Exact involute ply patterns

Claim 2

A hollow symmetrical structure, in the form of a body of revolution, comprising a plurality of a preselected number of identically shaped and sized exact involute surface plies which are successively disposed and joined circumferentially in a contacting, stack-like layered, and overlapping relationship.

Claim 3

A hollow symmetrical structure, as set forth in claim 1, wherein said body of revolution has inner and outer profile definitions and limitations, an inner surface, an outer surface, a top surface, and a bottom surface, and wherein each exact involute surface ply of said plurality has a limiting sized thickness, a limiting sized width, and a length extending from said inner surface of said body of revolution to said outer surface of said body of revolution, with each said ply positioned such that it extends from said top surface of said body of revolution to said bottom surface of said body of revolution.

Claim 4

A hollow symmetrical structure as set forth in claim 2: a. wherein said exact involute surface of each said ply is defined by the equations: r sin α=c, where r≧c and θ(α,z)-θ(z.sub.o)=Q(z-z.sub.o)+.sup.α (z.sub.o)+cot.sup.α (z.sub.o)-.sup.α (z)-cot.sup.α (z) where ##EQU7## b. wherein said exact involute surface of each said ply has an inner edge and an outer edge, and said inner edge is defined by the equation: θ.sub. (z)-θ.sub.1 (z.sub.o)=Q(z-z.sub.o)-α.sub.1 (z)-cot α.sub.1 (z)+α.sub.1 (z.sub.o)+cot α.sub.1 (z.sub.o) and said outer edge is determined by the equation: θ.sub.2 (z)-θ.sub.1 (z)=α.sub.1 (z)+cot α.sub.1 (z)-α.sub.2 (z)-cot α.sub.2 (z) where R i (z) sin α i (z)=c; i=1,2, and also c. wherein said limiting sized width of said exact involute surface of each said ply is defined by the equation: ##EQU8## where s(z)≦w; wherein, in all applicable foregoing equations: N=preselected number of plies T=preselected limiting sized thickness of each ply w=limiting sized width of each ply c=involute constant, where 2πc≧NT r,θ,z=radial, central angular, and axial coordinates, respectively α=arc angle γ=tilt angle; tan γ=dr/dz s=arc length R 1 (z),θ 1 (z)=radial and central angular coordinates of inner edge of involute surface R 2 (z),θ 2 (z)=radial and central angular coordinates of outer edge of involute surface and, thereby said exact involute surface of each said identical ply, and boundaries of said surface, are defined and limited.

Claim 5

A hollow symmetrical structure, as set forth in claim 3, wherein a flat ply pattern of said defined and limited exact involute surface of each said bounded identical ply is developed approximately by the equations: s.sub.ij =[(x.sub.i,j+1 -x.sub.ij).sup.2 +(y.sub.i,j+1 -y.sub.ij).sup.2 ].sup.1/2 l.sub.j =[(x.sub.2j -x.sub.1j).sup.2 +(y.sub.2j -y.sub.1j).sup.2 +(z.sub.2 -z.sub.1).sup.2 ].sup.1/2 ##EQU9## where ≧ (φ.sub.j,β.sub.j,λ.sub.j,v.sub.j,u.sub.j)≦.pi. wherein said developed flat ply pattern is in the geometric shape of a quadrilateral; and wherein: x=an axis y =an axis coplanar with, and perpendicular to, said x axis ##EQU10## (x 1 ,j+1; y 2 ,j+1)=still another plane coordinate point of said quadrilateral (x 2 ,j+2; y 2 ,j+2)=yet another plane coordinate point of said quadrilateral S 1j =one side of said quadrilateral, with this side extending from coordinate (x 1j ,y 1j ) to coordinate (x 1 ,j+1 ; y 2 ,j+1) .sub. j =another side of said quadrilateral, with this side extending from coordinate (x 1j , y 1j ) to coordinate (x 2j , y 2j ) φ j =the angle bounded by sides S 1j and 1 j , and internal of said quadrilateral. p j =diagonal of said quadrilateral, facing φ j , and extending from coordinate (x 1 ,j+1 ; y 1 ,j+1) to coordinate (x 2j , y 2j ) B j =the angle bounded by side 1 j and diagonal p j , and internal of said quadrilateral V j =the angle bounded by side S 1j and diagonal p j , and internal of said quadrilateral λ j =the angle internal of said quadrilateral, and bounded by diagonal p j and a side (S 2j ) of said quadrilateral which extends from coordinate (x 2j ,y 2j ) to coordinate (x 2 ,j+1 ;y 2 ,j+1) μ j =the angle internal of said quadrilateral, and bounded by diagonal p j and a side (1 j+1 ) of said quadrilateral which extends from coordinate (x 1 ,j+1 ;y 2 ,j+1) Ω j =the angle bounded by 1 j and the x axis.

Claim 6

A hollow symmetrical structure, as set forth in claim 4, wherein adjacent identical plies of said plurality are circumferentially overlapped a distance d which is defined by the equation: d(z)=2πR.sub.2 (z)/N where: d(z),R 2 , and N are defined as hereinbefore.

Claim 7

A planar symmetrical structure, as set forth in claim 1, wherein said successively circumferentially disposed and joined identical plies are joined by bonding.

Claim 8

A hollow symmetrical structure, as set forth in claim 5, wherein each said identical ply is made of a matrix of graphite cloth reinforced with phenolic, which said matrix is impregnated with a pitch-furfural blend, carbonized, and graphitized.

Claim 9

A hollow symmetrical structure, as set forth in claim 1, wherein said structure is for use as part of a rocket nozzle.

Claim 10

A hollow symmetrical structure, as set forth in claim 8, wherein said part of said rocket nozzle is an exit cone.

Claim 11

A hollow symmetrical structure, as set forth in claim 9, wherein said preselected number of identical plies is 92.

Claim 14

A method of fabricating a hollow symmetrical structure in the form of a body of revolution, as set forth in claim 10, comprising the step of determining said predetermined distance by the following equation: d(z)=2πR.sub.2 (z)/N wherein d=said predetermined distance N=said predetermined R 2 (z)=radial coordinates of outer edge of each of said plies.