CiteExport$(function(){PrimeFaces.cw("TieredMenu","widget_formSmash_upper_j_idt171",{id:"formSmash:upper:j_idt171",widgetVar:"widget_formSmash_upper_j_idt171",autoDisplay:true,overlay:true,my:"left top",at:"left bottom",trigger:"formSmash:upper:exportLink",triggerEvent:"click"});}); $(function(){PrimeFaces.cw("OverlayPanel","widget_formSmash_upper_j_idt172_j_idt174",{id:"formSmash:upper:j_idt172:j_idt174",widgetVar:"widget_formSmash_upper_j_idt172_j_idt174",target:"formSmash:upper:j_idt172:permLink",showEffect:"blind",hideEffect:"fade",my:"right top",at:"right bottom",showCloseIcon:true});});

Finite element methods for multiscale/multiphysics problemsPrimeFaces.cw("AccordionPanel","widget_formSmash_some",{id:"formSmash:some",widgetVar:"widget_formSmash_some",multiple:true}); PrimeFaces.cw("AccordionPanel","widget_formSmash_all",{id:"formSmash:all",widgetVar:"widget_formSmash_all",multiple:true});
function selectAll()
{
var panelSome = $(PrimeFaces.escapeClientId("formSmash:some"));
var panelAll = $(PrimeFaces.escapeClientId("formSmash:all"));
panelAll.toggle();
toggleList(panelSome.get(0).childNodes, panelAll);
toggleList(panelAll.get(0).childNodes, panelAll);
}
/*Toggling the list of authorPanel nodes according to the toggling of the closeable second panel */
function toggleList(childList, panel)
{
var panelWasOpen = (panel.get(0).style.display == 'none');
// console.log('panel was open ' + panelWasOpen);
for (var c = 0; c < childList.length; c++) {
if (childList[c].classList.contains('authorPanel')) {
clickNode(panelWasOpen, childList[c]);
}
}
}
/*nodes have styleClass ui-corner-top if they are expanded and ui-corner-all if they are collapsed */
function clickNode(collapse, child)
{
if (collapse && child.classList.contains('ui-corner-top')) {
// console.log('collapse');
child.click();
}
if (!collapse && child.classList.contains('ui-corner-all')) {
// console.log('expand');
child.click();
}
}
PrimeFaces.cw("AccordionPanel","widget_formSmash_responsibleOrgs",{id:"formSmash:responsibleOrgs",widgetVar:"widget_formSmash_responsibleOrgs",multiple:true}); 2011 (English)Doctoral thesis, comprehensive summary (Other academic)
##### Abstract [en]

##### Place, publisher, year, edition, pages

Umeå: Department of Mathematics and Mathematical Statistics, Umeå University , 2011. , 26 p.
##### Series

Doctoral thesis / Umeå University, Department of Mathematics, ISSN 1102-8300 ; 47
##### Keyword [en]

finite element methods, variational multiscale methods, Galerkin, convergence analysis, multiphysics, a posteriori error estimation, duality, adaptivity
##### National Category

Probability Theory and Statistics
##### Research subject

Mathematical Statistics
##### Identifiers

URN: urn:nbn:se:umu:diva-42713ISBN: 978-91-7459-193-4 (print)OAI: oai:DiVA.org:umu-42713DiVA: diva2:410033
##### Public defence

2011-05-05, MIT-huset, MA121, Umeå universitet, Umeå, 10:15 (English)
##### Opponent

PrimeFaces.cw("AccordionPanel","widget_formSmash_j_idt539",{id:"formSmash:j_idt539",widgetVar:"widget_formSmash_j_idt539",multiple:true});
##### Supervisors

PrimeFaces.cw("AccordionPanel","widget_formSmash_j_idt549",{id:"formSmash:j_idt549",widgetVar:"widget_formSmash_j_idt549",multiple:true});
#####

PrimeFaces.cw("AccordionPanel","widget_formSmash_j_idt555",{id:"formSmash:j_idt555",widgetVar:"widget_formSmash_j_idt555",multiple:true});
Available from: 2011-04-14 Created: 2011-04-12 Last updated: 2011-04-14Bibliographically approved
##### List of papers

In this thesis we focus on multiscale and multiphysics problems. We derive a posteriori error estimates for a one way coupled multiphysics problem, using the dual weighted residual method. Such estimates can be used to drive local mesh refinement in adaptive algorithms, in order to efficiently obtain good accuracy in a desired goal quantity, which we demonstrate numerically. Furthermore we prove existence and uniqueness of finite element solutions for a two way coupled multiphysics problem. The possibility of deriving dual weighted a posteriori error estimates for two way coupled problems is also addressed. For a two way coupled linear problem, we show numerically that unless the coupling of the equations is to strong the propagation of errors between the solvers goes to zero.

We also apply a variational multiscale method to both an elliptic and a hyperbolic problem that exhibits multiscale features. The method is based on numerical solutions of decoupled local fine scale problems on patches. For the elliptic problem we derive an a posteriori error estimate and use an adaptive algorithm to automatically tune the resolution and patch size of the local problems. For the hyperbolic problem we demonstrate the importance of how to construct the patches of the local problems, by numerically comparing the results obtained for symmetric and directed patches.

1. Adaptive finite element approximation of coupled flow and transport problems with applications in heat transfer$(function(){PrimeFaces.cw("OverlayPanel","overlay207459",{id:"formSmash:j_idt606:0:j_idt610",widgetVar:"overlay207459",target:"formSmash:j_idt606:0:partsLink",showEvent:"mousedown",hideEvent:"mousedown",showEffect:"blind",hideEffect:"fade",appendToBody:true});});

2. Convergence analysis of finite element approximations of the Joule heating problem in three spatial dimensions$(function(){PrimeFaces.cw("OverlayPanel","overlay410016",{id:"formSmash:j_idt606:1:j_idt610",widgetVar:"overlay410016",target:"formSmash:j_idt606:1:partsLink",showEvent:"mousedown",hideEvent:"mousedown",showEffect:"blind",hideEffect:"fade",appendToBody:true});});

3. $(function(){PrimeFaces.cw("OverlayPanel","overlay410030",{id:"formSmash:j_idt606:2:j_idt610",widgetVar:"overlay410030",target:"formSmash:j_idt606:2:partsLink",showEvent:"mousedown",hideEvent:"mousedown",showEffect:"blind",hideEffect:"fade",appendToBody:true});});

4. A variational multiscale method for poissons equation on mixed form$(function(){PrimeFaces.cw("OverlayPanel","overlay410020",{id:"formSmash:j_idt606:3:j_idt610",widgetVar:"overlay410020",target:"formSmash:j_idt606:3:partsLink",showEvent:"mousedown",hideEvent:"mousedown",showEffect:"blind",hideEffect:"fade",appendToBody:true});});

5. A discontinuous galerkin multiscale method for first order hyperbolic equations$(function(){PrimeFaces.cw("OverlayPanel","overlay410022",{id:"formSmash:j_idt606:4:j_idt610",widgetVar:"overlay410022",target:"formSmash:j_idt606:4:partsLink",showEvent:"mousedown",hideEvent:"mousedown",showEffect:"blind",hideEffect:"fade",appendToBody:true});});

isbn
urn-nbn$(function(){PrimeFaces.cw("Tooltip","widget_formSmash_j_idt1400",{id:"formSmash:j_idt1400",widgetVar:"widget_formSmash_j_idt1400",showEffect:"fade",hideEffect:"fade",showDelay:500,hideDelay:300,target:"formSmash:altmetricDiv"});});

CiteExport$(function(){PrimeFaces.cw("TieredMenu","widget_formSmash_lower_j_idt1457",{id:"formSmash:lower:j_idt1457",widgetVar:"widget_formSmash_lower_j_idt1457",autoDisplay:true,overlay:true,my:"left top",at:"left bottom",trigger:"formSmash:lower:exportLink",triggerEvent:"click"});}); $(function(){PrimeFaces.cw("OverlayPanel","widget_formSmash_lower_j_idt1458_j_idt1460",{id:"formSmash:lower:j_idt1458:j_idt1460",widgetVar:"widget_formSmash_lower_j_idt1458_j_idt1460",target:"formSmash:lower:j_idt1458:permLink",showEffect:"blind",hideEffect:"fade",my:"right top",at:"right bottom",showCloseIcon:true});});