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CSE 245: Computer Aided Circuit Simulation and Verification

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CSE 245: Computer Aided Circuit Simulation and Verification

Fall 2004, Oct 19

Lecture 7:

Matrix Solver II

-Iterative Method

- Iterative Method
- Stationary Iterative Method (SOR, GS,Jacob)
- Krylov Method (CG, GMRES)
- Multigrid Method

Zhengyong (Simon) Zhu, UCSD

Stationary:

x(k+1)=Gx(k)+c

where G and c do not depend on iteration count (k)

Non Stationary:

x(k+1)=x(k)+akp(k)

where computation involves information that change at each iteration

courtesy Alessandra Nardi, UCB

In the i-th equation solve for the value of xi while assuming the other entries of x remain fixed:

In matrix terms the method becomes:

where D, -L and -U represent the diagonal, the strictly lower-trg and strictly upper-trg parts of M

M=D-L-U

courtesy Alessandra Nardi, UCB

Like Jacobi, but now assume that previously computed results are used as soon as they are available:

In matrix terms the method becomes:

where D, -L and -U represent the diagonal, the strictly lower-trg and strictly upper-trg parts of M

M=D-L-U

courtesy Alessandra Nardi, UCB

Devised by extrapolation applied to Gauss-Seidel in the form of weighted average:

In matrix terms the method becomes:

where D, -L and -U represent the diagonal, the strictly lower-trg and strictly upper-trg parts of M

M=D-L-U

courtesy Alessandra Nardi, UCB

- Choose w to accelerate the convergence
- W =1 : Jacobi / Gauss-Seidel
- 2>W>1: Over-Relaxation
- W < 1: Under-Relaxation

Zhengyong (Simon) Zhu, UCSD

- Linear Equation: MX=b
- A sufficient condition for convergence of the solution(GS,Jacob) is that the matrix M is diagonally dominant.
- If M is symmetric positive definite, SOR converges for any w (0<w<2)
- A necessary and sufficient condition for the convergence is the magnitude of the largest eigenvalue of the matrix G is smaller than 1
- Jacobi:
- Gauss-Seidel
- SOR:

Zhengyong (Simon) Zhu, UCSD

- Iterative Method
- Stationary Iterative Method (SOR, GS,Jacob)
- Krylov Method (CG, GMRES)
- Steepest Descent
- Conjugate Gradient
- Preconditioning

- Multigrid Method

Zhengyong (Simon) Zhu, UCSD

- Quadratic function of vector x
- Matrix A is positive-definite, if for any nonzero vector x
- If A is symmetric, positive-definite, f(x) is minimized by the solution

Zhengyong (Simon) Zhu, UCSD

- Quadratic function
- Derivative
- If A is symmetric
- If A is positive-definite
is minimized by setting to 0

Zhengyong (Simon) Zhu, UCSD

from J. R. Shewchuk "painless CG"

The points in the direction of steepest increase of f(x)

from J. R. Shewchuk "painless CG"

Symmetric Positive-Definite Matrix A

- If A is symmetric positive definite
- P is the arbitrary point
- X is the solution point

since

We have,

If p != x

Zhengyong (Simon) Zhu, UCSD

- Positive definite matrix b) negative-definite matrix
- c) Singular matrix d) positive indefinite matrix

from J. R. Shewchuk "painless CG"

- State from initial guess x0, adjust it until close enough to the exact solution
- How to choose direction and step size?

i=0,1,2,3,……

Adjustment Direction

Step Size

Zhengyong (Simon) Zhu, UCSD

- Choose the direction in which f decrease most quickly: the direction opposite of
- Which is also the direction of residue

Zhengyong (Simon) Zhu, UCSD

- How to choose step size ?
- Line Search
should minimize f, along the direction of , which means

- Line Search

Orthogonal

Zhengyong (Simon) Zhu, UCSD

Given x0, iterate until residue is smaller than error tolerance

Zhengyong (Simon) Zhu, UCSD

- Starting at (-2,-2) take the
- direction of steepest descent of f
- b) Find the point on the intersec-
- tion of these two surfaces that
- minimize f
- c) Intersection of surfaces.
- d) The gradient at the bottommost
- point is orthogonal to the gradient
- of the previous step

from J. R. Shewchuk "painless CG"

from J. R. Shewchuk "painless CG"

let

Eigenvector:

EigenValue:

j=1,2,…,n

Energy norm:

Zhengyong (Simon) Zhu, UCSD

Zhengyong (Simon) Zhu, UCSD

assume

let

Spectral condition number

let

Zhengyong (Simon) Zhu, UCSD

from J. R. Shewchuk "painless CG"

from J. R. Shewchuk "painless CG"

It can be proved that it is

also valid for n>2, where

from J. R. Shewchuk "painless CG"

- Steepest Descent
- Repeat search direction

- Why take exact one step for each direction?

Search direction of Steepest

descent method

figure from J. R. Shewchuk "painless CG"

Pick orthogonal search direction:

- We don’t know !!!

Zhengyong (Simon) Zhu, UCSD

- Instead of orthogonal search direction, we make search direction A –orthogonal (conjugate)

from J. R. Shewchuk "painless CG"

Zhengyong (Simon) Zhu, UCSD

Initial error:

A-orthogonal

The error component at direction dj

is eliminated at step j. After n steps,

all errors are eliminated.

Zhengyong (Simon) Zhu, UCSD

- How to construct A-orthogonal search directions, given a set of n linear independent vectors.
- Since the residue vector in steepest descent method is orthogonal, a good candidate to start with

Zhengyong (Simon) Zhu, UCSD

- In Steepest Descent Method
- New residue is just a linear combination of previous residue and

- Let

We have

Krylov SubSpace: repeatedly applying a matrix to a vector

Zhengyong (Simon) Zhu, UCSD

let

For i > 0

Zhengyong (Simon) Zhu, UCSD

- can get next direction from the previous one, without saving them all.

let

then

Zhengyong (Simon) Zhu, UCSD

Given x0, iterate until residue is smaller than error tolerance

Zhengyong (Simon) Zhu, UCSD

- In exact arithmetic, CG converges in n steps (completely unrealistic!!)
- Accuracy after k steps of CG is related to:
- consider polynomials of degree k that are equal to 1 at 0.
- how small can such a polynomial be at all the eigenvalues of A?

- Thus, eigenvalues close together are good.
- Condition number:κ(A) = ||A||2 ||A-1||2 = λmax(A) / λmin(A)
- Residual is reduced by a constant factor by O(κ1/2(A)) iterations of CG.

courtesy J.R.Gilbert, UCSB

- Nonsymmetric linear systems:
- GMRES: for i = 1, 2, 3, . . . find xi Ki (A, b) such that ri = (Axi– b) Ki (A, b)But, no short recurrence => save old vectors => lots more space (Usually “restarted” every k iterations to use less space.)
- BiCGStab, QMR, etc.:Two spaces Ki (A, b)and Ki (AT, b)w/ mutually orthogonal bases Short recurrences => O(n) space, but less robust
- Convergence and preconditioning more delicate than CG
- Active area of current research

- Eigenvalues: Lanczos (symmetric), Arnoldi (nonsymmetric)

courtesy J.R.Gilbert, UCSB

- Suppose you had a matrix B such that:
- condition number κ(B-1A) is small
- By = z is easy to solve

- Then you could solve (B-1A)x = B-1b instead of Ax = b
- B = A is great for (1), not for (2)
- B = I is great for (2), not for (1)
- Domain-specific approximations sometimes work
- B = diagonal of A sometimes works
- Better: blend in some direct-methods ideas. . .

courtesy J.R.Gilbert, UCSB

- One matrix-vector multiplication per iteration
- One solve with preconditioner per iteration

x0 = 0, r0 = b, d0 = B-1r0, y0 = B-1r0

for k = 1, 2, 3, . . .

αk = (yTk-1rk-1) / (dTk-1Adk-1) step length

xk = xk-1 + αk dk-1 approx solution

rk = rk-1 – αk Adk-1 residual

yk = B-1rk preconditioning solve

βk = (yTk rk) / (yTk-1rk-1) improvement

dk = yk + βk dk-1 search direction

courtesy J.R.Gilbert, UCSB

- Iterative Method
- Stationary Iterative Method (SOR, GS,Jacob)
- Krylov Method (CG, GMRES)
- Multigrid Method

Zhengyong (Simon) Zhu, UCSD

- A multilevel iterative method to solve
- Ax=b

- Originated in PDEs on geometric grids
- Expend the multigrid idea to unstructured problem – Algebraic MG
- Geometric multigrid for presenting the basic ideas of the multigrid method.

Zhengyong (Simon) Zhu, UCSD

v3

v4

v1

v2

v5

v6

v8

v7

+

vs

Ax = b

Zhengyong (Simon) Zhu, UCSD

- x(0) -> x(1) -> … -> x(k)
- Jacobi iteration
- Matrix form : x(k) = Rjx(k-1) + Cj
- General form: x(k) = Rx(k-1) + C (1)
- Stationary: x* = Rx* + C (2)

Zhengyong (Simon) Zhu, UCSD

Definition: errore = x* - x (3)

residualr = b – Ax (4)

e, r relation: Ae = r (5) ((3)+(4))

e(1) = x*-x(1) = Rx* + C – Rx(0)– C =Re(0)

Error equatione(k) = Rke(0) (6) ((1)+(2)+(3))

Convergence:

Zhengyong (Simon) Zhu, UCSD

k= 1

k= 4

k= 2

- Wavenumber k and frequency
- = k/n
- High frequency error is more oscillatory between points

Zhengyong (Simon) Zhu, UCSD

- Smoothing iteration reduce high frequency error efficiently, but not low frequency error

Error

k = 1

k = 2

k = 4

Iterations

Zhengyong (Simon) Zhu, UCSD

2

1

3

4

3

4

1

2

5

6

8

7

- Two levels : coarse and fine grid

2h

A2hx2h=b2h

h

Ahxh=bh

Ax=b

Zhengyong (Simon) Zhu, UCSD

- Also called the nested iteration

Start with

2h

A2hx2h = b2h

A2hx2h = b2h

Iterate =>

Prolongation:

Restriction:

h

Ahxh = bh

Iterate to get

Question 1: Why we need the coarse grid ?

Zhengyong (Simon) Zhu, UCSD

2

1

3

4

3

4

1

2

5

6

8

7

- Prolongation (interpolation) operator
xh = x2h

Zhengyong (Simon) Zhu, UCSD

2

1

3

4

3

4

1

2

5

6

8

7

- Restriction operator
xh = x2h

Zhengyong (Simon) Zhu, UCSD

- The basic iterations in each level
In ph: xphold xphnew

- Iteration reduces the error, makes the error smooth geometrically.
So the iteration is called smoothing.

Zhengyong (Simon) Zhu, UCSD

- Coarse lever iteration is cheap.
- More than this…
- Coarse level smoothing reduces the error more efficiently than fine level in some way .
- Why ? ( Question 2 )

Zhengyong (Simon) Zhu, UCSD

- Map error to coarse grid will make the error more oscillatory

K = 4, =

K = 4, = /2

Zhengyong (Simon) Zhu, UCSD

- Known current solution x
- Solve Ax=b eq. to
- MG do NOT map x directly between levels
Map residual equation to coarse level

- Calculate rh
- b2h= Ih2h rh ( Restriction )
- eh =Ih2hx2h ( Prolongation )
- xh = xh + eh

Zhengyong (Simon) Zhu, UCSD

- Error is smooth at fine level, but the actual solution may not be.
- Prolongation results in a smooth error in fine level, which is suppose to be a good evaluation of the fine level error.
- If the solution is not smooth in fine level, prolongation will introduce more high frequency error.

Zhengyong (Simon) Zhu, UCSD

- Smoothing on xh
- Calculate rh
- b2h= Ih2h rh
- Smoothing on x2h
- eh =Ih2hx2h
- Correct: xh = xh + eh

2h h

`

Restriction

Prolongation

Zhengyong (Simon) Zhu, UCSD

- Galerkin condition

Zhengyong (Simon) Zhu, UCSD

- V-cycle and W-cycle
- Full Multigrid V-cycle

h

2h

4h

h

2h

4h

8h

Zhengyong (Simon) Zhu, UCSD

- Complexity comparison

Zhengyong (Simon) Zhu, UCSD

Three important ideas of MG

- Nested iteration
- Residual correction
- Elimination of error:
high frequency : fine grid

low frequency : coarse grid

Zhengyong (Simon) Zhu, UCSD

1

2

4

3

5

6

- Ax=b, no regular grid structure
- Fine grid defined from A

Zhengyong (Simon) Zhu, UCSD

- How to choose coarse grid
- How to define the smoothness of errors
- How are interpolation and prolongation done

Zhengyong (Simon) Zhu, UCSD

- Idea:
- C/F splitting
- As few coarse grid point as possible
- For each F-node, at least one of its neighbor is a C-node
- Choose node with strong coupling to other nodes as C-node

1

2

4

3

5

6

Zhengyong (Simon) Zhu, UCSD

- AMG fundamental concept:
Smooth error = small residuals

- ||r|| << ||e||

Zhengyong (Simon) Zhu, UCSD

- Prolongation is based on smooth error and strong connections
- Common practice: I

Zhengyong (Simon) Zhu, UCSD

Zhengyong (Simon) Zhu, UCSD

- Restriction :

Zhengyong (Simon) Zhu, UCSD

- Multigrid is a multilevel iterative method.
- Advantage: scalable
- If no geometrical grid is available, try Algebraic multigrid method

Zhengyong (Simon) Zhu, UCSD

Direct

A = LU

Iterative

y’ = Ay

More General

Non-

symmetric

Symmetric

positive

definite

More Robust

More Robust

Less Storage (if sparse)

courtesy J.R.Gilbert, UCSB