Download presentation

Presentation is loading. Please wait.

Published byAiyana Moyes Modified about 1 year ago

1
Computational Physics Linear Algebra Dr. Guy Tel-Zur Sunset in Caruaru by Jaime JaimeJunior. publicdomainpictures.netVersion , 14:00

2
MHJ Chapter 4 – Linear Algebra In this talk we deal with basic matrix operations Such as the solution of linear equations, calculate the inverse of a matrix, its determinant etc. Here we focus in particular on so-called direct or elimination methods, which are in principle determined through a finite number of arithmetic operations. Iterative methods will be discussed in connection with eigenvalue problems in MHJ chapter 12. This chapter serves also the purpose of introducing important programming details such as handling memory allocation for matrices and the usage of the libraries which follow these lectures.

3
Libraries LAPACK based on: – EISPACK – for solving symmetric, un-symmetric and generalized eigenvalue problems – LINPACK - linear equations and least square problems BLAS: Basic Linear Algebra Subprogram – Levels I, II and III Nelib:

4
LAPACK - Linear Algebra PACKage LAPACK is written in Fortran90 and provides routines for solving systems of simultaneous linear equations, least-squares solutions of linear systems of equations, eigenvalue problems, and singular value problems. The associated matrix factorizations (LU, Cholesky, QR, SVD…) are also provided. Dense and banded matrices are handled, but not general sparse matrices. In all areas, similar functionality is provided for real and complex matrices, in both single and double precision.

5
EISPACK EISPACK is a collection of Fortran subroutines that compute the eigenvalues and eigenvectors of nine classes of matrices: complex general, complex Hermitian, real general, real symmetric, real symmetric banded, real symmetric tridiagonal, special real tridiagonal, generalized real, and generalized real symmetric matices. In addition, two routines are included that use singular value decomposition to solve certain least-squares problems.

6
LINPACK LINPACK is a collection of Fortran subroutines that analyze and solve linear equations and linear least- squares problems. The package solves linear systems whose matrices are general, banded, symmetric indefinite, symmetric positive definite, triangular, and tridiagonal square. In addition, the package computes the QR and singular value decompositions of rectangular matrices and applies them to least-squares problems. LINPACK uses column-oriented algorithms to increase efficiency by preserving locality of reference.

7
LINPACK and EISPACK are based on BLAS I LAPACK is based on BLAS III

8
BLAS The BLAS (Basic Linear Algebra Subprograms) are routines that provide standard building blocks for performing basic vector and matrix operations. The Level 1 BLAS perform scalar, vector and vector- vector operations. The Level 2 BLAS perform matrix-vector operations The Level 3 BLAS perform matrix-matrix operations. Because the BLAS are efficient, portable, and widely available, they are commonly used in the development of high quality linear algebra software, LAPACK for example.LAPACK

9
LAPACK / CLAPACK / ScaLAPACK for Windows

10
Working with a Linear Algebra package using Visual Studio Demo Work dir: C:\Users\telzur\Documents\BGU\Teaching\ComputationalPhysics\2011A\Lectures\04\LAPACK\CLAPACK-EXAMPLE\Release>

11
Compare with the following MATLAB code clear all close all disp('solves Ax=b') A= [76, 27, 18; 25, 89, 60; 11, 51, 32] b=[10, 7, 43] invA=inv(A) x=b*inv(A) [L,U]=lu(A) inv(U)*inv(L)*b' clear all close all disp('solves Ax=b') A= [76, 27, 18; 25, 89, 60; 11, 51, 32] b=[10, 7, 43] invA=inv(A) x=b*inv(A) [L,U]=lu(A) inv(U)*inv(L)*b' Code location: C:\Users\telzur\Documents\BGU\Teaching\ComputationalPhysics\2011A\Lectures\04\lpack.m Demo

12
DGESV SUBROUTINE DGESV( N, NRHS, A, LDA, IPIV, B, LDB, INFO ) * * -- LAPACK driver routine (version 3.2) -- * -- LAPACK is a software package provided by Univ. of Tennessee, -- * -- Univ. of California Berkeley, Univ. of Colorado Denver and NAG Ltd..-- * November 2006 * *.. Scalar Arguments.. INTEGER INFO, LDA, LDB, N, NRHS *.. *.. Array Arguments.. INTEGER IPIV( * ) DOUBLE PRECISION A( LDA, * ), B( LDB, * ) *.. * * Purpose * ======= * * DGESV computes the solution to a real system of linear equations * A * X = B, * where A is an N-by-N matrix and X and B are N-by-NRHS matrices. * * The LU decomposition with partial pivoting and row interchanges is * used to factor A as * A = P * L * U, * where P is a permutation matrix, L is unit lower triangular, and U is * upper triangular. The factored form of A is then used to solve the * system of equations A * X = B. *

13
* Arguments * ========= * * N (input) INTEGER * The number of linear equations, i.e., the order of the * matrix A. N >= 0. * * NRHS (input) INTEGER * The number of right hand sides, i.e., the number of columns * of the matrix B. NRHS >= 0. * * A (input/output) DOUBLE PRECISION array, dimension (LDA,N) * On entry, the N-by-N coefficient matrix A. * On exit, the factors L and U from the factorization * A = P*L*U; the unit diagonal elements of L are not stored. * * LDA (input) INTEGER * The leading dimension of the array A. LDA >= max(1,N). * * IPIV (output) INTEGER array, dimension (N) * The pivot indices that define the permutation matrix P; * row i of the matrix was interchanged with row IPIV(i). * * B (input/output) DOUBLE PRECISION array, dimension (LDB,NRHS) * On entry, the N-by-NRHS matrix of right hand side matrix B. * On exit, if INFO = 0, the N-by-NRHS solution matrix X. * * LDB (input) INTEGER * The leading dimension of the array B. LDB >= max(1,N). * * INFO (output) INTEGER * = 0: successful exit * < 0: if INFO = -i, the i-th argument had an illegal value * > 0: if INFO = i, U(i,i) is exactly zero. The factorization * has been completed, but the factor U is exactly * singular, so the solution could not be computed. * * ===================================================================== * Cont’

14
*.. External Subroutines.. EXTERNAL DGETRF, DGETRS, XERBLA *.. *.. Intrinsic Functions.. INTRINSIC MAX *.. *.. Executable Statements.. * * Test the input parameters. * INFO = 0 IF( N.LT.0 ) THEN INFO = -1 ELSE IF( NRHS.LT.0 ) THEN INFO = -2 ELSE IF( LDA.LT.MAX( 1, N ) ) THEN INFO = -4 ELSE IF( LDB.LT.MAX( 1, N ) ) THEN INFO = -7 END IF IF( INFO.NE.0 ) THEN CALL XERBLA( 'DGESV ', -INFO ) RETURN END IF * * Compute the LU factorization of A. * CALL DGETRF( N, N, A, LDA, IPIV, INFO ) IF( INFO.EQ.0 ) THEN * * Solve the system A*X = B, overwriting B with X. * CALL DGETRS( 'No transpose', N, NRHS, A, LDA, IPIV, B, LDB, $ INFO ) END IF RETURN * * End of DGESV * END Cont’

15
Mathematicalintermezzo Mathematical intermezzo

16
science-and-engineering-i-fall-2008/

17
The K n Matrices The next slides are from: Computational Science and Engineering, by Gilbert Strang. An excellent recommended book. His course is available online from MIT Opencourseware. Very Recommended!!!! What are the properties of K ?

18
K n Properties 1.These matrices are symmetric. 2.The matrices Kn are sparse. 3.These matrices are tridiagonal. 4.The matrices have constant diagonals. 5.All the matrices K = Kn are invertible. 6.The symmetric matrices Kn are positive definite. Source: Computational Science and Engineering, by Gilbert Strang

19
In Signal Processing D=Kn/4 is a “High-Pass” Filter. Du picks out the rapidly varying parts of a vector u K are called Toeplitz Matrix and MATLAB has a function for generating such matrices, e.g. K = toeplitz([2 -1 zeros(l,2)]) constructs K4 from row 1 Source: Computational Science and Engineering, by Gilbert Strang

20
More properties (Pivots) An invertible matrix has n nonzero pivots. A positive definite symmetric matrix has n positive pivots. (Eigenvalues) An invertible matrix has n nonzero eigenvalues. A positive definite symmetric matrix has n positive eigenvalues. Source: Computational Science and Engineering, by Gilbert Strang

21
More special matrices T=Top, B=Bottom Source: Computational Science and Engineering, by Gilbert Strang

22
Building K,T,B,C in Matlab Source: Computational Science and Engineering, by Gilbert Strang Make a demo also using Octave Demo

23
Matlab Demos K4=toeplitz([ ]) C4=toeplitz([ ]) inv(K4) …OK inv(C4) …not OK singular eig(K4) positive >0 positive definite eig(C4) >=0 semi positive definite Both are symmetric: try transpose(K4) Check: [L,U]=lu(T4) all pivots are 1 [L,U]=lu(B4) 0 on the diagonal of U B isn’t invertibe inv(T4) …OK inv(B4) …not OK singular Demo

24
demos e=ones(8,1) B.e=0. = dot product B T =transpose(B) B is symmetric System to solve: Bu=f u T B T =f T B T. e=B.e=0 Thefore f T.e=0 Demo

25
Continued det(K8) = Π(diagonal of U) = 2/1 * 3/2 * 4/3 … * 9/8 = 9 Demo

26
For large size n THIS IS THE CODE TO CREATE K,T,B,C AS SPARSE MATRICES Then Matlab will not operate on all the zeros! function K=SKTBC(type,n,sparse) % SKTBC Create finite difference model matrix. % K=SKTBC(TYPE,N,SPARSE) creates model matrix TYPE of size N-by-N. % TYPE is one of the characters 'K', 'T', 'B', or 'C'. % The command K = SKTBC('K', 100, 1) gives a sparse representation % K=SKTBC uses the defaults TYPE='K', N=10, and SPARSE=false. % Change the 3rd argument from 1 to 0 for dense representation! % If no 3rd argument is given, the default is dense % If no argument at all, KTBC will give 10 by 10 matrix K if nargin<1, type='K'; end if nargin<2, n=10; end e=ones(n,1); K=spdiags([-e,2*e,-e],-1:1,n,n); switch type case 'K' case 'T' K(1,1)=1; case 'B' K(1,1)=1; K(n,n)=1; case 'C' K(1,n)=-1; K(n,1)=-1; otherwise error('Unknown matrix type.'); end if nargin<3 | ~sparse K=full(K); end Demo

27

28

29
Source: Numerical recipes in FORTRAN77: the art of scientific computing, page 65. By William H. Press

30
In Mathematics: Vectors and Matrices Are mapped to Computers as Memory arrays Fixed Memory allocation vs. Dynamic Memory Allocation Compile time vs. Run time In the next slides we will study two programs that demonstrate these issues In Mathematics: Vectors and Matrices Are mapped to Computers as Memory arrays Fixed Memory allocation vs. Dynamic Memory Allocation Compile time vs. Run time In the next slides we will study two programs that demonstrate these issues Let’s start with Table 4.2 in the book: Matrix handling program where arrays are defined at compilation time – Next slide Use Visual Studio for the demo solution file under: chap4_static Let’s start with Table 4.2 in the book: Matrix handling program where arrays are defined at compilation time – Next slide Use Visual Studio for the demo solution file under: chap4_static

31
int main() { int k,m, row = 3, col = 5; int vec[5]; // line a: a standard C++ declaration of a vector int matr[3][5]; // line b: a standard fixed-size C++ declaration of a matrix for(k = 0; k < col; k++) vec[k] = k; // data into vector[] for(m = 0; < row; m++) { // data into matr[][] for(k = 0; k < col ; k++) matr[m][k] = m + 10 * k; } printf("\n Vector data in main():\n”); // print vector data for(k = 0; k < col; k++) printf("vetor[%d]= %d ",k, vec[k]); printf("\n Matrix data in main():"); for(m = 0; m < row; m++) { printf(“\n”); for(k = 0; k < col; k++) printf("m atr[%d][%d]= %d ",m,k,matr[m][k]); } // הקוד שכתוב בספר קצת רשלני. לא ניתן להעתיק אותו אחד לאחד printf(“\n”); sub_1(row, col, vec, matr); // line c: transfer vec[] and matr[][] addresses to func. sub_1(). return 0; } // End: function main() void sub_1(int row, int col, int vec[], int matr[][5]) { //line d: a func. def. int k,m; printf("\n Vetor data in sub1():\n"); // print vector data for(k = 0; k < col; k++) printf("vetor[%d]= %d ",k, vec[k]); printf("\n Matrix data in sub1():"); for(m = 0; m < row; m++) { printf(“\n”); for(k = 0; k < col; k++) { printf("matr[%d][%d]= %d ",m, k, matr[m][k]); } printf(“\n”); } // End: function sub_1() equiv to int *vec equiv to int (*matr)[5] Table 4.2 Demo

32
Using Visual Studio 2010 Make demo in class

33
Static program execution

34
Table 4.3: Matrix handling program with dynamic array allocation. התכנית ב 4.3 לא מתקמפלת ומלאה באגים. בעתיד היא תתווסף כתכנית לדוגמה. בשלב הזה נתייחס אליה כאל פסאודו - קוד מבלי להריצה התכנית ב 4.3 לא מתקמפלת ומלאה באגים. בעתיד היא תתווסף כתכנית לדוגמה. בשלב הזה נתייחס אליה כאל פסאודו - קוד מבלי להריצה

35
we declare a pointer to an integer declares a pointer-to-a- pointer which will contain the address to a pointer of row vectors, each with col integers read in the size of vec[] and matr[][] through the numbers row and col we reserve memory for the vector #include int main() { int *vec; // line a int **matr; // line b int m, k, row, col, total = 0; printf("\n Read in number of rows= "); // line c scanf("%d",&row); printf("\n Read in number of column= "); scanf("%d", &col); vec = new int [col]; // line d matr = (int **)matrix(row, col, sizeof(int)); // line e for(k = 0; k < col; k++) vec[k] = k; // store data in vector[] for(m = 0; < row; m++) { // store data in array[][] for(k = 0; k < col; k++) matr[m][k] = m + 10 * k; } printf("\n Vetor data in main():\n"); // print vector data for(k = 0; k < col; k++) printf("vetor[%d]= %d ",k,vec[k]); printf("\n Array data in main():"); for(m = 0; m < row; m++) { printf("\n"); for(k = 0; k < col; k++) { printf("m atrix[%d][%d]= %d ",m, k, matr[m][k]); } printf("\n"); for(m = 0; m < row; m++) { // access the array for(k = 0; k < col; k++) total += matr[m][k]; } printf("\n Total= %d\n",total); sub_1(row, col, vec, matr); free_matrix((void **)matr); // line f delete [] vec; // line g return 0; } // End: function main() we use a user-defined function to reserve necessary memory for matrix[row][col] and again matr contains the address to the reserved memory location. The remaining part of the function main() are as in the previous case down to line f. the same procedure is performed for vec[]

36
void sub_1(int row, int col, int vec[], int ??matr) // line h { int k,m; printf("\n Vetor data in sub1():\n"); // print vector data for(k = 0; k < col; k++) printf("vetor[%d]= %d ",k, vec[k]); printf("\n Matrix data in sub1():"); for(m = 0; m < row; m++) { printf("\n"); for(k = 0; k < col; k++) { printf("matrix[%d][%d]= %d ",m,k,matr[m][k]); } printf("\n"); } // End: function sub_1() Continued from previous slide in line h an important difference from the previous case occurs. First, the vector declaration is the same, but the matr declaration is quite different. The corresponding parameter in the call to sub_1[] in line g is a double pointer. Consequently, matr in line h must be a double pointer

37
lib.cpp /* * The function * void **matrix( ) * reserves dynamic memory for a two-dimensional matrix * using the C++ command new. No initialization of the elements. * Input data : * int row - number of rows * int col - number of columns * int num_bytes - number of bytes for each element * Returns avoid **pointer to the reserved memory location. */ void **matrix( int row, int col, int num_bytes ) { int i, num; char **pointer, *ptr; pointer = new(nothrow) char* [ row ] ; if ( !pointer ) { cout << "Exeption handling Memory aloation failed"; cout << "for"<< row << "row addresses!"<< endl; return NULL; } i = ( row * col * num_bytes ) / size of ( char ) ; pointer [ 0 ] = new( nothrow ) char [ i ] ; if ( !pointer [ 0 ] ) { cout << "Exeption handling :Memory allocation failed"; cout << "for address to " << i << " characters!"<< endl ; return NULL; } ptr = pointer [ 0 ] ; num = col * num_bytes ; for ( i = 0 ; i < row ; i ++, ptr += num ) { pointer [ i ] = ptr ; } return ( void **) pointer ; } // end : function void **matrix ( )

38
Skip to section 4.4

39
C++ and Fortran features of matrix handling If we store a matrix in the sequence a11 a12... a1n a21 a22... a2n... ann This is called “row-major” order (we go along a given row i and pick up all column elements j) C++ stores them by row-major. We cloud also store in column-major order a11 a21... an1 a12 a22... an2... ann. Fortran stores matrices by column-major,

40
4.4 Linear Systems Gauss Elimination Upper/Lower triangular matrix Solve Linear System LU algorithm Cholesky decomposition (a special case)

41
(4.4) Linear Systems: An Example

42
…And we switched from a Differential Equation to Linear Algebra. This is the stiffness matrix, K, we met earlier!

43
Case #1: Assume first that the function f does not depend on u(x). Then our linear equation reduces to Au = f, (4.8) which is nothing but a simple linear equation with a tridiagonal matrix A. We will solve such a system of equations in subsection Case #1: Assume first that the function f does not depend on u(x). Then our linear equation reduces to Au = f, (4.8) which is nothing but a simple linear equation with a tridiagonal matrix A. We will solve such a system of equations in subsection

44
Case #2 If we assume that our boundary value problem is that of a quantum mechanical particle confined by a harmonic oscillator potential, then our function f takes the form (assuming that all constants m = h_bar = omega = 1 with λ being the eigenvalue. Inserting this into our equation, we define first a new matrix A as להבנה נוספת ראש השקף הבא

45

46
We will solve this type of equations in chapter 12.

47
(4.4.2) LU Decomposition LU Factorization Continue from page 83 at MHJ chap 4 PDF

48
Cholesky’s Factorization MHJ Chapter 4, page 87 (2009 edition) One has to check first if A is positive definite!

49

50

51
Vandermonde matrix MHJ Chap. 4, page 93

52
QR Decomposition is a decomposition of the matrix into an orthogonal and an upper triangular matrix.

53
singular value decomposition SVD M=UΣV* Matlab demo: M=[ ; ; ; ] [U S V]=svd(M) M=UΣV* Matlab demo: M=[ ; ; ; ] [U S V]=svd(M)

Similar presentations

© 2016 SlidePlayer.com Inc.

All rights reserved.

Ads by Google