Week 3.5 - Deriving 4th order approximation of a 2nd order derivative using Taylor Table method

Aim: - To derive and write a program for in MATLAB for 4th order approximation for second order derivative by following methods-

1. Central difference
2. Skewed right sided difference
3. Skewed left sided difference

Objective: - 1. To evaluate the second order derivative of the function  $f\left(x\right)=\exp \left(x\right)\cos x$   ,  Using above mentioned order of approximations.

2. To plot and compare the values and errors of the 3 methods derived.

Theory and derivations: -

During solving a CFD problem we may come across partial derivative equation which consists 2nd order derivative. Since due to complexity of the equation we may have to chose numerical approach rather than analytical. But when dealing with numerical approach we try to make the error margin as low as possible.

As the order of approximation get higher, we get higher accuracy. Hence, we are going to derive the three methods of approximation for an analytical function. The methods are following.

1. Central difference: - Here the nodes selected are symmetrical i.e. the data is taken from both sides of point of focus. Using Taylor’s method, we get

                                                $\frac{{\partial }^{2}f}{\partial x^2}=af(i-2)+bf(i-1)+cf\left(i\right)+df(i+1)+ef(i+2)$

 Here there are two nodes taken from both side of the point of focus i.e. f(i).

(NOTE: - To select the number of nodes in consideration, we use following expression:

                                        N=p + q -1                                      for central differencing

                                       N = p + q                                          for skewed differencing

  Here N is no. of nodes, p is order of derivative and q is order of approximation.)

 Taylor’s table for Central difference:

This table transform into matrix of type AX=B

$\left[\begin{array}{ccccc}1& 1& 1& 1& 1\\ -2& -1& 0& 1& 2\\ \frac{4}{2}& \frac{1}{2}& 0& \frac{1}{2}& \frac{4}{2}\\ 1& 2& 3& 4& 5\\ -\frac{8}{6}& -\frac{1}{6}& 0& \frac{1}{6}& \frac{8}{6}\\ \frac{16}{24}& \frac{1}{24}& 0& \frac{1}{24}& \frac{16}{24}\end{array}\right]$    *     $\left[\begin{array}{c}a\\ b\\ c\\ d\\ e\end{array}\right]$      =      $\left[\begin{array}{c}0\\ 0\\ 1\\ 0\\ 0\end{array}\right]$            on further solving we get the values of the unknown

i.e.   Values =      a =   -0.0833              b= 1.3333            c= -2.5000            d= 1.3333          e= -0.0833

These coefficients will further used in code to get the value of derivative.

1. Skewed right sided difference: - When the data point of the left nodes are not available (at initial boundary conditions) then we have to rely on the available data set.

                                                               $\frac{{\partial }^{2}f}{\partial x^2}=af\left(i\right)+bf(i+1)+cf(i+2)+df(i+3)+ef(i+4)+ff(i+5)$

 Taylor’s table for Skewed right sided difference:

This table transform into matrix of type AX=B:

 $\left[\begin{array}{cccccc}1& 1& 1& 1& 1& 1\\ 0& 1& 2& 3& 4& 5\\ 0& \frac{1}{2}& 2& \frac{9}{2}& \frac{16}{2}& \frac{25}{2}\\ 0& \frac{1}{6}& \frac{8}{6}& \frac{27}{6}& \frac{64}{6}& \frac{125}{6}\\ 0& \frac{1}{24}& \frac{16}{24}& \frac{81}{24}& \frac{256}{24}& \frac{625}{24}\\ 0& \frac{1}{120}& \frac{32}{120}& \frac{243}{120}& \frac{1024}{120}& \frac{3125}{120}\end{array}\right]$   *  $\left[\begin{array}{c}a\\ b\\ c\\ d\\ e\\ f\end{array}\right]$         =    $\left[\begin{array}{c}0\\ 0\\ 1\\ 0\\ 0\\ 0\end{array}\right]$     on further solving we get the values of the

unknown i.e.     Values =      a = 3.7500          b= -12.8333         c=     17.8333

                                         d=    -13.0000      e= 5.0833             f=   -0.8333              

 These coefficients will further used in code to get the value of derivative.

1. Skewed left sided difference: - When the data point of the right nodes are not available (at boundary conditions) then we have to rely on the available data set.

                                                           $\frac{{\partial }^{2}f}{\partial x^2}=af(i-5)+bf(i-4)+cf(i-3)+df(i-2)+ef(i-1)+ff\left(i\right)$

 Taylor’s table for Skewed right sided difference:

This table transform into matrix of type AX=B:

  $\left[\begin{array}{cccccc}1& 1& 1& 1& 1& 1\\ -5& -4& -3& -2& -1& 0\\ \frac{25}{2}& \frac{16}{2}& \frac{9}{2}& 2& \frac{1}{2}& 0\\ -\frac{125}{6}& -\frac{64}{6}& -\frac{27}{6}& -\frac{8}{6}& -\frac{1}{6}& 0\\ \frac{625}{24}& \frac{256}{24}& \frac{81}{24}& \frac{16}{24}& \frac{1}{24}& 0\\ -\frac{3125}{120}& -\frac{1024}{120}& -\frac{243}{120}& -\frac{32}{120}& -\frac{1}{120}& 0\end{array}\right]$  *    $\left[\begin{array}{c}a\\ b\\ c\\ d\\ e\\ f\end{array}\right]$           =   $\left[\begin{array}{c}0\\ 0\\ 1\\ 0\\ 0\\ 0\end{array}\right]$      on further solving we get the values of the

unknown i.e.     Values =      a = -0.8333              b= 5.0833          c=13.0000

                                          d= 17.8333      e= -12.8333           f= 3.7500      

These coefficients will further used in code to get the value of derivative.

MATLAB code: -

clear all
close all
clc

%analytical function defination and value assignment
x=pi/3;
dx=linspace(pi/10,pi/1000,100);
f=@(x)(exp(x)*cos(x));
g=@(x)(-2*exp(x)*sin(x));
d2f=g(x);
func=f(x);



%for central difference scheme 
%coefficients taken from taylor's table
P = [1 1 1 1 1
    -2 -1 0 1 2
    4/2 1/2 0 1/2 4/2
    -8/6 -1/6 0 1/6 8/6
    16/24 1/24 0 1/24 16/24];
    
   
    
    
C=[0;0;1;0;0];
%as P*a=C i.e. a=inverse(P)*c(fastest way to getby '\')

cf1=P\C;

%for right skewwd differnce scheme
Q= [1 1 1 1 1 1
    0 1 2 3 4 5
    0 1/2 2 9/2 16/2 25/2
    0 1/6 8/6 27/6 64/6 125/6
    0 1/24 16/24 81/24 256/24 625/24
    0 1/120 32/120 243/120 1024/120 3125/120];
D=[0;0;1;0;0;0];
%as Q*b=s i.e. b=inverse(Q)*s(fastest way to getby '\')

cf2=Q\D;

%for right skewwd differnce scheme
R= [1 1 1 1 1 1
    -5 -4 -3 -2 -1 0
    25/2 16/2 9/2 2 1/2 0
    -125/6 -64/6 -27/6 -8/6 -1/6 0
    625/24 256/24 81/24 16/24 1/24 0
    -3125/120 -1024/120 -243/120 -32/120 -1/120 0];
E=[0;0;1;0;0;0];
%as n*b=s i.e. b=inverse(n)*s(fastest way to getby '\')

cf3=R\E;

�lculating values of derivative using CDS RSDC,LSDC
�fining variable size befor using in loop
central_diff=zeros(1,100);
err_central=zeros(1,100);
right_sdiff=zeros(1,100);
err_right=zeros(1,100);
left_sdiff=zeros(1,100);
err_left=zeros(1,100);

for i=1:length(dx)
    �lculating value and error by central difference scheme
    central_diff(i)=(cf1(1)*f(x-2*dx(i))+cf1(2)*f(x-dx(i))+cf1(3)*f(x)+cf1(4)*f(x+dx(i))+cf1(5)*f(x+2*dx(i)))/(dx(i))^2;
    err_central(i)=abs(central_diff(i)-d2f);
    
    �lculating value and error by right skewed difference scheme
    right_sdiff(i)=(cf2(1)*f(x)+cf2(2)*f(x+dx(i))+cf2(3)*f(x+2*dx(i))+cf2(4)*f(x+3*dx(i))+cf2(5)*f(x+4*dx(i))+cf2(6)*f(x+5*dx(i)))/(dx(i))^2;
    err_right(i)=abs(right_sdiff(i)-d2f);
    
    �lculating value and error by left skewed difference scheme
   left_sdiff(i)=(cf3(1)*f(x-5*dx(i))+cf3(2)*f(x-4*dx(i))+cf3(3)*f(x-3*dx(i))+cf3(4)*f(x-2*dx(i))+cf3(5)*f(x-dx(i))+cf3(6)*f(x))/(dx(i))^2;
   err_left(i)=abs(left_sdiff(i)-d2f); 

end

%plotting values of derivative
subplot(2,1,1)
hold on
fplot(d2f,'--')
xlim([-0.05 0.35]);
plot(dx,central_diff,'linewidth',2,'color','r');
plot(dx,right_sdiff,'linewidth',2,'color','b');
plot(dx,left_sdiff,'linewidth',2,'color','g');
legend('analytical value at x=pi/3','central diff.','right skewed diff.','left skewed diff.','location','best')
xlabel('Grid siza(dx)');
ylabel('Value');
title('Comparision b\w value of derivative calculated by diff. order of approximation') 
hold off

%plotting errors in approximation of derivative
subplot(2,1,2)
loglog(dx,err_central,'linewidth',2,'color','r');
hold on
xlim([.002 0.4]);
loglog(dx,err_right,'linewidth',2,'color','b');
loglog(dx,err_left,'linewidth',2,'color','g');
legend('central diff.','right skewed diff.','left skewed diff.','location','best')
xlabel('Grid siza(dx)');
ylabel('Absolute error');
title('Comparision b/w 4th order approximation method for error in calculating d2f/dx2 ');