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Linear Equations

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Linear Equations



PSCI 702

September 21, 2005

Numerical Errors

• Round off Error









• Truncation Error

Linear Algebraic Equations

a11 x1  a12 x2  a13 x3  ... a1n xn  c1

a21 x1  a22 x1  a23 x3  ... a2 n xn  c2

a31 x1  a32 x1  a33 x3  ... a3n xn  c3

    

an1 x1  an 2 x2  an 3 x3  ... ann xn  cn





 a11 a12 a13  a1n   x1   c1 

a a22 a23  a2 n   x2  c 2 

 21    

 a31 a32 a33  a3n   x3   c 3 

    

           

an1

 an 2 an 3  ann   xn   cn 

   

Linear Algebraic Equations

• In Matrix Format

 

Ax  c

• Solution:



1 1   1

A Ax  A c  x  A c

Cramer’s Rule

• Mij is the determinant of the Matrix A with

the ith row and jth column removed.

• (-1)ij is called the cofactor of element aij.

n

Det A   (1) aij M ij , j

i j



i 1

n n

Det A   C ij aij , j   aij C ij , i

i 1 i j

Cramer’s Rule

a11 a12 a13  a1n a11x1 a12 a13  a1n

a21 a22 a23  a2 n a21x1 a22 a23  a2 n

x1 a31 a32 a33  a3n  a31x1 a32 a33  a3n 

         

an1 an 2 an3  ann an1x1 an 2 an3  ann

a11 x1  a12 x2  a13 x3  ... a1n xn a12  a1n c1 a12 a13  a1n

a21 x1  a22 x1  a23 x3  ... a2 n xn a22  a2 n c2 a22 a23  a2 n

a31 x1  a32 x1  a33 x3  ... a3n xn a32  a3n  c3 a32 a33  a3n

         

an1 x1  an 2 x2  an3 x3  ... ann xn an 2  ann cn an 2 an3  ann

Cramer’s Rule

c1 a12 a13  a1n a11  a1 j 1 c1 a1 j 1  a1n

c2 a22 a23  a2 n a21  a2 j 1 c2 a2 j 1  a2 n

c3 a32 a33  a3n a31  a3 j 1 c3 a3 j 1  a3n

       

cn an 2 an 3  ann an1  anj 1 cn an j 1  ann

x1  ,xj 

a11 a12 a13  a1n a11 a12 a13  a1n

a21 a22 a23  a2 n a21 a22 a23  a2 n

a31 a32 a33  a3n a31 a32 a33  a3n

         

an1 an 2 an3  ann an1 an 2 an 3  ann

Cramer’s Rule

• 3n2 operations for the determinant.

• 3n3 operations for every unknown.

• Unstable for large Matrices.

• Large error propagation.

• Good for small Matrices (n<20).

Gaussian Elimination

• Divide each row by the leading element.

• Subtract row 1 from all other rows.

• Move to the second row an continue the

process.

 a11 a12 a13  a1n   c1 

a a22 a23  a2 n  c 2 

 21  

a31 a32 a33  a3n  c 3 

  

        

an1 an 2 an 3  ann  cn 

  

Gaussian Elimination



 a11 a12 a13 a11   c1 

a   a 

a11 a11 a11

 11   11 

        

 a31 a32 a33 a3n   c3 

 

 a31 a31 a31 a31   a31 

        

a an 2 an 3 ann   cn 

 n1

  

 an1

 an1 an1 an1   an1 

 

Gaussian Elimination



 a12 a13 a11   c1 

1   a 

a11 a11 a11

  11



       

0 a32 a12 a33 a13 a3n a11   c3 c1 

    

 a31 a11 a31 a11 a31 a11   a31 a11 

       

 an 2 a12 an 3 a13 ann a11   cn c1 

0       



 an1 a11 an1 a11 an1 a11   an1 a11 

 

Gaussian Elimination



1 a12 a13  a1n   c1 

 

0 1

 a23  a2 n  c2 

 

 

0 0 1  a3n  c3 



  

       

0 0

 0  1   cn 

  

• Back substitution



x n  cn

n

x i  ci   a x

j i 1

ij j

Gaussian Elimination





• Division by zero: May occur in the forward

elimination steps.





• Round-off error: Prone to round-off errors.

Gaussian Elimination

Consider the system of equations:

Use five significant figures with chopping



 10  7 0  x1   7 

 3 2.099 6   

   x2  = 3.901



5

  1 5  x3   6 

    



At the end of Forward Elimination

10 7 0   x1   7 

 0  0.001 6   x  =  6.001 

   2  

0

 0 15005

  x3  15004

   

Gaussian Elimination

Back Substitution

15004

x3   0.99993

7 15005

10 0   x1   7 

 0  0.001 6   x 2    6.001

     6.001  6 x3

0 15005  x3  15004 x2   1.5

 0      0.001



7  7 x 2  0 x3

x1   0.3500

10

Gaussian Elimination



Compare the calculated values with the exact solution

 x1   0 

X  exact  x    1

  2  

 x3   1 

   

 x1    0.35 

X  calculated   x 2     1.5 

   

 x3  0.99993

   

Improvements



Increase the number of significant digits

Decreases round off error



Does not avoid division by zero





Gaussian Elimination with Partial Pivoting

Avoids division by zero



Reduces round off error

Partial Pivoting



Gaussian Elimination with partial pivoting applies row switching to

normal Gaussian Elimination.

How?

At the beginning of the kth step of forward elimination, find the maximum of



.......,ank

akk , ak 1,k ,.........

If the maximum of the values is a pk In the pth row, k  p  n,

then switch rows p and k.

Partial Pivoting



What does it Mean?





Gaussian Elimination with Partial Pivoting ensures that

each step of Forward Elimination is performed with the

pivoting element |akk| having the largest absolute value.

Partial Pivoting: Example

Consider the system of equations



10x1  7 x 2  7

 3x1  2.099x 2  3x 3  3.901

5x 1  x 2  5x 3  6

In matrix form

 10 7 0  x1   7 

 3 2.099 6  x  3.901

   2 =  

5

  1 5  x3 

   6 

 

Solve using Gaussian Elimination with Partial Pivoting using five

significant digits with chopping

Partial Pivoting: Example

Forward Elimination: Step 1

Examining the values of the first column

|10|, |-3|, and |5| or 10, 3, and 5

The largest absolute value is 10, which means, to follow the

rules of Partial Pivoting, we switch row1 with row1.





Performing Forward Elimination



 10 7 0  x1   7  10 7 0  x1   7 

 3 2.099 6  x   3.901



5



 2  

 1 5  x3   6 

  





  0  0.001 6  x   6.001



0

 2.5

 2  

5  x3   2.5 

  





Partial Pivoting: Example

Forward Elimination: Step 2

Examining the values of the first column

|-0.001| and |2.5| or 0.0001 and 2.5

The largest absolute value is 2.5, so row 2 is switched with

row 3





Performing the row swap



10 7 0  x1   7  10 7 0  x1   7 

 0  0.001 6  x   6.001



0

 2  

5  x3   2.5 

  0

 2.5 5  x2    2.5 

  

 0  0.001 6  x3  6.001



 2.5         

Partial Pivoting: Example

Forward Elimination: Step 2





Performing the Forward Elimination results in:





10  7 0   x1   7 

 0 2.5 5   x 2    2.5 

    

0

 0 6.002  x3  6.002

   

Partial Pivoting: Example

Back Substitution

Solving the equations through back substitution



10  7

6.002

0   x1   7  x3  1

 0 2.5 5   x 2    2.5  6.002

    

0

 0 6.002  x3  6.002

    2.5  5 x 2

x2  1

2.5



7  7 x 2  0 x3

x1  0

10

Partial Pivoting: Example

Compare the calculated and exact solution

The fact that they are equal is coincidence, but it does

illustrate the advantage of Partial Pivoting







 x1   0   x1   0 

X  calculated   x2    1

    X  exact   x 2    1

   

 x3   1 

     x3   1 

   

Gauss Jordan Elimination

• Start with the following system of Matrices.

 a11 a12 a13  a1n   c1  1 0 0  0

a a22 a23  a2 n  c 2  0 1 0  0

 21   

a31 a32 a33  a3n  c 3  0 0 1  0

   

            

an1

 an 2 an 3  ann  cn  0

  0 0  1



• Divide each row by the leading element.

• Subtract row 1 from all other rows.

• In addition to subtracting the line whose diagonal

term has been made unity from all those bellow it,

also subtract from the equations above it as well.

Gauss Jordan Elimination



a11 0 0  0   c1  b11 b12 b13  b1n 

 0 a 0  0  c2  b21 b22 b23  b2 n 

 22   

0 0 a33   0  c3  b31 b32 b33  b3n 

   

             

0

 0 0  ann   cn  bn1

    bn 2 bn 3  bnn 



 x1   c1 

 x  c 

 2  2

 x3   c3 

   

   

 xn   cn 

   

Matrix Factorization

• Assume A can be written as A=VU where V

and U are triangular Matrices.





 a11 a12 a13  a1n   v11 0 0  0  u11 u12 u13  u1n 

a  a2 n  v21 v22  0   0 u22  u2 n 

 21 a22 a23   0  u23 

a31 a32 a33  a3n   v31 v32 v33  0  0 0 u33  u3 n 

    

                  

an1 an 2

 an 3  ann  vn1 vn 2

  vn 3  vnn   0

 0 0  unn 

Matrix Factorization

Proof

If solving a set of linear equations AX   C 

If A  V U  Then V U X   C 

Multiply by V 1

Which gives V 1 V U X   V 1 C 

Remember V  V   I  which leads to I U X   V 1 C 

1







Now, if I U   U  then U X   V 1 C 

Now, let V 1C   Z 

Which ends with V Z  C  (1)

and U X  Z  (2)

Matrix Factorization



How can this be used?

GivenAX   C 

Decompose A into V  and U 



Then solve VZ  C  for Z 



And then solve U X  Z  for X 

Matrix Factorization

How is this better or faster than Gauss

Elimination?

Let’s look at computational time.

n = number of equations

n3

To decompose [A], time is proportional to

3





To solve U X   C  and V Z   C 

n2

time is proportional to

2

Matrix Factorization

Therefore, total computational time for LU Decomposition is

proportional to 3 2

n3

n n

 2( ) or  n2

3 2 3



Gauss Elimination computation time is proportional to

3 2

n n



3 2





How is this better?

Matrix Factorization

What about a situation where the [C] vector changes?

In VU factorization, VU decomposition of [A] is independent of

the [C] vector, therefore it only needs to be done once.

Let m = the number of times the [C] vector changes

The computational times are proportional to



n3 n2 n3

VU factorization = m(  ) Gauss Elimination=  m( n 2 )

3 2 3



Consider a 100 equation set with 50 right hand side vectors

VU factorization = 8.33105 Gauss Elimination = 1.69 107

Matrix Factorization

Another Advantage



Finding the Inverse of a Matrix



VU Factorization Gauss Elimination



n3

4n 3  n3 n2  n4 n3

 n( n ) 

2

n   

 3  3  2

3 3  2



For large values of n

4 3 3

n n 4n

 

3 2 3

Matrix Factorization

Method: Decompose [A] to [V] and [U]



1 0 0 u11 u12 u13 

A  V  U   v21 1

 0  0 u22

 u23 



v31 v32

 1  0

 0 u33 



[U] is the same as the coefficient matrix at the end of the forward

elimination step.

[V] is obtained using the multipliers that were used in the forward

elimination process

Matrix Factorization

Finding the [U] matrix

Using the Forward Elimination Procedure of Gauss Elimination

 25 5 1

 64 8 1

 

144 12 1

 

 25 5 1 

 Row1

Row 2    (64)   0  4.8  1.56

 25   

144 12

 1  

25 5 1 

 Row1

Row 3    (144)   0  4.8  1.56 

 25   

 0  16.8  4.76

 

Matrix Factorization

Finding the [U] matrix

Using the Forward Elimination Procedure of Gauss Elimination





25 5 1  25 5 1 

 0  4.8  1.56   Row 2 

Row 3    (16.8)   0  4.8  1.56

    4.8 

  

 0  16.8  4.76

  0

 0 0.7 



25 5 1 

 0  4.8  1.56

U    

0

 0 0. 7 



Matrix Factorization

Finding the [V] matrix

Using the multipliers used during the Forward Elimination Procedure

a 21 64

From the first step 1 0 0 v21    2.56

of forward v 0

a11 25

elimination

 21 1 

v31 v32

 1

 a 31 144

v31    5.76

a 11 25





From the second 25 5 1 

step of forward  0  4.8  1.56  a 32  16 .8

  v32    3 .5

elimination  0  16.8  4.76

 

a 22  4.8

Matrix Factorization

 1 0 0

V   2.56 1 0

 

5.76 3.5 1

 



Does V U   A ?







 1 0 0 25 5 1 

V U   2.56 1 0  0  4.8  1.56 

  

5.76 3.5 1  0

  0 0.7 

Matrix Factorization

Example: Solving simultaneous linear equations using VU factorization



Solve the following set of  25 5 1  a 1  106.8 

linear equations using VU  64 8 1 a   177.2 

   2  

Factorization 144 12 1 a 3  279.2

    



Using the procedure for finding the [V] and [U] matrices



 1 0 0 25 5 1 

A  V U   2.56 1 0  0  4.8  1.56

  

5.76 3.5 1  0

  0 0.7 

Matrix Factorization

Example: Solving simultaneous linear equations using VU factorization



Complete the forward substitution to solve for Z 



z1  106.8

z 2  177.2  2.56 z1

 177.2  2.56(106.8)  z1   106.8 

 96.2  z    96.21

Z    2  

z 3  279.2  5.76 z1  3.5 z 2 

 279.2  5.76(106.8)  3.5(96.21)  z3   0.735 

   

 0.735

Matrix Factorization

Example: Solving simultaneous linear equations using VU factorization



Set U X   Z  25 5 1   a1   106.8 

 0  4.8  1.56 a   - 96.21

   2  

0

 0 0.7   a3   0.735 

   



The 3 equations become

Solve for X  25a1  5a 2  a3  106.8

 4.8a 2  1.56a3  96.21

0.7a3  0.735

Matrix Factorization

Example: Solving simultaneous linear equations using VU factorization



From the 3rd equation Substituting in a3 and using the

second equation

0.7a3  0.735

 4.8a 2  1.56a3  96.21

0.735

a3   96.21  1.56a3

0.7 a2 

 4.8

 1.050 - 96.21 1.561.050



- 4.8

 19.70

Matrix Factorization

Example: Solving simultaneous linear equations using VU factorization



Substituting in a3 and a2 Hence the Solution Vector is:

using the first equation



25a1  5a2  a3  106.8  a1  0.2900

a1 

106.8  5a 2  a 3 a    19.70 

25  2  

106.8  519.70  1.050  a3   1.050 

   



25

 0.2900

Gauss Method



An iterative method.



Basic Procedure:

-Algebraically solve each linear equation for xi

-Assume an initial guess solution array

-Solve for each xi and repeat

-Use absolute relative approximate error after each iteration

to check if error is within a prespecified tolerance.

Gauss Method



Why?

The Gauss Method allows the user to control round-off error.





Elimination methods such as Gaussian Elimination and VU

Factorization are prone to round-off error.





Also: If the physics of the problem is understood, a close initial

guess can be made, decreasing the number of iterations needed.

Gauss Method

Algorithm

A set of n equations and n unknowns:

If: the diagonal elements are

a11 x1  a12 x2  a13 x3  ...  a1n xn  b1 non-zero

a21 x1  a22 x2  a23 x3  ...  a2n xn  b2 Rewrite each equation solving

. .

. . for the corresponding unknown

. .

ex:

an1 x1  an 2 x2  an 3 x3  ...  ann xn  bn

First equation, solve for x1

Second equation, solve for x2

Gauss Method

Algorithm

Rewriting each equation

c  a12 x 2  a13 x3   a1n x n From Equation 1

x1  1

a11



c2  a21 x1  a23 x3   a2 n xn

x2  From equation 2

a22

  

cn 1  an 1,1 x1  an 1, 2 x2   an 1,n  2 xn  2  an 1,n xn From equation n-1

xn 1 

an 1,n 1

cn  an1 x1  an 2 x2    an ,n 1 xn 1 From equation n

xn 

ann

Gauss Method

Algorithm

General Form of each equation

n



a

n

c1   a1 j x j cn 1  n 1, j xj

j 1 j 1

j  n 1

x1 

j 1 xn 1 

a11 an 1,n 1

n

c n   a nj x j

n

c2   a2 j x j

j 1 j 1

j n

x2 

j 2

xn 

a 22 a nn

Gauss Method

Gauss Algorithm

General Form for any row ‘i’



n

ci   aij x ( k 1) j

j 1

j i

x(k )i  , i  1,2,, n.

aii





How or where can this equation be used?

Gauss Method

Solve for the unknowns



Assume an initial guess for [X] Use rewritten equations to solve for

each value of xi.



 x1  Important: Remember to use the

most recent value of xi. Which

x  means to apply values calculated to

 2 the calculations remaining in the

   current iteration.

 

 xn -1 

 xn 

 

Gauss Method

Calculate the Absolute Relative Approximate Error

x inew  x iold

a i

 new

100

xi



So when has the answer been found?



The iterations are stopped when the absolute relative

approximate error is less than a pre-specified tolerance for all

unknowns.

Gauss-Seidel Method



• Improved method



i 1 n

ci   aij x j a x

( k 1)



(k )

ij j

j 1 j i 1



(k )

xi

aii

Gauss-Seidel Method: Pitfall

Diagonally dominant: The coefficient on the diagonal must be at least

equal to the sum of the other coefficients in that row and at least one row

with a diagonal coefficient greater than the sum of the other coefficients

in that row.

Which coefficient matrix is diagonally dominant?



 2 5.81 34 124 34 56 

A   45 43 1  [B]   23 53 5 

 

 

123 16 1  96 34 129

 

 





Most physical systems do result in simultaneous linear equations that

have diagonally dominant coefficient matrices.

Gauss-Seidel Method: Example



Given the system of equations The coefficient matrix is:

12x 1  3x 2 - 5x 3  1

x 1  5x 2  3x 3  28 12 3  5



3x1  7x2  13x3  76

A   1 5 3 

 

 3 7 13 

 

With an initial guess of

Will the solution converge using the

 x1  1

Gauss-Seidel method?

 x   0 

 2  

 x 3  1 

   

Gauss-Seidel Method: Example

Checking if the coefficient matrix is diagonally dominant



a11  12  12  a12  a13  3   5  8

12 3  5

A   1 5 3  a22  5  5  a21  a23  1  3  4

 

 3 7 13 

  a33  13  13  a31  a32  3  7  10





The inequalities are all true and at least one row is strictly greater than:

Therefore: The solution should converge using the Gauss-Seidel Method

Gauss-Siedel Method: Example



Rewriting each equation With an initial guess of

12 3  5  a1   1   x1  1

 1 5 3  a   28  x   0 

   2    2  

 3 7 13   a3  76

      x 3  1 

   



1  3 x 2  5 x3 1  30  51

x1  x1   0.50000

12 12

28  x1  3x3 28  0.5  31

x2  x2   4.9000

5 5

76  3x1  7 x2

x3  76  30.50000  74.9000

13 x3   3.0923

13

Gauss-Siedel Method: Example

The absolute relative approximate error



0.50000  1.0000

a 1  100  67 .662 %

0.50000



4.9000  0

a 2

 100  100 .00 %

4.9000



3.0923  1.0000

a 3

 100  67 .662 %

3.0923



The maximum absolute relative error after the first iteration is 100%

Gauss-Siedel Method: Example

After Iteration #1

 x1  0.5000

 x   4.9000

 2  

 x3  3.0923

   

Substituting the x values into the equations After Iteration #2

1  34.9000  53.0923  x1  0.14679

x1   0.14679  x    3.7153 

12  2  

 x3   3.8118 

   

28  0.14679  33.0923

x2   3.7153

5



76  30.14679  74.900

x3   3.8118

13

Gauss-Siedel Method: Example

Iteration #2 absolute relative approximate error

0.14679  0.50000

a 1  100  240 .62 %

0.14679



3.7153  4.9000

a 2  100  31 .887 %

3.7153

3.8118  3.0923

a 3  100  18 .876 %

3.8118



The maximum absolute relative error after the first iteration is 240.62%





This is much larger than the maximum absolute relative error obtained in

iteration #1. Is this a problem?

Gauss-Siedel Method: Example

Repeating more iterations, the following values are obtained

Iteration a1

a 1 a2

a 2

a3

a 3



1 0.50000 67.662 4.900 100.00 3.0923 67.662

2 0.14679 240.62 3.7153 31.887 3.8118 18.876

3 0.74275 80.23 3.1644 17.409 3.9708 4.0042

4 0.94675 21.547 3.0281 4.5012 3.9971 0.65798

5 0.99177 4.5394 3.0034 0.82240 4.0001 0.07499

6 0.99919 0.74260 3.0001 0.11000 4.0001 0.00000



 x1  0.99919

The solution obtained   

 x2    3.0001 



 x3   4.0001 

   

 x1  1 

is close to the exact solution of  x   3

 2  

 x 3  4

   

Comparison of different methods

• Gauss is slow convergent; however, more

stable.

• Gauss-Seidel might not be stable;

however, when stable, converges fast.

• Hotelling and bodewig uses an improved

iterative method for matrix inversion.

• In Relaxation techniques small corrections

will be applied to each element at each

iteration.

Transformations and Eigenvlues

 

• Many problems of the form: y  Ax

 

• Can be written as: y  Sx

• Where S is a diagonal Matrix.

• Where the primed vectors represent the original

vectors in the new space.

 

e   d ij e j

i

j

 

e  De

Eigenvalues and Eigenvectors

 

x  D 1x

 

e  De

  

y   [DAD1 ]x  Sx

DAD1  S

ADT  D T S (Assuming Orthonorma transform

l ations)

Writing in component format :

n n



a

k 1

ik d jk  d ji S jj  d

k 1

jk  ki S jj

n



 (a

k 1

ik   ki S jj ) d jk  0



Det aik   ki S jj  0, j


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