CS 290H 7 November Introduction to multigrid methods - PowerPoint PPT Presentation

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CS 290H 7 November Introduction to multigrid methods

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Restricts problem on fine grid P(i) to coarse grid P(i-1) Uses sampling or averaging. Right-hand sided is also restricted: b(i-1)= R(i) (b(i) ... – PowerPoint PPT presentation

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Title: CS 290H 7 November Introduction to multigrid methods


1
CS 290H 7 NovemberIntroduction to multigrid
methods
  • Homework 3 will be on the web page by the end of
    today
  • Talk to me by Wednesday about your final project
  • Read Saad 2nd edition (library reserve) 13.1
    13.5, skimming 13.2.1-13.2.3
  • See web page for other multigrid references
  • Multigrid intuition and overview (slides thanks
    to Kathy Yelick)
  • The model problem revisited
  • Stationary iterative methods (rest of slides
    thanks to Bill Briggs et al.)
  • Smoothing
  • Nested iteration
  • Coarse-grid correction
  • Prolongation and restriction
  • The multigrid V-cycle

2
Complexity of linear solvers
Time to solve model problem (Poissons equation)
on regular mesh
3
Multigrid (introduction)
  • Find an approximate solution on a coarser mesh
    and then improve it on a finer mesh
  • Use idea recursively on hierarchy of meshes
  • Solves the model problem (Poissons eqn) in
    linear time!
  • Often useful when hierarchy of meshes can be
    built
  • Hard to parallelize coarse meshes well
  • This is just the intuition lots of theory and
    technology

4
Multigrid Overview
  • Basic Algorithm
  • Replace problem on fine grid by an approximation
    on a coarser grid
  • Solve the coarse grid problem approximately, and
    use the solution as a starting guess for the
    fine-grid problem, which is then iteratively
    updated
  • Solve the coarse grid problem recursively, i.e.
    by using a still coarser grid approximation, etc.
  • Success depends on coarse grid solution being a
    good approximation to the fine grid

5
Multigrid Sketch on a Regular 1D Mesh
  • Consider a 2m1 grid in 1D for simplicity
  • Let P(i) be the problem of solving the discrete
    Poisson equation on a 2i1 grid in 1D
  • Write linear system as T(i) x(i) b(i)
  • P(m) , P(m-1) , , P(1) is a sequence of
    problems from finest to coarsest

6
Multigrid Sketch on a Regular 2D Mesh
  • Consider a 2m1 by 2m1 grid
  • Let P(i) be the problem of solving the discrete
    Poisson equation on a 2i1 by 2i1 grid in 2D
  • Write linear system as T(i) x(i) b(i)
  • P(m) , P(m-1) , , P(1) is a sequence of
    problems from finest to coarsest

7
Multigrid Operators
  • For problem P(i)
  • b(i) is the RHS and
  • x(i) is the current estimated solution
  • (T(i) is implicit in the operators below.)
  • Multigrid will be defined by a repeated sequence
    of operators
  • The multigrid operators average values on
    neighboring grid points
  • Neighboring grid points on coarse problems are
    far away in fine problems, so information moves
    quickly on coarse problems
  • Levels will be constructed explicitly
  • The next slide gives an overview of the
    operators details will come later

both live on grids of size 2i-1
8
Multigrid Operators
  • For problem P(i)
  • b(i) is the RHS and
  • x(i) is the current estimated solution
  • The restriction operator R(i) maps P(i) to P(i-1)
  • Restricts problem on fine grid P(i) to coarse
    grid P(i-1)
  • Uses sampling or averaging
  • Right-hand sided is also restricted b(i-1) R(i)
    (b(i))
  • The interpolation operator In(i-1) maps solution
    x(i-1) to x(i)
  • Maps one approximate solution to another
  • Interpolates solution on coarse grid P(i-1) to
    fine grid P(i)
  • x(i) In(i-1)(x(i-1))
  • The smoothing operator S(i) takes P(i) and
    improves solution x(i)
  • Uses weighted Jacobi or SOR on a single level
    of the grid
  • x improved (i) S(i) (b(i), x(i))

both live on grids of size 2i-1
9
Multigrid V-Cycle Algorithm
  • Function MGV ( b(i), x(i) )
  • Solve T(i)x(i) b(i) given b(i) and an
    initial guess for x(i)
  • return an improved x(i)
  • if (i 1)
  • compute exact solution x(1) of P(1)
    only 1 unknown
  • return x(1)
  • else
  • x(i) S(i) (b(i), x(i))
    improve solution by

  • damping high frequency
    error
  • r(i) T(i)x(i) - b(i)
    compute residual
  • d(i) In(i-1) ( MGV( R(i) ( r(i) ), 0 )
    ) solve T(i)d(i) r(i) recursively
  • x(i) x(i) - d(i)
    correct fine grid solution
  • x(i) S(i) ( b(i), x(i) )
    improve solution again
  • return x(i)

10
Why is this called a V-Cycle?
  • Just a picture of the call graph
  • In time a V-cycle looks like the following

11
Complexity of a V-Cycle on a 2D Grid
  • Work at each point in a V-cycle is O( of
    unknowns)
  • Cost of Level i is (2i-1)2 O(4 i)
  • If finest grid level is m, total time is
  • S O(4 i) O(4m) O(
    unknowns)

m i1
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