SlideShare une entreprise Scribd logo
1  sur  38
Convergence Criteria

1
Iterative Solution Methods






Starts with an initial approximation for the
solution vector (x0)
At each iteration updates the x vector by using
the sytem Ax=b
During the iterations A, matrix is not changed
so sparcity is preserved



Each iteration involves a matrix-vector product



If A is sparse this product is efficiently done
2
Iterative solution procedure








Write the system Ax=b in an equivalent form
x=Ex+f (like x=g(x) for fixed-point iteration)
Starting with x0, generate a sequence of
approximations {xk} iteratively by
x k+1 =Ex k +f
Representation of E and f depends on the type
of the method used
But for every method E and f are obtained from
A and b, but in a different way
3
Convergence








As k→∞, the sequence {xk} converges to the
solution vector under some conditions on E
matrix
This imposes different conditions on A matrix
for different methods
For the same A matrix, one method may
converge while the other may diverge
Therefore for each method the relation
between A and E should be found to decide on
the convergence
4
Different Iterative methods




Jacobi Iteration
Gauss-Seidel Iteration
Successive Over Relaxation (S.O.R)




SOR is a method used to accelerate the
convergence
Gauss-Seidel Iteration is a special case of SOR
method

5
Jacobi iteration
a11 x1 + a12 x2 +  + a1n xn = b1
a21 x1 + a22 x2 +  + a2 n xn = b2

an1 x1 + an 2 x2 +  + ann xn = bn

 x10 
 0
0
 x2 
x =

 0
 xn 
 

1
0
0
1 
(b1 − a12 x2 −  − a1n xn )
k +1
xi = bi −
a11
aii 
1
0
0
x1 =
(b2 − a21 x10 − a23 x3 −  − a2 n xn )
2
a22
1
0
0
x1 =
(bn − an1 x10 − an 2 x2 −  − ann −1 xn −1 )
n
ann
1
x1 =


∑ aij x − j∑1aij x 
j =1
=i +

i −1

k
j

n

k
j

6
xk+1=Exk+f iteration for Jacobi method
A can be written as A=L+D+U (not decomposition)
0 0  a11 0
0  0 a12 a13 
 a11 a12 a13   0
a
a22 a23  =  a21 0 0 +  0 a22 0  + 0 0 a23 
 21
 
 
 

 a31 a32 a33   a31 a32 0  0
0 a33  0 0
0

 
 
 


Ax=b ⇒ (L+D+U)x=b
1
k +1
xi =
aii
Dxk+1

i −1
n


k
k
bi − ∑ aij x j − ∑ aij x j 
j =1
j = i +1





Lx k



Uxk

Dxk+1 =-(L+U)xk+b
xk+1=-D-1(L+U)xk+D-1b
E=-D-1(L+U)
f=D-1b
7
Gauss-Seidel (GS) iteration
Use the latest
update

a11 x1 + a12 x2 +  + a1n xn = b1
a21 x1 + a22 x2 +  + a2 n xn = b2

an1 x1 + an 2 x2 +  + ann xn = bn

1
0
0
1 
(b1 − a12 x2 −  − a1n xn )
k +1
xi = bi −
a11
aii 
1
1
1
0
0
x2 =
(b2 − a21 x1 − a23 x3 −  − a2 n xn )
a22
1
1
x1 =
(bn − an1 x1 − an 2 x1 −  − ann −1 x1 −1 )
n
2
n
ann
1
x1 =

 x10 
 0
0
 x2 
x =

 0
 xn 
 
i −1

∑a x
j =1

ij

k +1
j


− ∑ aij x 
j = i +1

n

k
j

8
x(k+1)=Ex(k)+f iteration for Gauss-Seidel
Ax=b ⇒ (L+D+U)x=b
k +1
i

x

Dx

1
=
aii

k+1

i −1
n


k +1
k
bi − ∑ aij x j − ∑ aij x j 
j =1
j = i +1





Lx k +1



(D+L)xk+1 =-Uxk+b

Uxk

xk+1=-(D+L)-1Uxk+(D+L)-1b
E=-(D+L)-1U
f=-(D+L)-1b
9
Comparison






Gauss-Seidel iteration converges more rapidly
than the Jacobi iteration since it uses the latest
updates
But there are some cases that Jacobi iteration
does converge but Gauss-Seidel does not
To accelerate the Gauss-Seidel method even
further, successive over relaxation method can
be used
10
Successive Over Relaxation Method


GS iteration can be also written as follows
k +1
i

x

1
=x +
aii
k
i

i −1
n


k +1
k
bi − ∑ aij x j − ∑ aij x j 
j =1
j =i



xik +1 = xik + δ ik

Correction term
ωδ i2

xi3
xi2
xi1
0
i

x

δ

ωδ i1

2
i

δ i1

δ i0

Multiply with

ω >1

Faster
convergence

ωδ i0
11
SOR
xik +1 = xik + ωδ ik
i −1
n


k +1
k
x
bi − ∑ aij x j − ∑ aij x j 
j =1
j =i


i −1
n

1 
k +1
k
k +1
k
xi = (1 − ω ) xi + ω bi − ∑ aij x j − ∑ aij x j 
aii 
j =1
j =i +1

k +1
i

1
= x +ω
aii
k
i

1<ω<2 over relaxation (faster convergence)
0<ω<1 under relaxation (slower convergence)
There is an optimum value for ω
Find it by trial and error (usually around 1.6)
12
x(k+1)=Ex(k)+f iteration for SOR
1
k +1
k
xi = (1 − ω ) xi + ω
aii

i −1
n


k +1
k
bi − ∑ aij x j − ∑ aij x j 
j =1
j = i +1



Dxk+1=(1-ω)Dxk+ωb-ωLxk+1-ωUxk
(D+ ωL)xk+1=[(1-ω)D-ωU]xk+ωb
E=(D+ ωL)-1[(1-ω)D-ωU]
f= ω(D+ ωL)-1b
13
The Conjugate Gradient Method
d 0 = r0 = b − Ax0
T

ri ri
αi = T
d i Ad i
xi +1 = xi + α i Ad i

• Converges if A is a
symmetric positive
definite matrix
• Convergence is
faster

T
i +1 i +1
T
i i

r r
βi +1 =
r r

d i +1 = ri +1 + βi +1d i

14
Convergence of Iterative Methods
ˆ
Define the solution vector as x
k
Define an error vector as e

ˆ
x =e +x
k

k

Substitute this into x

k +1

= Ex + f
k

ˆ
ˆ
ˆ
e k +1 + x = E (e k + x) + f = Ex + f + Ee k
e k +1 = Ee k = EEe k −1 = EEEe k − 2 = E ( k +1) e 0
15
Convergence of Iterative Methods
iteration

e

k +1

= E

( k +1) 0

e ≤ E

( k +1)

e

0

power

The iterative method will converge for any initial
iteration vector if the following condition is satisfied
Convergence condition

Lim e k +1 → 0 if
k →∞

Lim E ( k +1) → 0
k →∞

16
Norm of a vector
A vector norm should satisfy these conditions

x ≥ 0 for every nonzero vector x
x = 0 iff x is a zero vector
αx = α x

for scalar α

x+ y ≤ x + y
Vector norms can be defined in different forms as
long as the norm definition satisfies these conditions
17
Commonly used vector norms
Sum norm or ℓ1 norm

x 1 = x1 + x2 +  + xn
Euclidean norm or ℓ2 norm
2
2
x 2 = x12 + x2 +  + xn

Maximum norm or ℓ∞ norm

x

∞

= max i xi
18
Norm of a matrix
A matrix norm should satisfy these conditions

A ≥0
A = 0 iff A is a zero matrix
for scalar α

αA = α A

A+ B ≤ A + B
Important identitiy

Ax ≤ A x

x is a vector
19
Commonly used matrix norms
Maximum column-sum norm or ℓ1 norm
m

A 1 = max ∑ aij
1≤ j ≤ n

i =1

Spectral norm or ℓ2 norm

A 2 = maximum eigenvalue of AT A
Maximum row-sum norm or ℓ∞ norm
n

A ∞ = max ∑ aij
1≤i ≤ m

j =1

20
Example


Compute the ℓ1 and ℓ∞ norms of the matrix

3 9 5
7 2 4 


6 8 1 


16

19

17 = A ∞
13
15

10

= A1
21
Convergence condition
lim e
k →∞

k +1

→ 0 if

lim E
k →∞

( k +1)

→0

Express E in terms of modal matrix P and Λ
Λ:Diagonal matrix with eigenvalues of E on the diagonal

E = PΛP

−1

E ( k +1) = PΛP −1 PΛP −1  PΛP −1
E ( k +1) = PΛ( k +1) P −1

k
λ1 +1



λk +1
2

Λk +1 = 





λk +1 

n 


lim E ( k +1) → 0 ⇒ lim PΛ( k +1) P −1 → 0 ⇒ lim Λ( k +1) → 0
k →∞

k →∞

k →∞

⇒ lim λki +1 → 0 ⇒ λ i < 1 for i = 1,2 ,...,n
k →∞

22
Sufficient condition for convergence
If the magnitude of all eigenvalues of iteration matrix
E is less than 1 than the iteration is convergent
It is easier to compute the norm of a matrix than to
compute its eigenvalues
Ex = λx

Ex = λ x 

⇒ λ x ≤ E x ⇒ λ ≤ E
Ex ≤ E x 


E < 1 is a sufficient condition for convergence
23
Convergence of Jacobi iteration
E=-D-1(L+U)

 0

 − a21
 a22
E= 



 an1
− a
 nn

a12
−
a11
0



a23
−
a22













ann −1
−
ann

a1n 
−
a11 

a2 n 
−
a22 
 
an −1n 
−

an −1n −1 

0 

24
Convergence of Jacobi iteration
Evaluate the infinity(maximum row sum) norm of E
E

n

∞

<1⇒ ∑
j =1
i≠ j

aij

< 1 for i = 1,2,..., n

aii
n

⇒ aii > ∑ aij
j =1
i≠ j

Diagonally dominant matrix

If A is a diagonally dominant matrix, then Jacobi
iteration converges for any initial vector
25
Stopping Criteria


Ax=b



At any iteration k, the residual term is
rk=b-Axk



Check the norm of the residual term
||b-Axk||



If it is less than a threshold value stop

26
Example 1 (Jacobi Iteration)
 4 − 1 1  x1   7 
 4 − 8 1  x  = − 21

 2  

− 2 1 5  x3   15 

  


0 
x 0 = 0 
 
0 
 

b − Ax 0

2

= 26.7395

Diagonally dominant matrix
0
0
7 + x2 − x3
7
x =
= = 1.75
4
4
0
21 + 4 x10 + x3
21
x1 =
= = 2.625
2
8
8
0
15 + 2 x10 − x2
15
1
x3 =
= = 3.0
5
5
1
1

b − Ax1 = 10.0452
2

27
Example 1 continued...
1
7 + x1 − x3
7 + 2.625 − 3
2
x =
=
= 1.65625
4
4
1
1
21 + 4 x1 + x3 21 + 4 × 1.75 + 3
2
x2 =
=
= 3.875
8
8
1
15 + 2 x1 − x1 15 + 2 × 1.75 − 2.625
2
2
=
= 4.225
x3 =
5
5
2
1

7 + 3.875 − 4.225
= 1.6625
4
21 + 4 ×1.65625 + 4.225
3
x2 =
= 3.98125
8
15 + 2 × 1.65625 − 3.875
3
x3 =
= 2.8875
5

b − Ax 2

2

= 6.7413

x13 =

b − Ax 2

2

= 1.9534

Matrix is diagonally dominant, Jacobi iterations are converging
28
Example 2
− 2 1 5  x1   15 
 4 − 8 1  x  = − 21

 2  

 4 − 1 1  x3   7 

  


0 
x 0 = 0 
 
0 
 

b − Ax 0

2

= 26.7395

The matrix is not diagonally dominant
0
0
− 15 + x2 + 5 x3 − 15
x =
=
= −7.5
2
2
0
21 + 4 x10 + x3
21
1
x2 =
= = 2.625
8
8
1
0
x3 = 7 − 4 x10 + x2
= 7.0
1
1

b − Ax1 = 54.8546
2

29
Example 2 continued...
− 15 + 2.625 + 5 × 7
= 11.3125
2
21 − 4 × 7.5 + 7
x1 =
= −0.25
2
8
1
x3 = 7 + 4 × 7.5 + 2.625 = 39.625
1
x1 =

b − Ax 2

2

= 208.3761

The residual term is increasing at each iteration,
so the iterations are diverging.
Note that the matrix is not diagonally dominant
30
Convergence of Gauss-Seidel
iteration






GS iteration converges for any initial vector if A
is a diagonally dominant matrix
GS iteration converges for any initial vector if A
is a symmetric and positive definite matrix
Matrix A is positive definite if
xTAx>0 for every nonzero x vector
31
Positive Definite Matrices






A matrix is positive definite if all its eigenvalues
are positive
A symmetric diagonally dominant matrix with
positive diagonal entries is positive definite
If a matrix is positive definite



All the diagonal entries are positive
The largest (in magnitude) element of the whole
matrix must lie on the diagonal
32
Positive Definitiness Check
20 12 25
12 15 2 


 25 2 5 



Not positive definite
Largest element is not on the diagonal

5
20 12
12 − 15 2 


5
2 25



Not positive definite
All diagonal entries are not positive

20 12 5 
12 15 2 


 5 2 25



Positive definite
Symmetric, diagonally dominant, all
diagonal entries are positive
33
Positive Definitiness Check
20 12 5 
12 15 2 


 8 2 25



A decision can not be made just by investigating
the matrix.
The matrix is diagonally dominant and all diagonal
entries are positive but it is not symmetric.
To decide, check if all the eigenvalues are positive
34
Example (Gauss-Seidel Iteration)
 4 − 1 1  x1   7 
 4 − 8 1  x  = − 21

 2  

− 2 1 5  x3   15 

  


0 
x 0 = 0 
 
0 
 

b − Ax 0

2

= 26.7395

Diagonally dominant matrix
0
0
7
7 + x2 − x3
= = 1.75
x =
4
4
1
0
21 + 4 x1 + x3 21 + 4 × 1.75
1
=
= 3 .5
x2 =
8
8
1
15 + 2 x1 − x1 15 + 2 × 1.75 − 3.5
1
2 =
= 3 .0
x3 =
5
5
1
1

b − Ax1 = 3.0414
2

b − Ax1 = 10.0452
2

Jacobi iteration
35
Example 1 continued...
1
7 + 3.5 − 3
7 + x1 − x3
2
x =
=
= 1.875
4
4
1
21 + 4 x12 + x3 21 + 4 × 1.875 + 3
2
x2 =
=
= 3.9375
8
8
2
15 + 2 x12 − x2 15 + 2 × 1.875 − 3.9375
2
=
= 2.9625
x3 =
5
5
2
1

b − Ax 2
b − Ax 2

2

2

= 0.4765
= 6.7413

Jacobi iteration

When both Jacobi and Gauss-Seidel iterations
converge, Gauss-Seidel converges faster

36
Convergence of SOR method





If 0<ω<2, SOR method converges for any initial
vector if A matrix is symmetric and positive
definite
If ω>2, SOR method diverges
If 0<ω<1, SOR method converges but the
convergence rate is slower (deceleration) than
the Gauss-Seidel method.
37
Operation count








The operation count for Gaussian Elimination
or LU Decomposition was 0 (n3), order of n3.
For iterative methods, the number of scalar
multiplications is 0 (n2) at each iteration.
If the total number of iterations required for
convergence is much less than n, then iterative
methods are more efficient than direct
methods.
Also iterative methods are well suited for
sparse matrices
38

Contenu connexe

Tendances

Lesson 19: Double Integrals over General Regions
Lesson 19: Double Integrals over General RegionsLesson 19: Double Integrals over General Regions
Lesson 19: Double Integrals over General Regions
Matthew Leingang
 
Numerical differentiation
Numerical differentiationNumerical differentiation
Numerical differentiation
andrushow
 
12 quadric surfaces
12 quadric surfaces12 quadric surfaces
12 quadric surfaces
math267
 

Tendances (20)

Integration by Parts & by Partial Fractions
Integration by Parts & by Partial FractionsIntegration by Parts & by Partial Fractions
Integration by Parts & by Partial Fractions
 
Linear Congruences, reduced residue systems.pptx
Linear Congruences, reduced residue systems.pptxLinear Congruences, reduced residue systems.pptx
Linear Congruences, reduced residue systems.pptx
 
Lesson 19: Double Integrals over General Regions
Lesson 19: Double Integrals over General RegionsLesson 19: Double Integrals over General Regions
Lesson 19: Double Integrals over General Regions
 
Numerical differentiation
Numerical differentiationNumerical differentiation
Numerical differentiation
 
BISECTION METHOD
BISECTION METHODBISECTION METHOD
BISECTION METHOD
 
Fixed point iteration
Fixed point iterationFixed point iteration
Fixed point iteration
 
Lesson 3: The Limit of a Function
Lesson 3: The Limit of a FunctionLesson 3: The Limit of a Function
Lesson 3: The Limit of a Function
 
limits and continuity
limits and continuity limits and continuity
limits and continuity
 
System of linear equations and their solution
System of linear equations and their solutionSystem of linear equations and their solution
System of linear equations and their solution
 
Matrices and determinants
Matrices and determinantsMatrices and determinants
Matrices and determinants
 
Solution of equations and eigenvalue problems
Solution of equations and eigenvalue problemsSolution of equations and eigenvalue problems
Solution of equations and eigenvalue problems
 
Integral calculus
Integral calculusIntegral calculus
Integral calculus
 
metric spaces
metric spacesmetric spaces
metric spaces
 
9.1 Systems of Linear Equations
9.1 Systems of Linear Equations9.1 Systems of Linear Equations
9.1 Systems of Linear Equations
 
Tugas Metode Numerik Golden ratio Pendidikan Matematika UMT
Tugas Metode Numerik Golden ratio Pendidikan Matematika UMTTugas Metode Numerik Golden ratio Pendidikan Matematika UMT
Tugas Metode Numerik Golden ratio Pendidikan Matematika UMT
 
Numerical Methods
Numerical MethodsNumerical Methods
Numerical Methods
 
3.2 Derivative as a Function
3.2 Derivative as a Function3.2 Derivative as a Function
3.2 Derivative as a Function
 
1575 numerical differentiation and integration
1575 numerical differentiation and integration1575 numerical differentiation and integration
1575 numerical differentiation and integration
 
12 quadric surfaces
12 quadric surfaces12 quadric surfaces
12 quadric surfaces
 
Bisection method
Bisection methodBisection method
Bisection method
 

En vedette (8)

Solving Poisson Equation using Conjugate Gradient Method and its implementation
Solving Poisson Equation using Conjugate Gradient Methodand its implementationSolving Poisson Equation using Conjugate Gradient Methodand its implementation
Solving Poisson Equation using Conjugate Gradient Method and its implementation
 
Gauss sediel
Gauss sedielGauss sediel
Gauss sediel
 
Khalid sarwar working principle of ewsd exchange 2014
Khalid sarwar working principle of ewsd exchange 2014Khalid sarwar working principle of ewsd exchange 2014
Khalid sarwar working principle of ewsd exchange 2014
 
Es272 ch4b
Es272 ch4bEs272 ch4b
Es272 ch4b
 
Interactives Methods
Interactives MethodsInteractives Methods
Interactives Methods
 
metode iterasi Gauss seidel
metode iterasi Gauss seidelmetode iterasi Gauss seidel
metode iterasi Gauss seidel
 
Linear Systems Gauss Seidel
Linear Systems   Gauss SeidelLinear Systems   Gauss Seidel
Linear Systems Gauss Seidel
 
Jacobi and gauss-seidel
Jacobi and gauss-seidelJacobi and gauss-seidel
Jacobi and gauss-seidel
 

Similaire à Convergence Criteria

Integration techniques
Integration techniquesIntegration techniques
Integration techniques
Krishna Gali
 
Newton Raphson method for load flow analysis
Newton Raphson method for load flow analysisNewton Raphson method for load flow analysis
Newton Raphson method for load flow analysis
divyanshuprakashrock
 
Calculus 08 techniques_of_integration
Calculus 08 techniques_of_integrationCalculus 08 techniques_of_integration
Calculus 08 techniques_of_integration
tutulk
 

Similaire à Convergence Criteria (20)

On the Seidel’s Method, a Stronger Contraction Fixed Point Iterative Method o...
On the Seidel’s Method, a Stronger Contraction Fixed Point Iterative Method o...On the Seidel’s Method, a Stronger Contraction Fixed Point Iterative Method o...
On the Seidel’s Method, a Stronger Contraction Fixed Point Iterative Method o...
 
03_AJMS_166_18_RA.pdf
03_AJMS_166_18_RA.pdf03_AJMS_166_18_RA.pdf
03_AJMS_166_18_RA.pdf
 
03_AJMS_166_18_RA.pdf
03_AJMS_166_18_RA.pdf03_AJMS_166_18_RA.pdf
03_AJMS_166_18_RA.pdf
 
Topic5
Topic5Topic5
Topic5
 
Maths04
Maths04Maths04
Maths04
 
AJMS_389_22.pdf
AJMS_389_22.pdfAJMS_389_22.pdf
AJMS_389_22.pdf
 
Integration techniques
Integration techniquesIntegration techniques
Integration techniques
 
Imc2016 day2-solutions
Imc2016 day2-solutionsImc2016 day2-solutions
Imc2016 day2-solutions
 
Newton Raphson method for load flow analysis
Newton Raphson method for load flow analysisNewton Raphson method for load flow analysis
Newton Raphson method for load flow analysis
 
QUADRATIC EQUATIONS WITH MATHS PROPER VERIFY
QUADRATIC EQUATIONS WITH MATHS PROPER VERIFYQUADRATIC EQUATIONS WITH MATHS PROPER VERIFY
QUADRATIC EQUATIONS WITH MATHS PROPER VERIFY
 
Solution to schrodinger equation with dirac comb potential
Solution to schrodinger equation with dirac comb potential Solution to schrodinger equation with dirac comb potential
Solution to schrodinger equation with dirac comb potential
 
exponen dan logaritma
exponen dan logaritmaexponen dan logaritma
exponen dan logaritma
 
Solved exercises simple integration
Solved exercises simple integrationSolved exercises simple integration
Solved exercises simple integration
 
Applications of Differential Calculus in real life
Applications of Differential Calculus in real life Applications of Differential Calculus in real life
Applications of Differential Calculus in real life
 
Integration
IntegrationIntegration
Integration
 
Calculus 08 techniques_of_integration
Calculus 08 techniques_of_integrationCalculus 08 techniques_of_integration
Calculus 08 techniques_of_integration
 
Lecture 9 f17
Lecture 9 f17Lecture 9 f17
Lecture 9 f17
 
Sample question paper 2 with solution
Sample question paper 2 with solutionSample question paper 2 with solution
Sample question paper 2 with solution
 
Cse41
Cse41Cse41
Cse41
 
Business Math Chapter 3
Business Math Chapter 3Business Math Chapter 3
Business Math Chapter 3
 

Plus de Tarun Gehlot

Plus de Tarun Gehlot (20)

Materials 11-01228
Materials 11-01228Materials 11-01228
Materials 11-01228
 
Binary relations
Binary relationsBinary relations
Binary relations
 
Continuity and end_behavior
Continuity and  end_behaviorContinuity and  end_behavior
Continuity and end_behavior
 
Continuity of functions by graph (exercises with detailed solutions)
Continuity of functions by graph   (exercises with detailed solutions)Continuity of functions by graph   (exercises with detailed solutions)
Continuity of functions by graph (exercises with detailed solutions)
 
Factoring by the trial and-error method
Factoring by the trial and-error methodFactoring by the trial and-error method
Factoring by the trial and-error method
 
Introduction to finite element analysis
Introduction to finite element analysisIntroduction to finite element analysis
Introduction to finite element analysis
 
Finite elements : basis functions
Finite elements : basis functionsFinite elements : basis functions
Finite elements : basis functions
 
Finite elements for 2‐d problems
Finite elements  for 2‐d problemsFinite elements  for 2‐d problems
Finite elements for 2‐d problems
 
Error analysis statistics
Error analysis   statisticsError analysis   statistics
Error analysis statistics
 
Matlab commands
Matlab commandsMatlab commands
Matlab commands
 
Introduction to matlab
Introduction to matlabIntroduction to matlab
Introduction to matlab
 
Linear approximations and_differentials
Linear approximations and_differentialsLinear approximations and_differentials
Linear approximations and_differentials
 
Local linear approximation
Local linear approximationLocal linear approximation
Local linear approximation
 
Interpolation functions
Interpolation functionsInterpolation functions
Interpolation functions
 
Propeties of-triangles
Propeties of-trianglesPropeties of-triangles
Propeties of-triangles
 
Gaussian quadratures
Gaussian quadraturesGaussian quadratures
Gaussian quadratures
 
Basics of set theory
Basics of set theoryBasics of set theory
Basics of set theory
 
Numerical integration
Numerical integrationNumerical integration
Numerical integration
 
Applications of set theory
Applications of  set theoryApplications of  set theory
Applications of set theory
 
Miscellneous functions
Miscellneous  functionsMiscellneous  functions
Miscellneous functions
 

Dernier

The basics of sentences session 3pptx.pptx
The basics of sentences session 3pptx.pptxThe basics of sentences session 3pptx.pptx
The basics of sentences session 3pptx.pptx
heathfieldcps1
 

Dernier (20)

Micro-Scholarship, What it is, How can it help me.pdf
Micro-Scholarship, What it is, How can it help me.pdfMicro-Scholarship, What it is, How can it help me.pdf
Micro-Scholarship, What it is, How can it help me.pdf
 
Sociology 101 Demonstration of Learning Exhibit
Sociology 101 Demonstration of Learning ExhibitSociology 101 Demonstration of Learning Exhibit
Sociology 101 Demonstration of Learning Exhibit
 
ICT Role in 21st Century Education & its Challenges.pptx
ICT Role in 21st Century Education & its Challenges.pptxICT Role in 21st Century Education & its Challenges.pptx
ICT Role in 21st Century Education & its Challenges.pptx
 
How to Manage Global Discount in Odoo 17 POS
How to Manage Global Discount in Odoo 17 POSHow to Manage Global Discount in Odoo 17 POS
How to Manage Global Discount in Odoo 17 POS
 
REMIFENTANIL: An Ultra short acting opioid.pptx
REMIFENTANIL: An Ultra short acting opioid.pptxREMIFENTANIL: An Ultra short acting opioid.pptx
REMIFENTANIL: An Ultra short acting opioid.pptx
 
Google Gemini An AI Revolution in Education.pptx
Google Gemini An AI Revolution in Education.pptxGoogle Gemini An AI Revolution in Education.pptx
Google Gemini An AI Revolution in Education.pptx
 
Unit-V; Pricing (Pharma Marketing Management).pptx
Unit-V; Pricing (Pharma Marketing Management).pptxUnit-V; Pricing (Pharma Marketing Management).pptx
Unit-V; Pricing (Pharma Marketing Management).pptx
 
Making communications land - Are they received and understood as intended? we...
Making communications land - Are they received and understood as intended? we...Making communications land - Are they received and understood as intended? we...
Making communications land - Are they received and understood as intended? we...
 
This PowerPoint helps students to consider the concept of infinity.
This PowerPoint helps students to consider the concept of infinity.This PowerPoint helps students to consider the concept of infinity.
This PowerPoint helps students to consider the concept of infinity.
 
Jamworks pilot and AI at Jisc (20/03/2024)
Jamworks pilot and AI at Jisc (20/03/2024)Jamworks pilot and AI at Jisc (20/03/2024)
Jamworks pilot and AI at Jisc (20/03/2024)
 
How to setup Pycharm environment for Odoo 17.pptx
How to setup Pycharm environment for Odoo 17.pptxHow to setup Pycharm environment for Odoo 17.pptx
How to setup Pycharm environment for Odoo 17.pptx
 
SOC 101 Demonstration of Learning Presentation
SOC 101 Demonstration of Learning PresentationSOC 101 Demonstration of Learning Presentation
SOC 101 Demonstration of Learning Presentation
 
80 ĐỀ THI THỬ TUYỂN SINH TIẾNG ANH VÀO 10 SỞ GD – ĐT THÀNH PHỐ HỒ CHÍ MINH NĂ...
80 ĐỀ THI THỬ TUYỂN SINH TIẾNG ANH VÀO 10 SỞ GD – ĐT THÀNH PHỐ HỒ CHÍ MINH NĂ...80 ĐỀ THI THỬ TUYỂN SINH TIẾNG ANH VÀO 10 SỞ GD – ĐT THÀNH PHỐ HỒ CHÍ MINH NĂ...
80 ĐỀ THI THỬ TUYỂN SINH TIẾNG ANH VÀO 10 SỞ GD – ĐT THÀNH PHỐ HỒ CHÍ MINH NĂ...
 
Food safety_Challenges food safety laboratories_.pdf
Food safety_Challenges food safety laboratories_.pdfFood safety_Challenges food safety laboratories_.pdf
Food safety_Challenges food safety laboratories_.pdf
 
Introduction to Nonprofit Accounting: The Basics
Introduction to Nonprofit Accounting: The BasicsIntroduction to Nonprofit Accounting: The Basics
Introduction to Nonprofit Accounting: The Basics
 
The basics of sentences session 3pptx.pptx
The basics of sentences session 3pptx.pptxThe basics of sentences session 3pptx.pptx
The basics of sentences session 3pptx.pptx
 
ICT role in 21st century education and it's challenges.
ICT role in 21st century education and it's challenges.ICT role in 21st century education and it's challenges.
ICT role in 21st century education and it's challenges.
 
Accessible Digital Futures project (20/03/2024)
Accessible Digital Futures project (20/03/2024)Accessible Digital Futures project (20/03/2024)
Accessible Digital Futures project (20/03/2024)
 
General Principles of Intellectual Property: Concepts of Intellectual Proper...
General Principles of Intellectual Property: Concepts of Intellectual  Proper...General Principles of Intellectual Property: Concepts of Intellectual  Proper...
General Principles of Intellectual Property: Concepts of Intellectual Proper...
 
Interdisciplinary_Insights_Data_Collection_Methods.pptx
Interdisciplinary_Insights_Data_Collection_Methods.pptxInterdisciplinary_Insights_Data_Collection_Methods.pptx
Interdisciplinary_Insights_Data_Collection_Methods.pptx
 

Convergence Criteria

  • 2. Iterative Solution Methods    Starts with an initial approximation for the solution vector (x0) At each iteration updates the x vector by using the sytem Ax=b During the iterations A, matrix is not changed so sparcity is preserved  Each iteration involves a matrix-vector product  If A is sparse this product is efficiently done 2
  • 3. Iterative solution procedure     Write the system Ax=b in an equivalent form x=Ex+f (like x=g(x) for fixed-point iteration) Starting with x0, generate a sequence of approximations {xk} iteratively by x k+1 =Ex k +f Representation of E and f depends on the type of the method used But for every method E and f are obtained from A and b, but in a different way 3
  • 4. Convergence     As k→∞, the sequence {xk} converges to the solution vector under some conditions on E matrix This imposes different conditions on A matrix for different methods For the same A matrix, one method may converge while the other may diverge Therefore for each method the relation between A and E should be found to decide on the convergence 4
  • 5. Different Iterative methods    Jacobi Iteration Gauss-Seidel Iteration Successive Over Relaxation (S.O.R)   SOR is a method used to accelerate the convergence Gauss-Seidel Iteration is a special case of SOR method 5
  • 6. Jacobi iteration a11 x1 + a12 x2 +  + a1n xn = b1 a21 x1 + a22 x2 +  + a2 n xn = b2  an1 x1 + an 2 x2 +  + ann xn = bn  x10   0 0  x2  x =   0  xn    1 0 0 1  (b1 − a12 x2 −  − a1n xn ) k +1 xi = bi − a11 aii  1 0 0 x1 = (b2 − a21 x10 − a23 x3 −  − a2 n xn ) 2 a22 1 0 0 x1 = (bn − an1 x10 − an 2 x2 −  − ann −1 xn −1 ) n ann 1 x1 =  ∑ aij x − j∑1aij x  j =1 =i +  i −1 k j n k j 6
  • 7. xk+1=Exk+f iteration for Jacobi method A can be written as A=L+D+U (not decomposition) 0 0  a11 0 0  0 a12 a13   a11 a12 a13   0 a a22 a23  =  a21 0 0 +  0 a22 0  + 0 0 a23   21         a31 a32 a33   a31 a32 0  0 0 a33  0 0 0         Ax=b ⇒ (L+D+U)x=b 1 k +1 xi = aii Dxk+1 i −1 n   k k bi − ∑ aij x j − ∑ aij x j  j =1 j = i +1    Lx k  Uxk Dxk+1 =-(L+U)xk+b xk+1=-D-1(L+U)xk+D-1b E=-D-1(L+U) f=D-1b 7
  • 8. Gauss-Seidel (GS) iteration Use the latest update a11 x1 + a12 x2 +  + a1n xn = b1 a21 x1 + a22 x2 +  + a2 n xn = b2  an1 x1 + an 2 x2 +  + ann xn = bn 1 0 0 1  (b1 − a12 x2 −  − a1n xn ) k +1 xi = bi − a11 aii  1 1 1 0 0 x2 = (b2 − a21 x1 − a23 x3 −  − a2 n xn ) a22 1 1 x1 = (bn − an1 x1 − an 2 x1 −  − ann −1 x1 −1 ) n 2 n ann 1 x1 =  x10   0 0  x2  x =   0  xn    i −1 ∑a x j =1 ij k +1 j  − ∑ aij x  j = i +1  n k j 8
  • 9. x(k+1)=Ex(k)+f iteration for Gauss-Seidel Ax=b ⇒ (L+D+U)x=b k +1 i x Dx 1 = aii k+1 i −1 n   k +1 k bi − ∑ aij x j − ∑ aij x j  j =1 j = i +1    Lx k +1  (D+L)xk+1 =-Uxk+b Uxk xk+1=-(D+L)-1Uxk+(D+L)-1b E=-(D+L)-1U f=-(D+L)-1b 9
  • 10. Comparison    Gauss-Seidel iteration converges more rapidly than the Jacobi iteration since it uses the latest updates But there are some cases that Jacobi iteration does converge but Gauss-Seidel does not To accelerate the Gauss-Seidel method even further, successive over relaxation method can be used 10
  • 11. Successive Over Relaxation Method  GS iteration can be also written as follows k +1 i x 1 =x + aii k i i −1 n   k +1 k bi − ∑ aij x j − ∑ aij x j  j =1 j =i   xik +1 = xik + δ ik Correction term ωδ i2 xi3 xi2 xi1 0 i x δ ωδ i1 2 i δ i1 δ i0 Multiply with ω >1 Faster convergence ωδ i0 11
  • 12. SOR xik +1 = xik + ωδ ik i −1 n   k +1 k x bi − ∑ aij x j − ∑ aij x j  j =1 j =i   i −1 n  1  k +1 k k +1 k xi = (1 − ω ) xi + ω bi − ∑ aij x j − ∑ aij x j  aii  j =1 j =i +1  k +1 i 1 = x +ω aii k i 1<ω<2 over relaxation (faster convergence) 0<ω<1 under relaxation (slower convergence) There is an optimum value for ω Find it by trial and error (usually around 1.6) 12
  • 13. x(k+1)=Ex(k)+f iteration for SOR 1 k +1 k xi = (1 − ω ) xi + ω aii i −1 n   k +1 k bi − ∑ aij x j − ∑ aij x j  j =1 j = i +1   Dxk+1=(1-ω)Dxk+ωb-ωLxk+1-ωUxk (D+ ωL)xk+1=[(1-ω)D-ωU]xk+ωb E=(D+ ωL)-1[(1-ω)D-ωU] f= ω(D+ ωL)-1b 13
  • 14. The Conjugate Gradient Method d 0 = r0 = b − Ax0 T ri ri αi = T d i Ad i xi +1 = xi + α i Ad i • Converges if A is a symmetric positive definite matrix • Convergence is faster T i +1 i +1 T i i r r βi +1 = r r d i +1 = ri +1 + βi +1d i 14
  • 15. Convergence of Iterative Methods ˆ Define the solution vector as x k Define an error vector as e ˆ x =e +x k k Substitute this into x k +1 = Ex + f k ˆ ˆ ˆ e k +1 + x = E (e k + x) + f = Ex + f + Ee k e k +1 = Ee k = EEe k −1 = EEEe k − 2 = E ( k +1) e 0 15
  • 16. Convergence of Iterative Methods iteration e k +1 = E ( k +1) 0 e ≤ E ( k +1) e 0 power The iterative method will converge for any initial iteration vector if the following condition is satisfied Convergence condition Lim e k +1 → 0 if k →∞ Lim E ( k +1) → 0 k →∞ 16
  • 17. Norm of a vector A vector norm should satisfy these conditions x ≥ 0 for every nonzero vector x x = 0 iff x is a zero vector αx = α x for scalar α x+ y ≤ x + y Vector norms can be defined in different forms as long as the norm definition satisfies these conditions 17
  • 18. Commonly used vector norms Sum norm or ℓ1 norm x 1 = x1 + x2 +  + xn Euclidean norm or ℓ2 norm 2 2 x 2 = x12 + x2 +  + xn Maximum norm or ℓ∞ norm x ∞ = max i xi 18
  • 19. Norm of a matrix A matrix norm should satisfy these conditions A ≥0 A = 0 iff A is a zero matrix for scalar α αA = α A A+ B ≤ A + B Important identitiy Ax ≤ A x x is a vector 19
  • 20. Commonly used matrix norms Maximum column-sum norm or ℓ1 norm m A 1 = max ∑ aij 1≤ j ≤ n i =1 Spectral norm or ℓ2 norm A 2 = maximum eigenvalue of AT A Maximum row-sum norm or ℓ∞ norm n A ∞ = max ∑ aij 1≤i ≤ m j =1 20
  • 21. Example  Compute the ℓ1 and ℓ∞ norms of the matrix 3 9 5 7 2 4    6 8 1    16 19 17 = A ∞ 13 15 10 = A1 21
  • 22. Convergence condition lim e k →∞ k +1 → 0 if lim E k →∞ ( k +1) →0 Express E in terms of modal matrix P and Λ Λ:Diagonal matrix with eigenvalues of E on the diagonal E = PΛP −1 E ( k +1) = PΛP −1 PΛP −1  PΛP −1 E ( k +1) = PΛ( k +1) P −1 k λ1 +1    λk +1 2  Λk +1 =       λk +1   n   lim E ( k +1) → 0 ⇒ lim PΛ( k +1) P −1 → 0 ⇒ lim Λ( k +1) → 0 k →∞ k →∞ k →∞ ⇒ lim λki +1 → 0 ⇒ λ i < 1 for i = 1,2 ,...,n k →∞ 22
  • 23. Sufficient condition for convergence If the magnitude of all eigenvalues of iteration matrix E is less than 1 than the iteration is convergent It is easier to compute the norm of a matrix than to compute its eigenvalues Ex = λx Ex = λ x   ⇒ λ x ≤ E x ⇒ λ ≤ E Ex ≤ E x   E < 1 is a sufficient condition for convergence 23
  • 24. Convergence of Jacobi iteration E=-D-1(L+U)   0   − a21  a22 E=      an1 − a  nn a12 − a11 0   a23 − a22         ann −1 − ann a1n  − a11   a2 n  − a22    an −1n  −  an −1n −1   0   24
  • 25. Convergence of Jacobi iteration Evaluate the infinity(maximum row sum) norm of E E n ∞ <1⇒ ∑ j =1 i≠ j aij < 1 for i = 1,2,..., n aii n ⇒ aii > ∑ aij j =1 i≠ j Diagonally dominant matrix If A is a diagonally dominant matrix, then Jacobi iteration converges for any initial vector 25
  • 26. Stopping Criteria  Ax=b  At any iteration k, the residual term is rk=b-Axk  Check the norm of the residual term ||b-Axk||  If it is less than a threshold value stop 26
  • 27. Example 1 (Jacobi Iteration)  4 − 1 1  x1   7   4 − 8 1  x  = − 21   2    − 2 1 5  x3   15       0  x 0 = 0    0    b − Ax 0 2 = 26.7395 Diagonally dominant matrix 0 0 7 + x2 − x3 7 x = = = 1.75 4 4 0 21 + 4 x10 + x3 21 x1 = = = 2.625 2 8 8 0 15 + 2 x10 − x2 15 1 x3 = = = 3.0 5 5 1 1 b − Ax1 = 10.0452 2 27
  • 28. Example 1 continued... 1 7 + x1 − x3 7 + 2.625 − 3 2 x = = = 1.65625 4 4 1 1 21 + 4 x1 + x3 21 + 4 × 1.75 + 3 2 x2 = = = 3.875 8 8 1 15 + 2 x1 − x1 15 + 2 × 1.75 − 2.625 2 2 = = 4.225 x3 = 5 5 2 1 7 + 3.875 − 4.225 = 1.6625 4 21 + 4 ×1.65625 + 4.225 3 x2 = = 3.98125 8 15 + 2 × 1.65625 − 3.875 3 x3 = = 2.8875 5 b − Ax 2 2 = 6.7413 x13 = b − Ax 2 2 = 1.9534 Matrix is diagonally dominant, Jacobi iterations are converging 28
  • 29. Example 2 − 2 1 5  x1   15   4 − 8 1  x  = − 21   2     4 − 1 1  x3   7       0  x 0 = 0    0    b − Ax 0 2 = 26.7395 The matrix is not diagonally dominant 0 0 − 15 + x2 + 5 x3 − 15 x = = = −7.5 2 2 0 21 + 4 x10 + x3 21 1 x2 = = = 2.625 8 8 1 0 x3 = 7 − 4 x10 + x2 = 7.0 1 1 b − Ax1 = 54.8546 2 29
  • 30. Example 2 continued... − 15 + 2.625 + 5 × 7 = 11.3125 2 21 − 4 × 7.5 + 7 x1 = = −0.25 2 8 1 x3 = 7 + 4 × 7.5 + 2.625 = 39.625 1 x1 = b − Ax 2 2 = 208.3761 The residual term is increasing at each iteration, so the iterations are diverging. Note that the matrix is not diagonally dominant 30
  • 31. Convergence of Gauss-Seidel iteration    GS iteration converges for any initial vector if A is a diagonally dominant matrix GS iteration converges for any initial vector if A is a symmetric and positive definite matrix Matrix A is positive definite if xTAx>0 for every nonzero x vector 31
  • 32. Positive Definite Matrices    A matrix is positive definite if all its eigenvalues are positive A symmetric diagonally dominant matrix with positive diagonal entries is positive definite If a matrix is positive definite   All the diagonal entries are positive The largest (in magnitude) element of the whole matrix must lie on the diagonal 32
  • 33. Positive Definitiness Check 20 12 25 12 15 2     25 2 5    Not positive definite Largest element is not on the diagonal 5 20 12 12 − 15 2    5 2 25   Not positive definite All diagonal entries are not positive 20 12 5  12 15 2     5 2 25   Positive definite Symmetric, diagonally dominant, all diagonal entries are positive 33
  • 34. Positive Definitiness Check 20 12 5  12 15 2     8 2 25   A decision can not be made just by investigating the matrix. The matrix is diagonally dominant and all diagonal entries are positive but it is not symmetric. To decide, check if all the eigenvalues are positive 34
  • 35. Example (Gauss-Seidel Iteration)  4 − 1 1  x1   7   4 − 8 1  x  = − 21   2    − 2 1 5  x3   15       0  x 0 = 0    0    b − Ax 0 2 = 26.7395 Diagonally dominant matrix 0 0 7 7 + x2 − x3 = = 1.75 x = 4 4 1 0 21 + 4 x1 + x3 21 + 4 × 1.75 1 = = 3 .5 x2 = 8 8 1 15 + 2 x1 − x1 15 + 2 × 1.75 − 3.5 1 2 = = 3 .0 x3 = 5 5 1 1 b − Ax1 = 3.0414 2 b − Ax1 = 10.0452 2 Jacobi iteration 35
  • 36. Example 1 continued... 1 7 + 3.5 − 3 7 + x1 − x3 2 x = = = 1.875 4 4 1 21 + 4 x12 + x3 21 + 4 × 1.875 + 3 2 x2 = = = 3.9375 8 8 2 15 + 2 x12 − x2 15 + 2 × 1.875 − 3.9375 2 = = 2.9625 x3 = 5 5 2 1 b − Ax 2 b − Ax 2 2 2 = 0.4765 = 6.7413 Jacobi iteration When both Jacobi and Gauss-Seidel iterations converge, Gauss-Seidel converges faster 36
  • 37. Convergence of SOR method    If 0<ω<2, SOR method converges for any initial vector if A matrix is symmetric and positive definite If ω>2, SOR method diverges If 0<ω<1, SOR method converges but the convergence rate is slower (deceleration) than the Gauss-Seidel method. 37
  • 38. Operation count     The operation count for Gaussian Elimination or LU Decomposition was 0 (n3), order of n3. For iterative methods, the number of scalar multiplications is 0 (n2) at each iteration. If the total number of iterations required for convergence is much less than n, then iterative methods are more efficient than direct methods. Also iterative methods are well suited for sparse matrices 38