of metal and retain their desirable physical properties
without degradation and also become electrically conductive. The metal
usually employed to coat the quartz fibers is typically aluminum and
coating is achieved by freezing molten aluminum on the surface of the
fiber. Quartz fiber, meaning silicon dioxide formed into fibers, is a
preferred fiber material because of its exceptionally low coefficient of
thermal expansion and other excellent properties.
Such metal-coated fibers are stretched over a mandrel or surface having the
desired shape so as to form a mesh structure with the desired mesh
spacings and are bonded together at their intersections, as shown in the
drawing, with an adhesive 6 preferably of the epoxide type although other
elastomeric and/or glassy adhesives may also be employed. After curing or
hardening the adhesive, a stable mesh structure is obtained which is
flexible and foldable.
In a typical example, a mesh structure for use as a reflector of incident
energy at a frequency of 1500 megacycles was fabricated using quartz
fibers coated with aluminum and having a composite diameter of 6.5 mils. A
square mesh pattern with a spacing of approximately 1/2 inch was formed.
After curing the adhesive, a stable mesh structure was obtained having a
weight of 0.002 lb./ft.sup.2 which reflected better than 90% of the
incident energy. A similar structure was fabricated employing such quartz
fibers having a diameter of 2.5 mil. With a mesh spacing of from 1/4 to
1/8 inch better than 90% of incident energy having a frequency of 5000
megacycles was reflected.
In general, the fiber spacing is predetermined by the frequency of the
radio waves to be reflected. The following table demonstrates the
approximate relationship between fiber spacing and frequency to achieve
better than 95% reflectivity of the incident energy:
Frequency
Wavelength, .lambda.
.lambda./20,
Band Hz Inches inches Fibers/Inch
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VHF 300 39.4 2.5
U 1200 9.8 0.6 2
S 3300 3.5 0.22 5
C 5000 2.3 0.14 7
7000 1.67 0.104 9.6
X 8000 0.093 11
9000 1.3 0.082 12
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As noted previously, a material suitable for a mesh-type reflector of radio
waves, especially for use in outer space, should be lightweight, strong,
and electrically conductive. While fused quartz fibers have remarkably
high tensile properties, having strengths of 800,000 psi when tested in
air and 1,200,000 psi when tested in vacuum, these fibers on first
consideration appear to have several serious drawbacks for use as a
reflector of radio waves. For one thing, the strength of quartz fibers
degrades catastrophically when abraded or subjected to chemical attack --
mere exposure to atmospheric moisture causes a large reduction in
strength. In providing such quartz fibers with a metallic coating to
render them suitable for reinforcing massive aluminum metal, it was
discovered that the fibers retained to a substantial degree their
attractive initial physical properties and quickly regained their strength
upon drying after being exposed to moisture. This was found to be
particularly true when a metal coating of aluminum is employed which
equals in cross-sectional area that of the quartz fiber itself and this is
a preferred form for the metallized quartz fibers of the invention. In
general, the requisite thickness of metal is about 0.4 times the radius of
the quartz fiber yielding an equal area of metal to quartz in cross
section.
Another undesirable characteristic of quartz fibers was their tendency to
break in flexure at any microscopic flaw in their surface, particularly as
might arise when abraded as during folding. It was found, however, that
fibers when metal-coated were not significantly degraded by flexure which
thus makes it feasible to fold the mesh structures of the invention into
small volume packs for later deployment in outer space.
Among the other outstanding physical properties of quartz fibers which
makes them exceptionally useful as mesh structures in space applications
are its elastic moduli, low coefficient of thermal expansion, and low
density. The elastic modulus (rigidity modulus = 4.5 .times. 10.sup.6 ;
Young's modulus = 30 .times. 10.sup.6) approach that of steel. Fiber
elongations resulting from electrostatic pressures and space environmental
loads have been found to be negligible. Because of their exceptional
flexibility, these fibers can be folded to extremely small radii of
curvature without breaking or kinking. The high elastic modulus together
with the low coefficient of thermal expansion (0.5 .times. 10.sup..sup.-6)
make it possible to obtain the very high precision necessary in the
fabrication of mesh structures over a high tolerance mandrel. The low
density of quartz (2.6 gm/cc) which is approximately equal to that of
aluminum enhances the low weight of the over-all structure.
When employed as a reflector for radio waves, the high porosity (95% at 8
GH.sub.z) of the mesh reduces solar shading problems to a minimum and
further minimizes thermal distortions of the whole antenna and spacecraft
structural system. Likewise the low temperature coefficient of the quartz
material essentially eliminates the thermal distortion problem in the
reflecting surface itself. At the same time, the high porosity of the mesh
permits the reflecting surface to be uniformly illuminated with minimum
thermal gradients.
As shown in FIG. 3, a typical antenna structure according to the invention
is a paraboloid mesh, the mesh being formed in the same operation as the
paraboloid, yielding a smooth curved shape which is dimensionally stable
and maintains its parabolic contour. Such an antenna mesh is essentially a
network of fibers precisely spaced on a male mandrel of exact paraboloidal
contour. The fiber spacing is predetermined by the frequency of the RF
energy to be reflected. The interweaving of fibers, as in normal cloth or
screen, is preferably avoided in the design of the mesh for the following
reasons. The weaving of fibers causes a bending of the fibers at the
cross-over points and the fiber is no longer a straight structural member
able to support tensile loads without undue strain. Secondly, the
interweaving of fibers complicates the fabrication of large meshes to an
extreme degree because it requires weaving machinery to control the
movement of each fiber as additional fibers are added to the pattern. The
significance of this complication will be appreciated when it is
considered that an antenna having a diameter of 120 feet and 10 fibers per
inch will require a total of 28,800 fibers having a total length of 660
miles.
According to the invention, the individual fibers are held in position and
in correct relation to each other by bonding the fibers to each other at
cross-over points or intersections. In this way, structural continuity is
maintained throughout the mesh without deforming or bending the fibers.
The fibers are laid individually in place in a predetermined winding
pattern on a male mandrel of precise shape. Each fiber is bonded to a
peripheral ring and, after the entire mesh is in place, the fiber
intersections are bonded. After removal of the mesh and ring assembly from
the mandrel, it may be folded and packaged. A convenient way to fabricate
the mesh structures of the invention is to machine grooves in the mandrel
surface for retaining the fibers therein during assembly. These grooves
may be V-shaped and only deep enough to accommodate the fiber. Small holes
may be provided at the intersections of the grooves in order to free the
fiber from the mandrel to permit unimpeded bonding.
Another method for fabricating a mesh structure for patterns other than
geodesic is to spray a pressure-sensitive adhesive on the mandrel. Fibers
laid on the mandrel will therefore remain in position during bonding.
After completion of the mesh, the adhesive film may be chemically
dissolved and the mesh removed from the mandrel. Vinyl or siliconebased
adhesives are satisfactory for this technique.
In applying the adhesive or bonding agent to the cross-over points of the
fibers, it has been found that the adhesive wets and wicks between the
intersecting fibers to form a small bead. The adhesive bead cures to form
a structural bond having a shear strength of from 2000 to 3000 psi. It is
generally preferable, especially where the fibers are closely spaced and a
mandrel without grooves is employed to place the first layer of fibers on
the mandrel and bond each intersection of each fiber as the second and
succeeding intersecting fibers are laid in place. This may be accomplished
by mounting an adhesive applicator on the fiber feeding mechanism to
precede the fiber and apply the adhesive thereto as it is fed onto the
mandrel. After the first layer of fibers is complete, the adhesive
applicator is adjusted in height to deposit a small amount of adhesive on
each fiber it passes over. The fiber being placed on the mandrel directly
behind the adhesive applicator therefore encounters adhesive at each
intersection.
An alternate and less complex procedure is to spray or brush the entire
mesh with a dilute adhesive followed immediately with a dry brushing or
blotting operation to remove excess adhesive except that which is wicked
between intersecting fibers. While a thin resin coating might adhere to
the upper surface of the fibers, the additional weight and stiffness added
to the mesh would be negligible.
The selection of a suitable adhesive for the bonding of the fibers is based
primarily on ease of application and good wetting properties. A
satisfactory adhesive giving excellent results is an amine-cured epoxy
system. The joints resulting are formed by a resin bead approximately 1/32
inch in diameter. Typical adhesive for the purposes of the present
invention comprises 100 parts of an epoxy prepolymer cross-linked by ten
parts of diethylene triamine. The useful life of this adhesive system is
30 to 60 minutes at room temperature. Usually the adhesive system is
prepared in 100 gram batches and blended with 1% of a carbon black slurry
to facilitate observability of the resin and the bead formed thereof. The
epoxy resin cures to a hard glassy polymer in approximately three hours at
room temperature. Flexible or rigid adhesive systems may be employed.
Generally, with close fiber spacing of ten per inch or more, it may be
necessary to employ a low modulus, high elongation elastomeric adhesive to
provide flexibility in the final mesh. Elastomeric properties may be
imparted to epoxy adhesives by modifying them with polyamines. In
addition, many silicone and polyurethane systems have the required
properties.
One of the novel and advantageous features of a mesh article according to
the invention is the fact that the article may be formed into a
configuration having at least one axis of curvature and still be of
one-piece or unitary structure. Previously, doubly-curved mesh articles,
for example, had to be formed from a plurality of pieces which were joined
together. The mesh articles of the invention are capable of being formed
into such doublycurved configurations without discontinuities and hence
are referred to herein as unitary.
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Description  |
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