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MATHEMATICAL METHODS
CONTENTS
•   Matrices and Linear systems of equations
•   Eigen values and eigen vectors
•   Real and complex matrices and Quadratic forms
•   Algebraic equations transcendental equations and
    Interpolation
•   Curve Fitting, numerical differentiation & integration
•   Numerical differentiation of O.D.E
•   Fourier series and Fourier transforms
•   Partial differential equation and Z-transforms
TEXT BOOKS
• 1.Mathematical Methods, T.K.V.Iyengar, B.Krishna
  Gandhi and others, S.Chand and company
• Mathematical Methods, C.Sankaraiah, V.G.S.Book
  links.
• A text book of Mathametical Methods,
  V.Ravindranath, A.Vijayalakshmi, Himalaya
  Publishers.
• A text book of Mathametical Methods, Shahnaz
  Bathul, Right Publishers.
REFERENCES
• 1. A text book of Engineering Mathematics,
  B.V.Ramana, Tata Mc Graw Hill.
• 2.Advanced Engineering Mathematics, Irvin Kreyszig
  Wiley India Pvt Ltd.
• 3. Numerical Methods for scientific and Engineering
  computation, M.K.Jain, S.R.K.Iyengar and R.K.Jain,
  New Age International Publishers
• Elementary Numerical Analysis, Aitkison and Han,
  Wiley India, 3rd Edition, 2006.
UNIT HEADER
     Name of the Course:B.Tech
        Code No:07A1BS02
Year/Branch:I Year CSE,IT,ECE,EEE,
            Unit No: I V
          No.of slides:23
UNIT INDEX
                      UNIT-IV
S.No.          Module        Lecture   PPT Slide
                             No.       No.
  1     Bisection Method,    L1-4      8-11
        Iteration
        method,Newton-
        Raphson,Regula
        Falsi method
  2     Finite Differences   L5-6      12-17

  3     Interpolation.       L7-12     18-24
UNIT-IV
               CHAPTER-5
Solutions of Algebraic and transcendental equations

               CHAPTER-6
                   Interpolation
LECTURE-1
Method 1: Bisection method

                  If a function f(x) is continuous b/w x0 and x1 and
  f(x0) & f(x1) are of opposite signs, then there exsist at least one
  root b/w x0 and x1
 Let f(x0) be –ve and f(x1) be +ve ,then the root lies b/w xo
   and x1 and its approximate value is given by x2=(x0+x1)/2
 If f(x2)=0,we conclude that x2 is a root of the equ f(x)=0
 Otherwise the root lies either b/w x2 and x1 (or) b/w x2 and x0
       depending on wheather f(x2) is +ve or –ve

         Then as before, we bisect the interval and repeat the
  process untill the root is known to the desired accuracy
LECTURE-2
Method 2: Iteration method or successive approximation
              Consider the equation f(x)=0 which can take in the form
    x = ø(x) -------------(1)
          where |ø1(x)|<1 for all values of x.
Taking initial approximation is x0
we put x1=ø(x0) and take x1 is the first approximation
      x2=ø(x1) , x2 is the second approximation
      x3=ø(x2) ,x3 is the third approximation
           .
           .
      xn=ø(xn-1) ,xn is the nth approximation
Such a process is called an iteration process
LECTURE-3
  Method 3: Newton-Raphson method or Newton iteration
                               method
 Let the given equation be f(x)=0
 Find f1(x) and initial approximation x0


The first approximation is x1= x0-f(x0)/ f1(x0)


The second approximation is x2= x1-f(x1)/ f1(x1)
   .
   .
 The nth approximation is xn= xn-1-f(xn)/ f1(xn)
LECTURE-4
Finite difference methods

        Let (xi,yi),i=0,1,2…………..n be the equally spaced data of the
 unknown function y=f(x) then much of the f(x) can be extracted by analyzing
the differences of f(x).
     Let x1 = x0+h
        x2 = x0+2h
            .
            .
            .
        xn = x0+nh be equally spaced points where the function value of f(x)
be y0, y1, y2…………….. yn
Symbolic operators

Forward shift operator(E) :
    It is defined as Ef(x)=f(x+h)    (or)     Eyx = yx+h

  The second and higher order forward shift operators are defined
   in similar manner as follows

          E2f(x)= E(Ef(x))= E(f(x+h)= f(x+2h)= yx+2h

     E3f(x)= f(x+3h)
               .
               .
          Ekf(x)= f(x+kh)
LECTURE-5
Backward shift operator(E-1) :
   It is defined as E-1f(x)=f(x-h)       (or) Eyx = yx-h

  The second and higher order backward shift operators
  are defined in similar manner as follows

    E-2f(x)= E-1(E-1f(x))= E-1(f(x-h)= f(x-2h)= yx-2h

     E-3f(x)= f(x-3h)
                 .
                 .
           E-kf(x)= f(x-kh)
Forward difference operator (∆) :

          The first order forward difference operator of a function
   f(x) with increment h in x is given by
         ∆f(x)=f(x+h)-f(x)     (or)     ∆fk =fk+1-fk ; k=0,1,2………
          ∆2f(x)= ∆[∆f(x)]= ∆[f(x+h)-f(x)]= ∆fk+1- ∆fk ; k=0,1,2…………
          …………………………….
          …………………………….
Relation between E and ∆ :
              ∆f(x)=f(x+h)-f(x)
                  =Ef(x)-f(x)              [Ef(x)=f(x+h)]
                   =(E-1)f(x)

              ∆=E-1    E=1+ ∆
LECTURE-6
                              ∇
Backward difference operator (nabla ) :

   The first order backward difference operator of a function
                                                   ∇
   f(x) with increment h in x is given by
        ∇ f(x)=f(x)-f(x-h)  (or)     ∇ k =fk+1-fk ; k=0,1,2………
                                      f
        ∇f(x)= ∇[ f(x)]=
                ∇      [f(x+h)-f(x)]=∇ fk+1- ∇k ; k=0,1,2…………
                                              f
          …………………………….
          …………………………….
Relation between E and nabla :
            nabla f(x)=f(x+h)-f(x)
                 =Ef(x)-f(x)                 [Ef(x)=f(x+h)]
                  =(E-1)f(x)

         nabla=E-1     E=1+ nabla
Central difference operator ( δ) :

        The central difference operator is
defined as
        δf(x)= f(x+h/2)-f(x-h/2)
          δf(x)= E1/2f(x)-E-1/2f(x)
               = [E1/2-E-1/2]f(x)
              δ= E1/2-E-1/2
LECTURE-7
INTERPOLATION : The process of finding a
  missed value in the given table values of X, Y.



FINITE DIFFERENCES : We have three finite
   differences
  1. Forward Difference
  2. Backward Difference
  3. Central Difference
RELATIONS BETWEEN THE OPERATORS
              IDENTITIES:



    ∇
1. ∆=E-1 or E=1+ ∆          ∇


2. = 1- E -1
3. δ = E 1/2 – E -1/2
4. µ= ½∇ 1/2-E-1/2)
         (E ∇
5. ∆=E = ∇E= δE1/2
6. (1+ ∆)(1- )=1
LECTURE-8,9
Newtons Forward interpolation formula :

y=f(x)=f(x0+ph)= y0 + p∆y0 + p(p-1)/2! ∆2y0 + p(p-1)(p-
  2)/3! ∆3y0+…….. ………………+p(p-1)(p2) …… [p-
  (n-1)]/n! ∆ny0 .




Newtons Backward interpolatin formula :
y=f(x)=f(xn+ph)= yn + p∆yn + p(p+1)/2! ∆2yn + p(p+1)
  (p+2)/3! ∆3yn+…….. ………………+p(p+1)(p+2)
  …… [p+(n-1)]/n! ∆nyn .
LECTURE-10,11
          GAUSS INTERPOLATION
The Guass forward interpolation is given by yp = yo + p
  ∆y0+p(p-1)/2! ∆2y-1 +(p+1)p(p-1)/3! ∆3y-1+(p+1)p(p-
  1)(p-2)/4! ∆4y-2+……


The Guass backward interpolation is given by
 yp = yo + p ∆y-1+p(p+1)/2! ∆2y-1 +(p+1)p(p-1)/3! ∆3y-2+
 (p+2)(p+1)p(p-1)/4! ∆4y-2+……
LECTURE-12
INTERPOLATIN WITH UNEQUAL INTERVALS:


The various interpolation formulae Newton’s forward
formula, Newton’s backward formula possess can be
applied only to equal spaced values of argument. It is
therefore, desirable to develop interpolation formula for
unequally spaced values of x. We use Lagrange’s
interpolation formula.
The Lagrange’s interpolation formula is given by

 Y = (X-X1)(X-X2)……..(X-Xn)           Y0 +
     (X0-X1)(X0-X2)……..(X0-Xn)


   (X-X0)(X-X2)……..(X-Xn)        Y1 +…………………..
     (X1-X0)(X1-X2)……..(X1-Xn)


   (X-X0)(X-X1)……..(X-Xn-1)        Yn +
     (Xn-X0)(Xn-X1)……..(Xn-Xn-1)

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Unit iv

  • 2. CONTENTS • Matrices and Linear systems of equations • Eigen values and eigen vectors • Real and complex matrices and Quadratic forms • Algebraic equations transcendental equations and Interpolation • Curve Fitting, numerical differentiation & integration • Numerical differentiation of O.D.E • Fourier series and Fourier transforms • Partial differential equation and Z-transforms
  • 3. TEXT BOOKS • 1.Mathematical Methods, T.K.V.Iyengar, B.Krishna Gandhi and others, S.Chand and company • Mathematical Methods, C.Sankaraiah, V.G.S.Book links. • A text book of Mathametical Methods, V.Ravindranath, A.Vijayalakshmi, Himalaya Publishers. • A text book of Mathametical Methods, Shahnaz Bathul, Right Publishers.
  • 4. REFERENCES • 1. A text book of Engineering Mathematics, B.V.Ramana, Tata Mc Graw Hill. • 2.Advanced Engineering Mathematics, Irvin Kreyszig Wiley India Pvt Ltd. • 3. Numerical Methods for scientific and Engineering computation, M.K.Jain, S.R.K.Iyengar and R.K.Jain, New Age International Publishers • Elementary Numerical Analysis, Aitkison and Han, Wiley India, 3rd Edition, 2006.
  • 5. UNIT HEADER Name of the Course:B.Tech Code No:07A1BS02 Year/Branch:I Year CSE,IT,ECE,EEE, Unit No: I V No.of slides:23
  • 6. UNIT INDEX UNIT-IV S.No. Module Lecture PPT Slide No. No. 1 Bisection Method, L1-4 8-11 Iteration method,Newton- Raphson,Regula Falsi method 2 Finite Differences L5-6 12-17 3 Interpolation. L7-12 18-24
  • 7. UNIT-IV CHAPTER-5 Solutions of Algebraic and transcendental equations CHAPTER-6 Interpolation
  • 8. LECTURE-1 Method 1: Bisection method If a function f(x) is continuous b/w x0 and x1 and f(x0) & f(x1) are of opposite signs, then there exsist at least one root b/w x0 and x1  Let f(x0) be –ve and f(x1) be +ve ,then the root lies b/w xo and x1 and its approximate value is given by x2=(x0+x1)/2  If f(x2)=0,we conclude that x2 is a root of the equ f(x)=0  Otherwise the root lies either b/w x2 and x1 (or) b/w x2 and x0 depending on wheather f(x2) is +ve or –ve Then as before, we bisect the interval and repeat the process untill the root is known to the desired accuracy
  • 9. LECTURE-2 Method 2: Iteration method or successive approximation Consider the equation f(x)=0 which can take in the form x = ø(x) -------------(1) where |ø1(x)|<1 for all values of x. Taking initial approximation is x0 we put x1=ø(x0) and take x1 is the first approximation x2=ø(x1) , x2 is the second approximation x3=ø(x2) ,x3 is the third approximation . . xn=ø(xn-1) ,xn is the nth approximation Such a process is called an iteration process
  • 10. LECTURE-3 Method 3: Newton-Raphson method or Newton iteration method Let the given equation be f(x)=0 Find f1(x) and initial approximation x0 The first approximation is x1= x0-f(x0)/ f1(x0) The second approximation is x2= x1-f(x1)/ f1(x1) . . The nth approximation is xn= xn-1-f(xn)/ f1(xn)
  • 11. LECTURE-4 Finite difference methods Let (xi,yi),i=0,1,2…………..n be the equally spaced data of the unknown function y=f(x) then much of the f(x) can be extracted by analyzing the differences of f(x). Let x1 = x0+h x2 = x0+2h . . . xn = x0+nh be equally spaced points where the function value of f(x) be y0, y1, y2…………….. yn
  • 12. Symbolic operators Forward shift operator(E) : It is defined as Ef(x)=f(x+h) (or) Eyx = yx+h The second and higher order forward shift operators are defined in similar manner as follows E2f(x)= E(Ef(x))= E(f(x+h)= f(x+2h)= yx+2h E3f(x)= f(x+3h) . . Ekf(x)= f(x+kh)
  • 13. LECTURE-5 Backward shift operator(E-1) : It is defined as E-1f(x)=f(x-h) (or) Eyx = yx-h The second and higher order backward shift operators are defined in similar manner as follows E-2f(x)= E-1(E-1f(x))= E-1(f(x-h)= f(x-2h)= yx-2h E-3f(x)= f(x-3h) . . E-kf(x)= f(x-kh)
  • 14. Forward difference operator (∆) : The first order forward difference operator of a function f(x) with increment h in x is given by ∆f(x)=f(x+h)-f(x) (or) ∆fk =fk+1-fk ; k=0,1,2……… ∆2f(x)= ∆[∆f(x)]= ∆[f(x+h)-f(x)]= ∆fk+1- ∆fk ; k=0,1,2………… ……………………………. ……………………………. Relation between E and ∆ : ∆f(x)=f(x+h)-f(x) =Ef(x)-f(x) [Ef(x)=f(x+h)] =(E-1)f(x) ∆=E-1 E=1+ ∆
  • 15. LECTURE-6 ∇ Backward difference operator (nabla ) : The first order backward difference operator of a function ∇ f(x) with increment h in x is given by ∇ f(x)=f(x)-f(x-h) (or) ∇ k =fk+1-fk ; k=0,1,2……… f ∇f(x)= ∇[ f(x)]= ∇ [f(x+h)-f(x)]=∇ fk+1- ∇k ; k=0,1,2………… f ……………………………. ……………………………. Relation between E and nabla : nabla f(x)=f(x+h)-f(x) =Ef(x)-f(x) [Ef(x)=f(x+h)] =(E-1)f(x) nabla=E-1 E=1+ nabla
  • 16. Central difference operator ( δ) : The central difference operator is defined as δf(x)= f(x+h/2)-f(x-h/2) δf(x)= E1/2f(x)-E-1/2f(x) = [E1/2-E-1/2]f(x) δ= E1/2-E-1/2
  • 17. LECTURE-7 INTERPOLATION : The process of finding a missed value in the given table values of X, Y. FINITE DIFFERENCES : We have three finite differences 1. Forward Difference 2. Backward Difference 3. Central Difference
  • 18. RELATIONS BETWEEN THE OPERATORS IDENTITIES: ∇ 1. ∆=E-1 or E=1+ ∆ ∇ 2. = 1- E -1 3. δ = E 1/2 – E -1/2 4. µ= ½∇ 1/2-E-1/2) (E ∇ 5. ∆=E = ∇E= δE1/2 6. (1+ ∆)(1- )=1
  • 19. LECTURE-8,9 Newtons Forward interpolation formula : y=f(x)=f(x0+ph)= y0 + p∆y0 + p(p-1)/2! ∆2y0 + p(p-1)(p- 2)/3! ∆3y0+…….. ………………+p(p-1)(p2) …… [p- (n-1)]/n! ∆ny0 . Newtons Backward interpolatin formula : y=f(x)=f(xn+ph)= yn + p∆yn + p(p+1)/2! ∆2yn + p(p+1) (p+2)/3! ∆3yn+…….. ………………+p(p+1)(p+2) …… [p+(n-1)]/n! ∆nyn .
  • 20. LECTURE-10,11 GAUSS INTERPOLATION The Guass forward interpolation is given by yp = yo + p ∆y0+p(p-1)/2! ∆2y-1 +(p+1)p(p-1)/3! ∆3y-1+(p+1)p(p- 1)(p-2)/4! ∆4y-2+…… The Guass backward interpolation is given by yp = yo + p ∆y-1+p(p+1)/2! ∆2y-1 +(p+1)p(p-1)/3! ∆3y-2+ (p+2)(p+1)p(p-1)/4! ∆4y-2+……
  • 21. LECTURE-12 INTERPOLATIN WITH UNEQUAL INTERVALS: The various interpolation formulae Newton’s forward formula, Newton’s backward formula possess can be applied only to equal spaced values of argument. It is therefore, desirable to develop interpolation formula for unequally spaced values of x. We use Lagrange’s interpolation formula.
  • 22. The Lagrange’s interpolation formula is given by Y = (X-X1)(X-X2)……..(X-Xn) Y0 + (X0-X1)(X0-X2)……..(X0-Xn) (X-X0)(X-X2)……..(X-Xn) Y1 +………………….. (X1-X0)(X1-X2)……..(X1-Xn) (X-X0)(X-X1)……..(X-Xn-1) Yn + (Xn-X0)(Xn-X1)……..(Xn-Xn-1)