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Weak Boundary and Interface Procedures for Wave and Flow 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});
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2011 (English)Doctoral thesis, comprehensive summary (Other academic)
##### Abstract [en]

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

Uppsala: Acta Universitatis Upsaliensis , 2011. , p. 42
##### Series

Digital Comprehensive Summaries of Uppsala Dissertations from the Faculty of Science and Technology, ISSN 1651-6214 ; 862
##### Keywords [en]

weak boundary conditions, multiple penalty, finite difference methods, summation-by-parts, high order scheme, hybrid methods, MUSCL scheme, shocks, stability, energy estimate, steady-state, non-reflecting
##### National Category

Computational Mathematics
##### Research subject

Scientific Computing with specialization in Numerical Analysis
##### Identifiers

URN: urn:nbn:se:uu:diva-159440ISBN: 978-91-554-8176-6 (print)OAI: oai:DiVA.org:uu-159440DiVA, id: diva2:445243
##### Public defence

2011-11-07, Room 2446, Polacksbacken, Lägerhyddsvägen 2D, Uppsala, 10:15 (English)
##### Opponent

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##### Supervisors

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#####

PrimeFaces.cw("AccordionPanel","widget_formSmash_j_idt547",{id:"formSmash:j_idt547",widgetVar:"widget_formSmash_j_idt547",multiple:true}); Available from: 2011-10-14 Created: 2011-10-02 Last updated: 2011-11-09Bibliographically approved
##### List of papers

In this thesis, we have analyzed the accuracy and stability aspects of weak boundary and interface conditions (WBCs) for high order finite difference methods on Summations-By-Parts (SBP) form. The numerical technique has been applied to wave propagation and flow problems.

The advantage of WBCs over strong boundary conditions is that stability of the numerical scheme can be proven. The boundary procedures in the advection-diffusion equation for a boundary layer problem is analyzed. By performing Navier-Stokes calculations, it is shown that most of the conclusions from the model problem carries over to the fully nonlinear case.

The work was complemented to include the new idea of using WBCs on multiple grid points in a region, where the data is known, instead of at a single point. It was shown that we can achieve high accuracy, an increased rate of convergence to steady-state and non-reflecting boundary conditions by using this approach.

Using the SBP technique and WBCs, we have worked out how to construct conservative and energy stable hybrid schemes for shocks using two different approaches. In the first method, we combine a high order finite difference scheme with a second order MUSCL scheme. In the second method, a procedure to locally change the order of accuracy of the finite difference schemes is developed. The main purpose is to obtain a higher order accurate scheme in smooth regions and a low order non-oscillatory scheme in the vicinity of shocks.

Furthermore, we have analyzed the energy stability of the MUSCL scheme, by reformulating the scheme in the framework of SBP and artificial dissipation operators. It was found that many of the standard slope limiters in the MUSCL scheme do not lead to a negative semi-definite dissipation matrix, as required to get pointwise stability.

Finally, high order simulations of shock diffracting over a convex wall with two facets were performed. The numerical study is done for a range of Reynolds numbers. By monitoring the velocities at the solid wall, it was shown that the computations were resolved in the boundary layer. Schlieren images from the computational results were obtained which displayed new interesting flow features.

1. Weak versus strong no-slip boundary conditions for the Navier-Stokes equations$(function(){PrimeFaces.cw("OverlayPanel","overlay289286",{id:"formSmash:j_idt623:0:j_idt627",widgetVar:"overlay289286",target:"formSmash:j_idt623:0:partsLink",showEvent:"mousedown",hideEvent:"mousedown",showEffect:"blind",hideEffect:"fade",appendToBody:true});});

2. A weak boundary procedure for high order finite difference approximations of hyperbolic problems$(function(){PrimeFaces.cw("OverlayPanel","overlay444411",{id:"formSmash:j_idt623:1:j_idt627",widgetVar:"overlay444411",target:"formSmash:j_idt623:1:partsLink",showEvent:"mousedown",hideEvent:"mousedown",showEffect:"blind",hideEffect:"fade",appendToBody:true});});

3. Accurate and stable calculations involving shocks using a new hybrid scheme$(function(){PrimeFaces.cw("OverlayPanel","overlay275274",{id:"formSmash:j_idt623:2:j_idt627",widgetVar:"overlay275274",target:"formSmash:j_idt623:2:partsLink",showEvent:"mousedown",hideEvent:"mousedown",showEffect:"blind",hideEffect:"fade",appendToBody:true});});

4. A stable and conservative method for locally adapting the design order of finite difference schemes$(function(){PrimeFaces.cw("OverlayPanel","overlay371498",{id:"formSmash:j_idt623:3:j_idt627",widgetVar:"overlay371498",target:"formSmash:j_idt623:3:partsLink",showEvent:"mousedown",hideEvent:"mousedown",showEffect:"blind",hideEffect:"fade",appendToBody:true});});

5. Energy stability of the MUSCL scheme$(function(){PrimeFaces.cw("OverlayPanel","overlay359726",{id:"formSmash:j_idt623:4:j_idt627",widgetVar:"overlay359726",target:"formSmash:j_idt623:4:partsLink",showEvent:"mousedown",hideEvent:"mousedown",showEffect:"blind",hideEffect:"fade",appendToBody:true});});

6. The Effect of Reynolds Number in High Order Accurate Calculations with Shock Diffraction$(function(){PrimeFaces.cw("OverlayPanel","overlay291135",{id:"formSmash:j_idt623:5:j_idt627",widgetVar:"overlay291135",target:"formSmash:j_idt623:5:partsLink",showEvent:"mousedown",hideEvent:"mousedown",showEffect:"blind",hideEffect:"fade",appendToBody:true});});

isbn
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