Ever J. Barbero, CRC, 2007, ISBN 1-4200-5433-3
Updated May 7, 2008
Note: In addition to corrections for typos, this file includes comments that attempt to clarify and enhance the existing content in the book as well as highlight new code and examples as they become available in the Website.
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Where it reads |
Correction, should read as follows … |
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32, Eq. (1.105) |
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Click or download this page to correct (1.105) |
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56, comment in 4th line of source code |
th = 2 mm |
th = 4 mm |
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56, comment in 5th line of source code |
E=200000 MPa |
E=190000 MPa |
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98, 3rd line Solution to Example 3.12 |
The second way uses FB … |
The second way uses TB … |
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147, fifth line after Eq.(6.18) |
Example 6.1 |
Example 6.2 |
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163, 1st line in Eq.(6.51) |
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181, 5th line after (7.67) |
"C' defined by (1.74)" |
"C' defined by (1.74, 1.93)" |
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192, footnote 2 |
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194, Eq.(8.11) |
>=0 |
<=0 |
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195, 1st Eq. in Ex. 8.1 |
>=0 |
<=0 |
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196, Eq.(8.16), upper limit of integral |
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196, Eq.(8.16), the integrand must use a dummy variable. |
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197, missing “/” |
threshold value |
threshold value |
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197, Eq.(8.19) |
>=0 |
<=0 |
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211, Eq. (8.64) |
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217, 1st Eq. in Ex. 8.4; insert a 2 in front of G12 |
G12 |
2 G12 |
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217, below 1st Eq. in Ex. 8.4 |
…are the in-plane… |
…are the undamaged in-plane… (Author’s note: I apologize for this departure from the notation used everywhere else in the book). |
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218, below 3rd Eq. |
…where the damage variables appear in S22 and S66. |
…where the damage variables appear in S12, S21,
S22, and S66. (Authors
note: Note that tensor strains |
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218, above the Eq. for M |
and where the effective damage tensor M in Voigt contracted notation is |
and the effective damage tensor M in Voigt contracted notation, multiplied by the 3x3 version of the Reuter matrix (A.13), is |
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219, 1st Eq. on this page; insert a 2 in front of G12 |
G12 |
2 G12 |
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219, 4 lines below Eq. (8.101) |
is possible by decreasing the value... |
is possible by increasing the value... |
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221, Eqs. (8.115), (8.116), (8.118), Substitute f for g |
g |
f |
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222, bottom |
5. Damage evolution exists. Starting at iteration k=k+1, |
5. Damage evolution exists. Starting at iteration k, |
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222, last eq. |
-(g)k |
-(g)k-1 |
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224, Caption of Table 8.2 |
8.2 Strength, critical energy |
8.2 Critical energy |
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224, 3rd eq. from bottom of page |
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224, last Eq., position 3,3; delete the “4” |
The following are written in contracted notation |
The following are written in contracted notation |
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225, two changes; positions 2,2 and 3,3 |
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227, below 1st Eq. in Problem. 8.3 |
…are the in-plane… |
…are the undamaged in-plane… |
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228 |
in Tables 8.4 and 8.4 |
in Tables 8.3 and 8.4 |
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233, Eq. (9.11) |
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Click or download this page to correct (9.11) |
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234, Eq. (9.18) |
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302, 2nd line after (A.19) |
= inverse of the reduced form of… |
= inverse of the contracted form of… |
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302, 3rd line after (A.19) |
= reduced form of… |
= contracted form of… |
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302, line above (A.20) |
In other words, the matrix [a]-1 is computed as |
In other words, the matrix [a-1] is computed as |
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311, Eq. (C.12) |
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Click or download this page to correct (C.12) |
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312, Eqs. (C.15, 16, 17, 18, 19) |
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Click or download this page to correct all those eqs. |
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313, Eq. (C.25) |
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Click or download this page to correct (C.25) |
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Please e-mail additional corrections to http://www.mae.wvu.edu/barbero/
Corrections have been made
thanks to the helpful contributions from:
·
Joan Andreu
Mayugo Majo,
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·
Norbert Blanco,
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Any Others??