Heat and Thermal Energy Transfer

Heat and Thermal Energy Transfer
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Exploring the principles of heat transfer and thermal energy in Chapter 9, covering states of matter, conduction, convection, radiation, and insulators. Learn about different types of heat transfer methods and materials' thermal properties.

  • Heat transfer
  • Thermal energy
  • Conduction
  • Convection
  • Radiation

Uploaded on Mar 05, 2025 | 1 Views


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  1. CS 219: Sparse Matrix Algorithms John R. Gilbert (gilbert@cs.ucsb.edu) home page: www.cs.ucsb.edu/~gilbert/cs219

  2. Systems of linear equations: Ax = b Eigenvalues and eigenvectors: Aw = w

  3. Systems of linear equations: Ax = b Alice is four years older than Bob. In three years, Alice will be twice Bob s age. How old are Alice and Bob now?

  4. Poisson s equation for temperature

  5. Example: The Temperature Problem A cabin in the snow Wall temperature is 0 , except for a radiator at 100 What is the temperature in the interior?

  6. Example: The Temperature Problem A cabin in the snow (a square region ) Wall temperature is 0 , except for a radiator at 100 What is the temperature in the interior?

  7. The physics: Poissons equation

  8. Many Physical Models Use Stencil Computations PDE models of heat, fluids, structures, Weather, airplanes, bridges, bones, Game of Life many, many others 6.43

  9. From Stencil Graph to System of Linear Equations Solve Ax = b for x Matrix A, right-hand side vector b, unknown vector x A is sparse: most of the entries are 0

  10. The (2-dimensional) model problem n1/2 Graph is a regular square grid with n = k^2 vertices. Corresponds to matrix for regular 2D finite difference mesh. Gives good intuition for behavior of sparse matrix algorithms on many 2-dimensional physical problems. There s also a 3-dimensional model problem.

  11. Solving Poisson s equation for temperature k = n1/3 For each i from 1 to n, except on the boundaries: x(i-k2) x(i-k) x(i-1) + 6*x(i) x(i+1) x(i+k) x(i+k2) = 0 n equations in n unknowns: A*x = b Each row of A has at most 7 nonzeros.

  12. Spectral graph clustering

  13. Definitions The Laplacian matrix of an n-vertex undirected graph G is the n-by-n symmetric matrix A with aij = -1 if i j and (i, j) is an edge of G aij = 0 if i j and (i, j) is not an edge of G aii = the number of edges incident on vertex i Theorem: The Laplacian matrix of G is symmetric, singular, and positive semidefinite. The multiplicity of 0 as an eigenvalue is equal to the number of connected components of G. A generalized Laplacian matrix (more accurately, a symmetric weakly diagonally dominant M-matrix) is an n-by-n symmetric matrix A with aij 0 if i j aii |aij| where the sum is over j i

  14. Administrivia Course web site: www.cs.ucsb.edu/~gilbert/cs219 Be sure you re on the Piazza class discussion list. First homework is on the web site, due next Monday About 5 weekly homeworks, then a final project (implementation experiment, application, or survey paper) Assigned readings: Davis book, Saad book, Multigrid Tutorial

  15. Course Outline Sparse direct (Gaussian elimination) methods Sparse iterative and preconditioned methods Multigrid methods Sparse eigenvalue/eigenvector methods Solvers for graph Laplacians Graph algorithms in the language of linear algebra

  16. The Landscape of Sparse Ax=b Solvers Direct A = LU Iterative y = Ay More General Non- Pivoting LU GMRES, QMR, symmetric Symmetric positive definite Cholesky Conjugate gradient More Robust More Robust Less Storage D

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