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2D Steady State Temperature Distribution Matrix Structural Analysis Giuliano Basile Vinh Nguyen Christine Rohr University of Massachusetts Dartmouth July 21, 2010 Introduction Advisor Dr. Nima Rahbar: Civil Engineer Project Description Learning the fundamentals for creating matrices. We will be working with 2 Dimensional frames. Constructing elements and nodes, which will be used to study temperature distribution through out our specimen. Application of Research Study the thermal distribution Test different types of materials Compare Numerical vs. Analytical results Basile, Nguyen, Rohr (UMD) Matrix Structural Analysis July 21, 2010 2 / 24 Objectives Use Matlab to calculate the 2D Steady State Temperature Distribution Consider the boundary conditions (will be discussed) Use Triangular Elements Compare your numerical solution with the exact analytical solution Calculate number of nodes, elements needed for accurate results Compute Errors Basile, Nguyen, Rohr (UMD) Matrix Structural Analysis July 21, 2010 3 / 24 Thermal Distribution in Materials We consider all materials to be at Steady State Different materials have different temperature distributions; This is due to different atomic structures Metals – Crystalline Ceramics – Amorphous Polymers – Chains Atomic structure leads to different Thermal Conductivity (how heat travels throughout) This knowledge can be to choose the correct material for engineering designs Basile, Nguyen, Rohr (UMD) Matrix Structural Analysis July 21, 2010 4 / 24 Metals Figure: Crystalline Atomic Structure Basile, Nguyen, Rohr (UMD) Matrix Structural Analysis July 21, 2010 5 / 24 Ceramics Figure: Amorphous Atomic Structure Basile, Nguyen, Rohr (UMD) Matrix Structural Analysis July 21, 2010 6 / 24 Polymers Figure: Chain Atomic Structure Basile, Nguyen, Rohr (UMD) Matrix Structural Analysis July 21, 2010 7 / 24 Thermal Distribution in Materials Table: Thermal Conductivity of Materials (Watts/meter*Kelvin) Basile, Nguyen, Rohr (UMD) Materials Values Wood Rubber Polypropylene Cement Glass Soil Steel Lead Aluminum Gold Silver Diamond 0.04-0.4 0.16 0.25 0.29 1.1 1.5 12.11-45.0 35.3 237.0 318.0 429.0 90.0-2320.0 Matrix Structural Analysis July 21, 2010 8 / 24 Why study 2D Thermal Distribution? To generate new understanding and improve computer methods for calculating thermal distribution. 2D computer modeling is cheap fast to process gives accurate numerical results parallel method can be used for higher efficiency Basile, Nguyen, Rohr (UMD) Matrix Structural Analysis July 21, 2010 9 / 24 Short Description Here we are modeling heat flux for a 2D plate No heat is applied to the x and y axis (x-nodes = y-nodes = 0) Flux is also considered zero on the right side of the plate Steady heat is being applied at the top of the plate: θ = 100 sin( πx ) 10 (1) ! Basile, Nguyen, Rohr (UMD) Matrix Structural Analysis July 21, 2010 10 / 24 What’s Included Elements We start with 32 triangular elements Numbering left to right; bottom to top Each element has 3 local and global nodes Number of Elements and Global Nodes will change Nodes Local nodes are used to indicate Global nodes Nodes are used to define elements Independent Element Number ien (3,5) = 17 3 is the Local node number 5 is the Element number 17 is the Global node number Basile, Nguyen, Rohr (UMD) Matrix Structural Analysis July 21, 2010 11 / 24 25 Nodes (32 Elements) — Plate vs. MatLab Solution Temperature Distribution 10 90 9 85 8 80 Vertical Side 7 75 6 70 5 65 4 60 3 55 2 50 1 45 0 0 1 2 3 4 Horizontal Side Basile, Nguyen, Rohr (UMD) 5 Matrix Structural Analysis July 21, 2010 12 / 24 81 Nodes (128 Elements) — Plate vs. MatLab Solution Temperature Distribution 10 9 90 8 Vertical side 7 85 6 5 80 4 75 3 2 70 1 0 0 1 2 3 4 Horizontal side Basile, Nguyen, Rohr (UMD) 5 Matrix Structural Analysis July 21, 2010 13 / 24 324 Nodes (512 Elements) — Plate vs. MatLab Solution Temperature Distribution 10 96 9 94 8 Vertical side 7 92 6 90 5 88 4 3 86 2 84 1 0 82 0 1 2 3 4 Horizontal side 5 Basile, Nguyen, Rohr (UMD) Matrix Structural Analysis July 21, 2010 14 / 24 900 Nodes (1682 Elements) — Plate vs. MatLab Solution Temperature Distribution 10 98 9 97 8 96 Vertical Side 7 95 6 5 94 4 93 3 92 2 91 1 90 0 0 1 2 3 4 Horizontal Side 5 Basile, Nguyen, Rohr (UMD) Matrix Structural Analysis July 21, 2010 15 / 24 Temperature Distribution (Right Side) 100 sinh πy 10 sin δ(x, y ) = sinh(π) πx 10 100 90 80 Temperature 70 60 32 Elements 50 40 30 20 10 0 0 1 Basile, Nguyen, Rohr (UMD) 2 3 4 5 Y!Axis 6 Matrix Structural Analysis 7 8 9 10 July 21, 2010 16 / 24 Temperature Distribution (Right Side) 100 sinh πy 10 sin δ(x, y ) = sinh(π) πx 10 100 90 80 Temperature 70 60 50 128 elements 40 30 32 elements 20 10 0 0 1 Basile, Nguyen, Rohr (UMD) 2 3 4 5 Y!Axis 6 Matrix Structural Analysis 7 8 9 10 July 21, 2010 17 / 24 Temperature Distribution (Right Side) 100 sinh πy 10 sin δ(x, y ) = sinh(π) πx 10 100 90 80 Temperature 70 128 elements 60 50 32 elements 40 30 512 elements 20 10 0 0 1 Basile, Nguyen, Rohr (UMD) 2 3 4 5 Y!Axis 6 Matrix Structural Analysis 7 8 9 10 July 21, 2010 18 / 24 Temperature Distribution (Right Side) 100 sinh πy 10 sin δ(x, y ) = sinh(π) πx 10 100 Temperature at The Right Side of The Plate 90 80 Temperature 70 60 50 The temperature lines converge to a smooth line as the number of elements increases 40 30 32 elements 128 elements 512 elements 1682 elements 20 10 0 0 1 Basile, Nguyen, Rohr (UMD) 2 3 4 5 Y!Axis 6 Matrix Structural Analysis 7 8 9 10 July 21, 2010 19 / 24 Maximum Error Computed 32 elements 7 128 elements 2 5 Percentage Error Percentage Error 6 4 3 2 1.5 1 0.5 1 0 0 1 2 3 4 0 5 0 1 2 X!axis 512 elements 0.45 3 4 5 4 5 X!axis 1682 elements 0.14 0.4 0.12 Percentage Error Percentage Error 0.35 0.3 0.25 0.2 0.15 0.1 0.08 0.06 0.04 0.1 0.02 0.05 0 0 1 2 3 4 5 0 0 X!axis Basile, Nguyen, Rohr (UMD) 1 2 3 X!axis Matrix Structural Analysis July 21, 2010 20 / 24 What’s Next??? Goals Continue modeling temperature change Add defect to material and relate it to original material Add hole to the specimen to be continued... Basile, Nguyen, Rohr (UMD) Matrix Structural Analysis July 21, 2010 21 / 24 References [Civil Engineer] Dr. Nima Rahbar Fundamental Matrix Algebra University of Massachusetts Dartmouth, Summer 2010. [Thermal Conductivity of some common Materials] Thermal Conductivity of Materials www. engineeringtoolbox. com , July 2010 Cu Atomic Structure Crystalline Atomic Structure http: // www. webelements. com , July 2010 Ceramic Atomic Structure Amorphous Atomic Structure http: // www. bccms. uni-bremen. de , July 2010 Polymer Atomic Structure Chain Atomic Structure http: // www. themolecularuniverse. com , July 2010 Thank You for Listening We would like to take this time to thank some very special people during this whole learning process. Dr. Gottlieb Dr. Davis Dr. Kim Dr. Rahbar Dr. Hausknecht CSUMS Staff Daniel Higgs Zachary Grant Charels Poole Sidafa Conde CSUMS Students Questions? ??????????????????????????????????????????????????????????????????? Basile, Nguyen, Rohr (UMD) Matrix Structural Analysis July 21, 2010 24 / 24