978-0124081369 Chapter 8 Part 3

subject Type Homework Help
subject Pages 9
subject Words 1433
subject Authors Martin H. Sadd Ph.D.

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page-pf1
8.39.
)cos31(
2
cos
2
)cos1(
2
sin
2
)
2
sin
3
5
2
3
sin()
2
cos5
2
3
cos(
1
4
3
:coordinateangular theChanging
)
2
sin
3
1
2
3
(sin)
2
cos
2
3
(cos
1
4
3
)
2
cos
2
3
(cos)
2
sin3
2
3
(sin
1
4
3
)
2
cos
3
5
2
3
(cos)
2
sin5
2
3
(sin
1
4
3
gives relations stress general theinto results thesengSubstituti
3
)2(
,,
2
3
gave problem theon condtionsBoundary
])2sin()2()2cos()2(sincos[)1(
])2cos()2sin(cossin[)1(
])2cos()45()2sin()45(
cos)1(sin)1([
])2cos()2sin(cossin[
2
2
22
2
++
=
++
+=
==
=
+
=
++
+=
=
===
+=
+++=
++++
+=
+++=
r
r
BA
r
BA
r
BA
r
BA
r
A
A
CBD
DCBAr
DCBAr
DC
BAr
DCBAr
r
r
r
r
r
page-pf2
8.40*.
A
r
A
r
A
r
A
r
A
r
A
r
A
r
A
r
A
r
r
r
r
/ of contoursplot wish toWe
sin
2
3
2
cos
2
sin2
2
3
2
cos
2
sin
2
cos
2
sin4
2
3
2
cos4
2
sin
2
cos
2
sin4
2
3
)cos1(
2
sin
2
cos)cos1(
2
3
2
)cos1(
2
sin
2
3
)cos1(
2
cos
2
3
)cos3(
2
cos
2
3
:I Mode
max
2222
4224
2222
2
2
max
=
=
+
=
+
=
+
+
=
+
=
+
=
+
=
=
B
r
B
r
r
B
r
B
r
B
r
B
r
r
r
/ of contoursplot wish toWe
)3cos(1
2
2
sin
2
coscos6
2
cos
2
sincos9
2
cos
2
sin
2
2
2
2
2
)cos31(
2
cos
2
)cos1(
2
sin
2
3
)cos31(
2
sin
2
:II Mode
max
2
2222
2
2
+=
+
+
+
=
=
+
=
=
max - Contours Mode I
max - Contours Mode II
page-pf3
8.41.
2
sin
2
,
2
cos
2
,
2
sin
become stresses and ntsdisplaceme theso and2/110
10at StressesSingular
00at ntsDisplaceme Finite
,5,3,1,2/,5,3,1,2/ 0cos 0 since;0),(
:surfacescrack on conditionsboundary stress Zero
cos,sin,0
:aresolution nt displaceme from Stresses
singivespart odd only the Choosing,cossin :Solution
00
11
)1(
0in)( Using
11
2
2
12
2
=
=
=
=
======
=
==
=====
=+=
=+
=
++
==
r
A
r
A
rAw
r
r
nnnnr
rA
w
r
rA
r
w
AfBAf
fffr
r
fr
r
fr
wfArw
rzz
z
zrzrzr
page-pf4
8.42.*
% Solution Contours for Antiplane Strain Crack
Fields
clc; clear all; clf
[x,y]=meshgrid(-0.5:0.05:1,-1:0.01:1);
z Contours
page-pf5
8.43*.
2/)(,
)/log(
,,
)(
)(
:Solution Materialsof Strength
)][log(4)( with
])log()log()log([
4
222222
2222
2
22
baR
ab
ab
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a
b
baabN
ab
r
a
a
b
r
b
a
b
r
ba
N
M
+=
==
=
=
+++=
Ma /
2
page-pf6
8.44.
generated. becan
moment endarbitrary an for solution the(8.4.61),solution by given case bending pure theadding
by that however, notebut ;
2
)(
with case special for the solved is problem theSo
satisfied,log)()()2/,(
2
0
2
20),(),(
:case for this ConditionsBoundary Check
sin
2
2
1
cos
2
6
cos
2
2
11
cos)log( :function stress usingsolution exploreFirst
22
22
22
3
3
32
2
32
2
2
3
baT
M
T
a
b
Dab
ba
B
abATdrr
a
D
a
B
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r
D
r
B
Ar
rr
r
D
r
B
Ar
r
r
D
r
B
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r
rr
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r
B
Ar
b
ar
rr
r
r
+
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+=
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page-pf7
8.45*.
:Plots MATLAB
1
))/(1(
42
)//()0,(1
)4(
42
)0,(
)/(1
)/(12
)//()0,(
4
42
)0,(
are 0on stresses normal two the35,-8 Figurein shown problemdisk For
22222
4
2
2
2
2
22
22
+
=
+
=
+
=
+
=
=
Rx
DPx
xD
D
D
P
x
Rx
Rx
DPx
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D
P
x
y
yy
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-1
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0.5
1
)//()0,( DPx
y
page-pf8
8.46*.
0),0(,
1
2
2
2
22
),0(,
2
),0(
0,
1
)(
4
,
1
)(
4
)0( axis-On
)()()()(2
2)()()()(2
2)()()()(2
)(,
)()(2
1)()(2
1)()(2
)(,
)()(2
1)()(2
1)()(2
and of einterchang simple usingshown as problems two theofion superposit Use
22222
2
222
3
4
2
2
4
1
2
4
2
2
4
1
2
)2()1(
4
2
2
4
1
2
4
2
3
4
1
3
)2()1(
4
2
3
4
1
3
4
2
2
4
1
2
)2()1(
22
2,1
4
2
4
1
)2(
4
2
4
2
)2(
4
2
3
4
1
3
)2(
22
2,1
4
2
2
4
1
2
)1(
4
2
3
4
1
3
)1(
4
2
2
4
1
2
)1(
=
+
+
=
=
=
+
+
+
=
+
=
=
+
+
+
=+=
+
+
+
+
+
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+
+
+
+
+
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+=
+
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+
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=
+
+
=
+=
+
=
+
+
=
+
+
=
y
DyDyD
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y
D
P
y
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Ry
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D
Ry
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xy
r
yxR
r
yxR
r
xyR
r
xyRP
D
r
yxR
r
yxR
r
yR
r
yRP
D
r
xR
r
xR
r
xyR
r
xyRP
xRyr
r
yxR
r
yxRP
D
r
yxR
r
yxRP
D
r
xR
r
xRP
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r
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r
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D
r
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r
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D
r
xyR
r
xyRP
yx
xyyx
xyyx
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yyy
xxx
xy
y
x
xy
y
x
P
P
P
P
(1)
(2)
P
x
y
y
page-pf9
8.46*. Continued
MATLAB Comparison Plot:
)//( DP
page-pfa
8.47.
0,lim
, as case limiting for the so and Load Total
,16,8,4,0, (c) case general for the Thus
0,
8
twooffactor aby stresses theincrease thusandamount same theaddsimply will(b) casein
shown as loadings morefour ofaddition the).,(isotropic chydrostati are case(a)for stresses theSince
(b) Case
0
)()()()(2
42)()()()(2
42)()()()(2
:bygiven arecenter sdisk' at the stresses the8.46, Exercise From (a) Case
0,
4
2
2
4
1
2
4
2
2
4
1
2
0,
4
2
2
4
1
2
4
2
3
4
1
3
0,
4
2
3
4
1
3
4
2
2
4
1
2
==
==
===
==
==
=
==
=
+
+
+
=
=
+
+
+
+
+
=
=
+
+
+
+
+
=
=
=
=
xy
N
yx
xyyx
xyyx
yx
xy
yx
y
yx
x
p
D
NP
N
D
NP
pNPDp
N
D
NP
D
P
r
yxR
r
yxR
r
xyR
r
xyRP
D
P
D
r
yxR
r
yxR
r
yR
r
yRP
D
P
D
r
xR
r
xR
r
xyR
r
xyRP
page-pfb
8.48.
disk solid theof that twiceisdisk annular thein stress maximum the
)(,
8
3
)0()0(
11-8 ExampleFrom
8
)3(
)(, when
8
)3(
)(
8
)3(
8
31
)()(
8
)3(
)(
8
)3(
8
31
8
)3(
,)(
4
)3(
gives and for relations conditionboundary theSolving
0
28
)3(
0)(
0
28
)3(
0)(
28
31
28
)3(
22
max
22
max
2222222
max
222
2
22222
222
2
222
1
21
2
21
22
2
21
22
2
21
22
2
21
22

+
===

+


+
++
+
+
+
==

+
++
+
+
+
=

+
=+
+
=
=++
+
=
=++
+
=
+
+
=
++
+
=
abb
bab
bbaaa
ba
r
bar
baCbaC
CC
b
CC
bb
a
CC
aa
r
CC
r
r
CC
r
r
r
r
r
8.49.
)()(
11
)(
1
)(
1
:Law sHooke'
)(
1
:surface On the
)(
1
(8.5.4)1
xpp
E
p
E
p
EE
e
xp
Edx
ud
e
xp
Edx
ud
yxx
xyxx
x
x
x
==+=
+==
==
=
page-pfc
8.50.
% Calculate and Plot Stress Contours Under Surface Loading to a Half Space
% Numerically Evaluate Integrals Using quadv(....) Function in Eqn.(8.5.13)
% Elliptical Normal Loading Case: p(s)=(2P/pi*a)sqrt(1-(s/a)^2)
function elliptical

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