Vasconcellos et al 2016a - Revision history

Scipediacontent: Scipediacontent moved page Draft Content 428379833 to Vasconcellos et al 2016a

2017-05-25T13:55:46Z

Scipediacontent moved page Draft Content 428379833 to Vasconcellos et al 2016a

Scipediacontent at 13:12, 25 May 2017

2017-05-25T13:12:15Z

Scipediacontent at 13:11, 25 May 2017

2017-05-25T13:11:14Z

Scipediacontent: Created page with "==Resumo== Um modelo numérico da equação de difusão unidimensional com fluxo bimodal em regime permanente e malhas uniformes foi desenvolvido utilizando‐se o método de..."

2017-05-25T13:02:42Z

Created page with "==Resumo== Um modelo numérico da equação de difusão unidimensional com fluxo bimodal em regime permanente e malhas uniformes foi desenvolvido utilizando‐se o método de..."

Show changes

@@ Line 628: / Line 628: @@
 {| style="text-align: center; margin:auto;"
 |-
-| <math>w_{i2}=w_{i1}\left(1+c_0\right)\frac{n\pi }{L}\mbox{\;  }\mbox{para}\mbox{\;  }i=</math><math>0,1</math>
+| <math>w_{i2}=w_{i1}\left(1+c_0\right)\frac{n\pi }{L};\mbox{para};i=</math><math>0,1</math>
 |}
 | style="width: 5px;text-align: right;white-space: nowrap;" | (39)
@@ Line 640: / Line 640: @@
 {| style="text-align: center; margin:auto;"
 |-
-| <math>e_{i2}=\left(1+c_0\right)\left[e_{i0}sen\left(n\pi \right)+\right. </math><math>\left. e_{i1}\frac{n\pi }{L}cos\left(n\pi \right)\right]\mbox{\;  }\mbox{para}\mbox{\;  }i=</math><math>0,1</math>
+| <math>e_{i2}=\left(1+c_0\right)\left[e_{i0}sen\left(n\pi \right)+\right. </math><math>\left. e_{i1}\frac{n\pi }{L}cos\left(n\pi \right)\right];\mbox{para};i=</math><math>0,1</math>
 |}
 | style="width: 5px;text-align: right;white-space: nowrap;" | (40)

@@ Line 217: / Line 217: @@
 {| style="text-align: center; margin:auto;"
 |-
-| <math>w_{10}{\phi }_{x=0}+{w_{11}\frac{d\phi }{dx}}_{x=0}=</math><math>w_{12}\mbox{\;  }\mbox{e}\mbox{\;  }w_{20}{\phi }_{x=0}+</math><math>{w_{21}\frac{d\phi }{dx}}_{x=0}=w_2</math>
+| <math>w_{10}{\phi }_{x=0}+{w_{11}\frac{d\phi }{dx}}_{x=0}=</math><math>w_{12};{ }\mbox{e};{ }w_{20}{\phi }_{x=0}+</math><math>{w_{21}\frac{d\phi }{dx}}_{x=0}=w_2</math>
 |}
 | style="width: 5px;text-align: right;white-space: nowrap;" | (13)
@@ Line 497: / Line 497: @@
+|
 {| style="text-align: center; margin:auto;"
-|-
+| <math>e_{10}{\phi }_{x=L}+{e_{11}\frac{d\phi }{dx}}_{x=L}=</math><math>|-e_{12};{ }\mbox{e};{ }e_{20}{\phi }_{x=L}+</math><math>{e_{21}\frac{d\phi }{dx}}_{x=L}=e_{22}</math>
-| <math>e_{10}{\phi }_{x=L}+{e_{11}\frac{d\phi }{dx}}_{x=L}=</math><math>e_{12}\mbox{\;  }\mbox{e}\mbox{\;  }e_{20}{\phi }_{x=L}+</math><math>{e_{21}\frac{d\phi }{dx}}_{x=L}=e_{22}</math>
 |}
 | style="width: 5px;text-align: right;white-space: nowrap;" | (30)

← Older revision	Revision as of 13:55, 25 May 2017
(No difference)