978-0124081369 Chapter 11 Part 1

subject Type Homework Help
subject Pages 9
subject Words 1951
subject Authors Martin H. Sadd Ph.D.

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page-pf1
11.1.
exist moduli elastict independen 21only that implies thus
and symmetric ismatrix stiffness canisotropi 66 general the thusand
s,Hooke' From
=
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kl
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ee
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e
page-pf2
11.2.
relations. newany producenot wouldplane, about the reflection (third) final theEmploying
constants. elastict independen nine with materials corthotropifor form desired thegiving
0
00
000
000
000
ations transform twoThese
0
0
0
0
tensor,elasticity for the lawtion Transforma
100
010
001
Q:plane, about the Reflection
0
0
0
0
0
0
0
0
tensor,elasticity for the lawtion Transforma
100
010
001
Q:plane, about the Reflection
s.reflection three theChoose planes. coordinate theofeach about sreflection three
or axes coordinate about the rotations threedoeither toequivalent isIt
13
66
55
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2322
131211
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3633122133331236
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page-pf3
11.3.
22
222
22
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4
22
22
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22
12
4
11
22
4
66
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2
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)cossin()coscossin2(sin
coscossin)(2cossin2sin
coscossin4cossin2sin
C
:Check
)sin(cossincos
C
:Check
100
0cossin
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:bygiven isrotation particular The
2/)(, :and
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CCC
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page-pf4
11.4.
0
3
2
0)23(40
2
2
2
0
2
2
0:Case Isotropic
2)(00
00
00
:Case Isotropicly Transverse
2
00
00
00
00
:Case cOrthotropi
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0 minors principal all so and definite positive bemust
2
4
2
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1
++
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p
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page-pf5
11.5.
11
0
11
0
11
0
positive be ofminor principaleach that function energy strain definite Positive
0
00
000
000
000
, materials corthotropiFor
2
1
3
2
31
2
3
31
13
2
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1
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=
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page-pf6
11.6.
page-pf7
11.7.
0
02
as writtenbe can equation aldifferenti original The
,2
roots for the quadratic theSolving
equation sticcharacteri02
0)2(
parametera is where,)(),( form theof solutionsfor Look
02
:equation sHomogeneou
21
22
2
2
22
55
45
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2
55
44
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55
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fSSS
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page-pf8
11.8.
xyyx
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+
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662616
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16
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11
2
00 withrelations stress plane develop to wishNow we
strain planefor law s Hooke'into relations theseUsing
,,
,,
(11.5.3) Relations
11.9.
form the yieldsbefore as gIntegratin
, with
0 : EquationGoverning
,:2Case
4321
4321
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DD
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page-pf9
11.10.
( )
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,94.2
17
50
:materialy Glass/Epox-SFor
22
2
1
:for equation quadratica as Solving
0)2(
0 materials corthotropiFor
02)2(2
2,1
2
2
2,1
12
1
12
11
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1
11
22
11
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11
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2
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=
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11.11.
)]()([2
)()()()(
)()()()(
)]()([2
)()()()(
)]()([2
)()()()(
)()()()(
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page-pfa
11.12.
strainshear for the expression thein results theseUsing
)()]()([2
)()]()([2
relationsnt displaceme-stain thegIntegratin
/)(and where
)]()()()[(22
)]()([2
)]()([2
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stress, planeFor
)]()([2
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page-pfb
11.13.
)]()sincos()()sincos[(2
)]()sincoscossincossin(
)()sincoscossincossin[(2
)sin(coscossincossin
)]()sin(cos)()sin[(cos2
)]()cossin2cossin()()cossin2cossin[(2
cossin2cossin
)]()cos(sin)()cos[(sin2
)]()cossin2sincos()()cossin2sincos[(2
cossin2sincos
theory,ation transformstress From
)]()([2
)]()([2
)]()([2
:Stresses
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2
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2
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11
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2
1
222
222
2111
222
1
22
22
2
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2
1
222
222
2111
222
1
22
222111
2211
22
2
211
2
1
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z
zRe
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+++
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++=
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page-pfc
11.14*.
 
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545.5,577.0 :yBoron/Epox
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: MATLABUsing
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2
1
2
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,1 case, isotropic For the
Defining
4
22
2
1
:for equation quadratica as Solving
0)2(
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02)2(2
:equation sticcharacteri General
2,1
2,1
2,1
2,1
22
2,1
11
6612
11
22
2
2,1
2
2,12,11,2
11
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2,1
2
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page-pfd
11.15.
*)}(){(2
*)}(){(2
*)}({2*)}({2*)(*)( real bemust Since
* where,*)(*)()()(
as written becan equation governing osolution t general so and
),( pairs conjugatecomplex are rootsshown previously As
-
:gives roots twofor the Solving
02
equation sticcharacteri quadratic theproduces termcommon theCancelling
0)2(gives)( solutionsfor Looking
020 Eqns. Equilbrium
22
22
0
0
2
2
0
0
0
0
0
00
00
00
becomes materials monclinicfor law sHooke' thereforeand
,0),(,0With
4544
5545
111
2121
2
44
5544
2
4545
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2
44
2
444555
2
2
44
2
45
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2
55
45444544
55455545
66
55
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3633
262322
16131211
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zFCCRe
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yxzzFzFyxFyxFw
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F
FCCCyxFw
w
C
w
C
w
C
x
w
C
y
w
CeCeC
x
w
C
y
w
CeCeC
e
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C
C
CC
CC
CCC
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eeeeyxwwvu
yz
xz
yz
xz
xzyzyz
xzyzxz
xyzyx
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yz
xy
zx
yz
z
y
x
xyzyx
+=
+=
==+=
+=+=+++=
=
=++
=
+++=
=
+
+
=
+
+
=+=
+
=+=
====
=
=======

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