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The Behavior of
3 _: n4 k' C: Z. \" V6 UStructures Composed of
7 {* d+ e; ]1 o0 m- ^! ^Composite Materials- a) @) V. V1 L
Second Edition2 y/ L1 t0 v2 g J( P* l
by
+ q: p. H2 Q5 s3 uJACK R. VINSON6 t/ V3 Z# M' H) i
H. Fletcher Brown Porfessor of Mechanical & Aerospace Engineering,7 v: Q9 `% W9 V% P W
The Center for Composite Materials and The College of Marine Studies,
+ d/ k A4 t6 nDepartment of Mechanical Engineering," @+ q$ }2 h6 D' D& |
University of Delaware,
+ l2 L4 j+ a! M* jNewark, Delaware, U.S.A.
4 h. R. X& O# Sand" ^" M; F1 Y% z r, d* F6 Q4 R
ROBERT L. SIERAKOWSKI5 j. C( v0 n5 i( I1 X/ p, [
Chief Scientist,' k# z1 s; i7 `3 {6 {: C S
AFRL/MN Eglin AFB,
) h0 k5 K! V; o7 |: u) ]Florida, U.S.A.
9 |) e' _3 ^2 ^. Z0 W# m6 y5 ^% G! P: Q9 J
9 p9 p n: d) m' F
+ z; P* G* |2 Q' ]Contents
% M. g) Q6 }7 {) n1 v% R) g6 K' p2 U
1. Introduction to Composite Materials 1) g. J. h7 U5 K2 l0 Y$ S0 Y
3 J( u# B0 d/ Y. N; K, o$ P$ [ DGeneral History
' A' E7 \. F- ~5 vComposite Material Description' j8 ^; J9 K9 k' g
Types of Composite Materials
. K% ]* s2 B; S" _! L) aConstituent Properties
- A" Q0 F& D: ^' p ~' c$ a" b! N6 AComposite Manufacturing, Fabrication and Processing
7 V: p2 m2 @* Y! u9 [9 zUses of Composite Materials }0 Q5 s1 l" c I9 L1 j
Design and Analyses with Composite Materials
" x7 h, D/ u* D( t) A4 Z. s8 z& i9 eReferences5 z/ i. ` u% n* C
Journals0 W& n% ^7 P9 l, N) D
Problems
( @2 V% I d. n; i: |9 o% o, E( U- q& E6 o( S
2. Anisotropic Elasticity and Composite Laminate Theory5 t! r2 r2 y0 B2 f4 S# r4 J# _
5 K: `: u; @+ T' t# `
Introduction
* N) q, o) O4 K7 J; _, D X& zDerivation of the Anisotropic Elastic Stiffness and Compliance Matrices
, y y% O2 Z! h% C0 e% ~2 AThe Physical Meaning of the Components of the Orthotropic Elasticity
) T. b; o; e0 N& u% l% sTensor
" p3 f+ f! @" c( D( zMethods to Obtain Composite Elastic Properties from Fiber and Matrix3 h4 S+ @# ~) K/ ]
Properties
; _' B5 H" U4 ?Thermal and Hygrothermal Considerations
' h+ D- g! S i9 W! t8 s8 |; iTime-Temperature Effects on Composite Materials
4 m6 L1 _5 `1 g& r% c) ?) Q5 wHigh Strain Rate Effects on Material Properties
' j8 j4 q0 c5 ^9 s, m0 w( [- bLaminae of Composite Materials
1 C) K& ~0 d: M) D# v+ VLaminate Analyses5 b) X. F$ y% `# P
Piezoelectric Effects- U/ s I( d) Y e
References, d. A7 d0 h5 T
Problems
9 t. K8 U. {+ P: e! v
3 P* Y& b' v8 k6 E3. Plates and Panels of Composite Materials
4 z8 S" f7 \9 ~- S' {; [. q8 U2 l% v8 `; _( f
Introduction
; G; j! H' v; `# u! }* cPlate Equilibrium Equations
6 q% n) f" F: X, W; I$ J* y) g) D: GThe Bending of Composite Material Laminated Plates: Classical Theory$ T9 c8 Q: }1 F' [
Classical Plate Theory Boundary Conditions# I3 S0 z4 O5 k6 U% e; c& H2 h
Navier Solutions for Rectangular Composite Material Plates
4 L8 ]# N& \# f0 T1 ?1 B5 h' @2 VNavier Solution for a Uniformly Loaded Simply Supported Plate – An
$ K9 D, y9 a- m5 g. ]1 ]Example Problem
( w$ X- b0 d( E5 WLevy Solution for Plates of Composite Materials
9 k5 w8 m* |! r. s i4 T7 ]) ?8 B2 @# @8 ~% V, \/ r% I
Perturbation Solutions for the Bending of a Composite Material Plate With
! D2 L# k1 E4 d( iMid-Plane Symmetry and No Bending-Twisting Coupling
1 t/ }6 D! B8 g0 d% L, YQuasi-Isotropic Composite Panels Subjected to a Uniform Lateral Load
7 f8 A% c7 H2 J5 X/ K. l; |' q iA Static Analysis of Composite Material Panels Including Transverse+ T: [" S$ o9 Z$ E* ~) b
Shear Deformation Effects
3 a. z& t! `/ z wBoundary Conditions for a Plate Using the Refined Plate Theory Which
) r1 o% d6 _; D$ m7 }9 SIncludes Transverse Shear Deformation+ x. F& T5 D3 Z" t8 k/ p+ K
Composite Plates on an Elastic Foundation
6 h& K, h/ j3 i& p- @6 vSolutions for Plates of Composite Materials Including Transverse-Shear7 } l9 d. }1 S6 I0 R# X' m2 w' ^
Deformation Effects, Simply Supported on All Four Edges4 t V5 d! S4 j+ D1 r! ?3 H
Dynamic Effects on Panels of Composite Materials; {7 n* p4 e( _
Natural Flexural Vibrations of Rectangular Plates: Classical Theory
/ D& ]4 O' W1 }1 E. J. a5 _Natural Flexural Vibrations of Composite Material Plate Including# \( ] R7 i* K: ^' I4 r8 ^
Transverse-Shear Deformation Effects
6 _% o" N# M% K1 L- E% p+ IForced-Vibration Response of a Composite Material Plate Subjected to a
9 n8 |) G; G' c ?+ e8 p# NDynamic Lateral Load2 L7 u3 P8 e& }/ p1 d
Buckling of a Rectangular Composite Material Plate – Classical Theory
! X6 U2 N I2 |7 xBuckling of a Composite Material Plate Including Transverse-Shear4 }& O" E: W2 l# Q9 B; ^
Deformation Effects
' ?. y6 p3 a9 N! w4 {Some Remarks on Composite Structures- ?$ w/ ^' W0 w! G, @& h
Methods of Analysis for Sandwich Panels With Composite Material" _" h2 Y$ J$ R. s
Faces, and Their Structural Optimization
' h' n, a: K5 F* lGoverning Equations for a Composite Material Plate With Mid-Plane
. Y2 S, N1 u% u7 |) o5 YAsymmetry( |0 P; p3 s0 ?
Governing Equations for a Composite Material Plate With Bending-
5 {" ~5 X# w6 Q: e' ITwisting Coupling
0 S$ V9 z6 f" c/ S8 B! [- `/ hConcluding Remarks
) y- o: [+ U' H% v& {% TReferences
7 }8 y+ a4 s7 GProblems and Exercises
* x. Z8 g& V7 j6 A- P* U( I, l, V9 G. a, ?) N
% `0 x7 e4 a7 X+ r; @6 E$ E4. Beams, Columns and Rods of Composite Materials6 {- {7 p' o. L( o. a
' V4 C( C- B8 x$ u# C+ J" M
Development of Classical Beam Theory
# v- ~7 G, p) b' L H2 nSome Composite Beam Solutions) N9 b) ~2 g5 e# O$ o( M3 G8 _3 M* |0 n
Composite Beams With Abrupt Changes in Geometry or Load) h4 f& y% m+ k8 V
Solutions by Green’s Functions
" `: Y8 e# p0 l( UComposite Beams of Continuously Varying Cross-Section
* o! b* Q- b' W yRods
( y! g" q {6 x( K. U( S3 oVibration of Composite Beams2 }% e$ U3 W( W u0 j
Beams With Mid-Plane Asymmetry! j9 H% Y1 m: O8 U- I
Advanced Beam Theory for Dynamic Loading Including Mid-Plane
0 k; C. Y' q, d& @Asymmetry
, ~2 n$ [% Z4 W+ r9 ~Advanced Beam Theory Including Transverse Shear Deformation Effects8 i# ]+ j: N+ }
Buckling of Composite Columns
2 ~) d% P8 U5 O8 }, M% mReferences7 R$ X5 l; ~+ g5 o- |3 Z4 e" _
Problems9 S# y+ d& ]' `8 Z- P
6 j3 M+ F- j7 s0 @3 | E
! u# F' p7 S# K4 h( f/ \5 T5. Composite Material Shells
% a/ O" d- A5 M& D$ p5 i/ w9 ?* t
7 R1 n: v5 M) V; E0 z4 G+ SIntroduction' Y( ?9 \( a" V; j
Analysis of Composite Material Circular Cylindrical Shells: r1 u/ n! B+ e3 z, A' D
Some Edge Load and Particular Solutions
/ q& ^' K3 ?7 `6 T% x3 pA General Solution for Composite Cylindrical Shells Under Axially
! X* D: h9 _8 p! V, w3 ^Symmetric Loads: |% [( j) T$ v) h
Response of a Long Axi-Symmetric Laminated Composite Shell to an, F* M6 A M3 z4 q6 d L! k
Edge Displacement, b3 z( A+ F. B- y6 z1 K
Sample Solutions
, a9 X/ l8 v% [Mid-Plane Asymmetric Circular Cylindrical Shells1 Q* j! B# c) i, k! y0 F
Buckling of Circular Cylindrical Shells of Composite Materials Subjected* F8 s/ P+ w* p% U& x
to Various Loads" |+ i7 k3 B! @' k \
Vibrations of Composite Shells! g: x1 i- ^( H, \: y
Additional Reading On Composite Shells1 \7 u. z+ l9 `. B/ \
References6 N% ^+ J6 n8 N' U( Z. I4 V2 W3 q! c
Problems
6 ^9 r+ i1 t& c3 j/ v) t: S& F6 A/ d0 E8 z, T) c
% F; M7 z7 F/ F+ r% |
6. Energy Methods For Composite Material Structures4 D5 T; Q4 {* N- ~
& I: [3 l2 }* q" h6 B9 S) B" [4 ?
Introduction
6 z3 K) L2 z' h0 o2 O. J$ F6 sTheorem of Minimum Potential Energy% X4 @) O& V; F1 ^8 D! a2 B
Analysis of a Beam Using the Theorem of Minimum Potential Energy
; M4 z! X% `8 J9 m9 K, RUse of Minimum Potential Energy for Designing a Composite Electrical
1 p3 k3 x/ {, p8 K6 V( WTransmission Tower
6 Q" B# e7 v+ g5 JMinimum Potential Energy for Rectangular Plates
2 Q5 C: m8 n6 ^4 YA Rectangular Composite Material Plate Subjected to Lateral and
; M; q" l% r* h+ B1 A' }Hygrothermal Loads
# y$ D, V8 R4 n3 d, J% o9 V0 kIn-Plane Shear Strength Determination of Composite Materials in
, w& |, J* L. I% aLaminated Composite Panels! G/ z6 U- c6 i3 }! C2 p
Use of the Theorem of Minimum Potential Energy to Determine Buckling( {1 W4 m2 n9 o1 T, a, l% g9 }3 j
Loads in Composite Plates
k3 R' m0 d1 X" }Trial Functions for Various Boundary Conditions for Composite Material
/ m/ F/ X4 }% Y6 W4 k* H0 qRectangular Plates
# j7 d8 ~8 c+ F3 i yReissner’s Variational Theorem and its Applications4 b3 y/ M* s8 j* e
Static Deformation of Moderately Thick Beams
/ L- T7 V5 {' AFlexural Vibrations of Moderately Thick Beams t0 ]; D- O2 M2 i
Flexural Natural Frequencies of a Simply Supported Beam Including2 \% T: B5 N t2 ]
Transverse Shear Deformation and Rotatory Inertia Effects
0 U+ D5 V2 n" iReferences1 u$ A, i0 F% l) M
Problems! i7 X! U) o) K+ W8 P( e. ?
. R8 U7 i, ~9 n/ L6 g0 P* S7. Strength and Failure Theories
) D9 d% o4 W! y7 ~' O) f( h' f8 ~0 K' V/ c! n- ~0 V# P1 V
Introduction
* ^: f' b; Z$ z4 iFailure of Monolithic Isotropic Materials; [7 A( l3 x+ r# p
Anisotropic Strength and Failure Theories5 r8 w6 S- E( y5 x9 l8 x( A
Maximum Stress Theory
0 r, n! P( L5 @- k: s, A+ OMaximum Strain Theory
+ w, P2 g& g: m1 A4 e/ AInteractive Failure Theories
: H X/ Q, V7 P: x/ @6 y( O" BLamina Strength Theories2 u7 q4 Z l/ g/ L1 \, F; ~$ o
Laminate Strength Analysis
& V5 g+ f7 a( |8 j7 l) GReferences5 S- f M& l4 j+ n( h- x" ^
Problems
5 @0 A9 W% n9 D# q* l* Y! R0 O" A6 l5 L3 p9 ?1 c0 j
, R/ z- }4 ^- h2 o8 x" {
8. Joining of Composite Material Structures% M0 j' `7 e" d# T7 S$ M7 [
! F6 t0 u: x3 `! ~
General Remarks
- w7 r* q5 Z: V) OAdhesive Bonding) j4 {/ I/ J0 X4 ? q+ ~
Mechanical Fastening
n2 o' y5 T: z, w4 _* P+ dRecommended Reading
4 H. e% |$ V6 r; SReferences
: E3 V5 r/ ^8 U5 y7 {! wProblems
; }: o7 s# L ^0 m3 q9 f# Z% n0 |% _0 b
: v! S! F) a" W! P q% i3 v9. Introduction to Composite Design
/ D" L$ B6 ?& t1 Q4 [
( @6 d5 S- Z! v6 J; S5 ]. D$ MIntroduction
! M) `0 t3 N1 X4 H, w5 b- p$ h: E: c, LStructural Composite Design Procedures
, W6 b9 {7 h0 L& I$ gEngineering Analysis
9 b4 e8 K7 \1 PAppendices: Y2 P! j4 g; L+ V: o: H
* p1 Q- h! @$ V% M
) B& }2 B2 m+ \+ S, |+ v3 {& NMicromechanics& x2 [" h4 ]. e$ ?- Z
Test Standards for Polymer Matrix Composites
5 [" i: \4 E5 S4 i( W& s% {. @- fProperties of Various Polymer Composites
6 g; D% [. e j& G X) SAuthor Index
, ]0 w1 G& Z) g8 JSubject Index
3 j, w l) F( E$ o% a& e) t, k7 F# a
[ 本帖最后由 jove20020 于 2008-2-22 23:41 编辑 ] |
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