coordinate system of the element face, the triangularregions have straightedges and lie in a single plane.. The domain of the projection of Fl onto the element face is divided into trian
Trang 1coordinate system of the element face, the triangularregions have straightedges and lie in a single plane The domain of the projection of Fl onto the element face is divided into triangularregions for the purpose of cal-culating surface integrals overFm.
19
Trang 2* -. \
Figure 3: An edge of F1 (solid line) and its projection onto the mastersurface (dashed line) viewed from a direction nearly orthogonal to F1 The edge shown spans three different element faces on the master surface The projection of the edge onto the master surface is a piecewise continuous line with possible discontinui-ties in slope at edges on the master surface The solid and dashed lines appear as straightlines in the coordi-nate systems of element faces on the slave and master surfaces, respectively
Trang 3k e2
el
Mesh 2 Mesh
(2hl,h2,0)
(o
(a)
(b)
Figure 4: (a) Mesh configuration H8T4 with nl 1= n21= n31= 2and FZ12= 7222= n32= 3, (b) openedviewof meshes revealing shared boundary
21
Trang 48
0.92465 0.76437
0.92385
0.92385 0.92385 0.76437 0.92465 7
6
1.1049
1.1049
1.1064
1.1064
1.1084
1.1064
0.92385
0.92385
1.1049
1.1049
m5
*
0.92385 4
3
2
0.92465 0.76437 0.92385 0.92385 0.76437 0.92465
1
1.104
Figure 7: Stress component G1, at centroids of elements with faces on the slave surface for Example 3.1 Results presented are for mesh configuration H20H20 using the standardmaster-slaveapproach
Trang 5BEl 0.527
0.514
0.511
0.505
log(lhz)
Figure 8: Energy norms of the error for Example 3.1 obtained using the standardmaster-slave approach Slopes of lines connecting the data points are shown above the line segments
25
Trang 6I I I I I I I
0.977 0.993
0.997
1.836
1.803
1.762
-11
log(lln)
Figure 9: Energy norms of the error for Example 3.2 obtained using the presentmethod Slopes of lines connecting the data points are shown above the line segments
Trang 7Figure 10: Energy norms of the error for Example 3.3 obtained using the present method
27
Trang 89
T ,
7
6
*N 5
Q
u
2
1
x3
Figure 11: Stress component olzat centroids ofelements with faces onthe slave surface forCasel of
Example 3.3
Trang 9I I I
:)
-rI
f? 5
4
I
2.0026e–07
I
I
x3
Figure 12: Stress componento12at centroidsofelements withfaces onthe slave surface forCase 2of Example 3.3
29
Trang 10Internal Distribution:
1 MS 9042
1 MS 9042
1 MS 9042
1 MS 9042
1 N’fs 9405
1 11S 9042
1 hfs 9405
1 lls 0828
1 llS 0826
1 hlS 0835
1 \fs o-143
1 \Iso4-i3
1 MS 0443
1 31S 0443
10 hfso443
10 hls 0443
1 hlso443
1 L1S0443
1 Lls 0443
1 hlS 0836
1 MS0836
1 JIS0819
1 MS0819
1 hlS0819
1 hls 0443
1 }1s0441
1 hIS0441
1 hlso439
10 MS0439
1 MS0439
1 MS0439
1 MS0439
1 MS9018
2 MS0899
1 MS0619
E P Chen, 8742
R E Jones, 8742
L E Voelker,8742
L I Weingarten, 8742
P E Nielan,8743
M L Chiesa,8743
J F Lathrop, 8743
F J Mello, 9104
D K Gartling, 9111
R J Cochran,9113
H S Morgan, 9117
S W Attaway, 9117
11 L Blanford,9117
K H Brown, 9117
lf W Heinstein, 9117
S W Key, 9117
J R Koteras,9117
J W Swegle, 9117
C M Stone, 9117
J R Stewart, 9121
L M Taylor, 9121
K G Budge, 9231
J S Peery,9231
J R Weatherby, 9231
J Jung, 9135
R W Leland, 9226
S A Mitchell, 9226
D R Martinez, 9234
C R Dohrmann, 9234
C W Fulcher, 9234
G M Reese, 9234
D J Segalman, 9234 Central Technical Files, 8940-2 Technical Library, 4916
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