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# Numerical approximation for the solution of linear sixth order boundary value problems by cubic B-spline

*Advances in Difference Equations*
**volumeÂ 2019**, ArticleÂ number:Â 492 (2019)

## Abstract

In the current paper, authors proposed a computational model based on the cubic B-spline method to solve linear 6th order BVPs arising in astrophysics. The prescribed method transforms the boundary problem to a system of linear equations. The algorithm we are going to develop in this paper is not only simply the approximation solution of the 6th order BVPs using cubic B-spline, but it also describes the estimated derivatives of 1st order to 6th order of the analytic solution at the same time. This novel technique has lesser computational cost than numerous other techniques and is second order convergent. To show the efficiency of the proposed method, four numerical examples have been tested. The results are described using error tables and graphs and are compared with the results existing in the literature.

## 1 Introduction

The applications of boundary value problems (BVPs) are almost unlimited, and they play an important role in all the branches of science, engineering, and technology. They are applied to model many systems in several fields of science and engineering. In recent years, there has been significant advancement in solving problems related to a system of linear and nonlinear partial and ordinary differential equations concerning boundary conditions (BC). Two point nonlinear BVPs often cannot be solved by analytical techniques. With cumulative interest in finding solutions to linear/nonlinear BVPs has come an increasing requirement for solution techniques. In the present paper, we will study the algebraic results of the following linear 6th order BVP:

with boundary conditions

where \(\alpha_{0}\), \(\alpha_{1}\), \(\alpha_{2}\) and \(\beta_{0}\), \(\beta_{1}\), \(\beta_{2}\) are given real constants, (\(a_{i}(z)\); \(i = 1, 2,\ldots, 6\)), and *f* is continuous on the given interval \([a, b]\).

A variety of numerical methods [1, 2, 4, 5, 8, 9, 11, 12, 16, 31] have been presented to solve BVPs problem, e.g., global phase-integral methods, shooting methods, sinc-Galerkin methods, splines methods, finite difference methods, finite element methods, variational iteration, the collocation methods, and other numerical techniques.

In [23], a variation of parameter technique was used for solving sixth order boundary value problems. Perturbation method for nonlinear engineering problems was specified in [24]. Homotopy perturbation technique for solving linear and nonlinear sixth order boundary value problems was described in [25]. In [26], algebraic results of 6th order BVPs were originated by applying non-polynomial spline method. Neural networks mimic the learning procedure of the human brain in order to excerpt designs from ancient data as defined in [27]. These networks are rehabilitated into 6th order boundary value problems and then resolved by diverse approaches for precise and estimated results. Numerical methods for sixth order boundary value problems were discussed in [32]. In [33], the authors established a family of algebraic procedures for the solutions of 6th order boundary value problems with application to Benard layer eigenvalue problems. Numerical solutions of fifth and sixth order nonlinear boundary value problems by Daftardarâ€“Jafari method were found in [34]. Wazwaz in [35] used decomposition and modified domain decomposition approaches to examine the solution of 6th order boundary value problems.

Discrete methods, e.g., Adomian decomposition, shooting, homotopy-perturbation, finite differences, and variational-iterative technique, only obtained the discrete approximate values of dependent variable \(y(x)\). We require further data processing procedures to acquire exact fitted curve to data. For the case of spline approximation or interpolation approaches the dependent variable \(y(x)\) is supposed to be piecewise polynomial which involves at least piecewise higher order derivatives of the function \(f(x, y, y')\). To overcome these shortcomings, several researchers [3, 6, 7, 10, 13,14,15, 17,18,19,20,21,22, 28,29,30] introduced the spline/subdivision based methods for the solution of BVPs. However, the higher order problems have not been solved by spline/subdivision techniques. This motivates us to solve 6th order boundary value problems by spline. This paper does not only introduce a numerical approximation based on cubic B-spline for the solution of linear 6th order BVPs, but it also describes the estimated derivatives of 1st order to 6th order of the analytic solution at the same time. This novel technique has lesser computational cost than numerous other techniques and is second order convergent.

## 2 Materials and methods

In this section the fundamentals of cubic B-spline and its application on sixth order BVP are discussed in detail. When we contrasted the cubic B-spline method with the other methods, we came to know that our results are well accepted. Moreover, this method is second order convergent and has comparatively lesser computational cost. Furthermore, solving with cubic B-spline method, we also can acquire the estimated derivative values of \({w} ( z )\), \({w}'(z)\), \({w}''(z)\), \({w}^{(3)} ( z )\), \({w}^{(4)} ( z )\), \({w}^{(5)}(z)\), and \(w^{(6)} ( z )\) at the knots, which is the main advantage of the cubic B-spline method, as other methods are unable to obtain these values. In the current paper, we will use cubic B-spline to resolve 6th order BVP.

### 2.1 Fundamentals of cubic B-splines

The assumed choice of independent variable is \([a, b]\). For an interval \(\varOmega = [a, b]\), we divide it into *n* subintervals \(\varOmega _{i} = [z _{i}, z_{i+1}]\) (\(i =0, 1,\ldots , n -1\)) by the equidistant knots, and for this range we select equidistant points assumed by

i.e.,

Let us describe \(S_{3} ( \varOmega ) = \{ p' ( t ) \in C^{2} [ a,b ] \}\) such that \(p' ( t )\) decreases to cubic polynomial on separately sub-interval \(( z_{i}, {z}_{i + 1} )\). The basis function is defined as

for \(i = 2, 3, 4,\ldots, n - 2\). Since to each \(B_{i} ( {z} )\) is similarly a piecewise cubic with knots at *Î©*, collectively \(B_{i} ( z ) \in S_{3}(\varOmega )\). Let \(\varPsi = \{ B_{ - 1},B_{0},B_{1},\ldots,B_{n + 1}\}\) and let \(B_{3}(\varOmega ) = \operatorname{span} \varPsi\). The functions in *Î¨* are linearly independent on \([a, b]\), thus \(B_{3} ( \varOmega )\) is \((n + 3)\)-dimensional and \(B_{3} ( \varOmega ) = S_{3} ( \varOmega )\). Let \(s ( z )\) be the cubic B-spline interpolating function at the nodal points and \(s ( z ) \in B_{3} ( \varOmega )\). Then \(s ( z )\) can be written as

The values of \(B_{i} ( z )\), \(B_{i}^{\prime} ( z )\), and \(B_{i}^{\prime\prime} ( z )\) at the knots are listed in TableÂ 1.

Consequently, now for an assumed function \(w ( z )\) there happened to be a distinctive cubic B-spline \(s ( z ) = \sum_{i = - 1}^{n + 1} l_{i}B_{i} ( z )\) satisfying the interpolating conditions:

and \(s' ( a ) = w' ( a )\), \(s' ( b ) = w' ( b )\). Let \(m_{i} = s' ( z_{i} )\) and \(M_{i} = s^{\prime\prime} ( z_{i} )\), then from [15] we have

\(M_{i}\) can be used to calculate the numerical difference formulas for \(w^{(3)} ( z_{i} )\), \({w}^{(4)}(z_{i})\) where \(i = 1, 2,\ldots, n - 1\) and \(w^{(5)}(z_{i})\), \({w}^{(6)}(z_{i})\) where \(i = 2, 3,\ldots, n - 2\) as follows, wherever the errors are acquired by the Taylor series expansion

Since \(s ( z' ) = \sum_{i = - 1}^{n + 1} l_{i}B_{i} ( z' )\), by means of TableÂ 1 and beyond equations, we get estimate values of \({w} ( z )\), \({w}'(z)\), \({w}''(z)\), \({w}^{(3)} ( z )\), \({w}^{(4)} ( z )\), \({w}^{(5)}(z)\), and \(w^{(6)} ( z )\) as

and following the above, we have the Taylor series expansion for \(w^{(6)} ( z )\) at the selected collocation points with central difference as follows:

Using Eq.Â (6), we can have

Using the above two equations and Eq.Â (6) in Eq.Â (9), we have

As \(M_{i} = \frac{l_{i + 1} - 2l_{i} + l_{i - 1}}{h^{2}}\), so we can conclude

Using the above equations, we have

Simplifying

Neglecting the error order, we have

### 2.2 Cubic B-spline solutions of sixth order BVP

Let \(w(z) = s ( z ) = \sum_{i = - 1}^{n + 1} l_{i}B_{i} ( z )\) be the approximate solution of sixth order BVP

with boundary conditions

where \(\alpha_{0}\), \(\alpha_{1}\), \(\alpha_{2}\) and \(\beta_{0}\), \(\beta_{1}\), \(\beta_{2}\) are given real constants (\(a_{i}(z)\); \(i = 1, 2,\ldots, 6\)) and *f* is continuous on the given interval \([a, b]\).

Using Eqs.Â (8) and (10) in Eq.Â (11), we have

Simplifying

By solving Eq.Â (12) we will have a linear system of \((n - 3)\) linear equations \(( i = 2, 3,\ldots, n - 2 )\) with \((n + 3)\) unknowns \(l_{i}\), where \(i = - 1,0,1,\ldots,n + 1 \), so six more equations are desirable. By the boundary conditions at \(z = a\), we get

Similarly, for \(z = b\),

The approximate solution \(w(z) = s ( z ) = \sum_{i = - 1}^{n + 1} l_{i}B_{i} ( z )\) is attained by resolving the above system of \((n+3)\) linear equations in \((n+3)\) unknowns using the above set of Eqs.Â (12)â€“(14).

## 3 Results and discussion

In the numerical section, we have solved four examples to show the efficiency of cubic B-spline method. Obviously, the results of our method are very encouraging because this method signifies the fastest convergence as well as an incredibly low error.

### Problem 1

subject to

The precise solution is \(w ( z ) = (1 - z) e^{z}\). Algebraic outcomes for this problem are presented in TableÂ 2 for \(h= \frac{1}{10}\) and TableÂ 3 for \(h= \frac{1}{5}\) respectively. The graphical comparison of absolute errors at \(h= \frac{1}{10}\) and \(h= \frac{1}{5}\) is demonstrated in Figs.Â 1 and 2 respectively.

At \(h= \frac{1}{10}\) we will have unknowns \(l _{i}\) where \(i = -1, 0, 1, \dots, n+1 \). At \(n=10\) we will have seven equations from Eq.Â (12), three equations from Eq.Â (13), three equations from Eq.Â (14), so in total we will have thirteen equations and thirteen unknowns. The values of thirteen unknowns \(l _{i}\) where \(i = -1, 0, 1, \dots, 11 \) are

At \(h= \frac{1}{5}\) we will have unknowns \(l _{i}\) where \(i = -1, 0, 1, \dots, n+1 \). At \(n = 5\) we will have two equations from Eq.Â (12), three equations from Eq.Â (13), three equations from Eq.Â (14), so in total we will have eight equations and eight unknowns. The values of eight unknowns \(l _{i}\) where \(i = -1, 0, 1, \dots, 6 \) are

The results of [9] for Problem 1 is demonstrated as follows in TableÂ 4, and obviously our results are encouraging.

Solving with cubic B-spline method, we also can acquire the estimated derivative at the knots, which is described in TableÂ 5, which is the main advantage of cubic B-spline method, as other methods are unable to obtain these values.

### Problem 2

subject to

The exact solution is \(w ( z ) = {z} (1 - z) e^{z}\). Algebraic outcomes for this problem are presented in TableÂ 6 for \(h= \frac{1}{10}\) and TableÂ 7 for \(h= \frac{1}{5}\) respectively. The graphical comparison of absolute errors at \(h= \frac{1}{10}\) and \(h= \frac{1}{5}\) is demonstrated in Fig.Â 3.

At \(h= \frac{1}{10}\) we will have unknowns \(l _{i}\) where \(i = -1, 0, 1, \dots, n+1 \). At \(n=10\) we will have seven equations from Eq.Â (12), three equations from Eq.Â (13), three equations from Eq.Â (14), so in total we will have thirteen equations and thirteen unknowns. The values of thirteen unknowns \(l _{i}\) where \(i = -1, 0, 1, \dots, 11 \) are

At \(h= \frac{1}{5}\) we will have unknowns \(l _{i}\) where \(i = -1, 0, 1, \dots, n+1 \). At \(n=5\) we will have two equations from Eq.Â (12), three equations from Eq.Â (13), three equations from Eq.Â (14), so in total we will have eight equations and eight unknowns. The values of eight unknowns \(l _{i}\) where \(i = -1, 0, 1, \dots, 6 \) are

The maximum absolute errors corresponding to Problem 2 in [30] are demonstrated in TableÂ 8, and obviously our results are encouraging.

Solving with cubic B-spline method, we also can acquire the estimated derivative at the knots, which is described in TableÂ 9, which is the main advantage of cubic B-spline method, as other methods are unable to obtain these values.

### Problem 3

subject to

The exact solution is \(w ( z ) = (z)^{3} (1 - z)^{3}\). Algebraic outcomes for this problem are presented in TableÂ 10 for \(h= \frac{1}{10}\) and TableÂ 11 for \(h= \frac{1}{5}\) respectively. The graphical comparison of absolute errors at \(h= \frac{1}{10}\) and \(h= \frac{1}{5}\) is demonstrated in Fig.Â 4.

At \(h= \frac{1}{10}\) we will have unknowns \(l _{i}\) where \(i = -1, 0, 1, \dots, n+1 \). At \(n=10\) we will have seven equations from Eq.Â (12), three equations from Eq.Â (13), three equations from Eq.Â (14), so in total we will have thirteen equations and thirteen unknowns. The values of thirteen unknowns \(l _{i}\) where \(i = -1, 0, 1, \dots, 11 \) are

At \(h= \frac{1}{5}\) we will have unknowns \(l _{i}\) where \(i = -1, 0, 1, \dots, n+1 \). At \(n=5\) we will have two equations from Eq.Â (12), three equations from Eq.Â (13), three equations from Eq.Â (14), so in total we will have eight equations and eight unknowns. The values of eight unknowns \(l _{i}\) where \(i = -1, 0, 1, \dots, 6 \) are

The results of [9] for Problem 3 are demonstrated in TableÂ 12 and obviously our results are encouraging.

Solving with Cubic B-spline method, we also can acquire the estimated derivative at the knots, which is described in TableÂ 13, which is the main advantage of cubic B-spline method, as other methods are unable to obtain these values.

### Problem 4

subject to

The precise solution is \(w ( z ) = \operatorname{Cos} (z) + \operatorname{Sin} (z)\). Algebraic outcomes for this problem are presented in TableÂ 14 for \(h= \frac{1}{10}\) and TableÂ 15 for \(h= \frac{1}{5}\) respectively. The graphical comparison of absolute errors at \(h= \frac{1}{10}\) and \(h= \frac{1}{5}\) is demonstrated in Fig.Â 5.

At \(h= \frac{1}{5}\) we will have unknowns \(l _{i}\) where \(i = -1, 0, 1, \dots, n+1 \). At \(n=5\) we will have two equations from Eq.Â (12), three equations from Eq.Â (13), three equations from Eq.Â (14), so in total we will have eight equations and eight unknowns. The values of eight unknowns \(l _{i}\) where \(i = -1, 0, 1, \dots, 6 \) are as follows.

Solving with cubic B-spline method, we also can acquire the estimated derivative at the knots, which is described in TableÂ 16, which is the main advantage of cubic B-spline method, as other methods are unable to obtain these values.

## 4 Conclusion

The preceding segments demonstrate that the cubic B-spline technique is a sensible tactic to the numerical solution of sixth order BVP. The calculations associated with the examples deliberated above were accomplished by using Matlab R2015a. The algebraic outcomes validate the effectiveness and accurateness of the anticipated scheme. The anticipated algorithm formed a rapidly convergent series. We recommend that the cubic B-spline technique can also be accommodating when we investigate further higher order BVPs. It works soundly for higher order problems and signifies the fastest convergence as well as a notably low error.

## References

Baldwin, P.: Asymptotic estimates of the eigenvalues of a sixth-order boundary-value problem obtained by using global phase-integral methods. Philos. Trans. R. Soc. Lond. A, Math. Phys. Eng. Sci.

**322**(1566), 281â€“305 (1987)Boutayeb, A., Twizell, E.: Numerical methods for the solution of special sixth-order boundary-value problems. Int. J. Comput. Math.

**45**(3â€“4), 207â€“223 (1992)Caglar, H., Caglar, N., Elfaituri, K.: B-spline interpolation compared with finite difference, finite element and finite volume methods which applied to two-point boundary value problems. Appl. Math. Comput.

**175**(1), 72â€“79 (2006)Chandrasekhar, S.: Hydrodynamic and Hydromagnetic Stability. Dover, New York (2013)

Chawla, M., Katti, C.: Finite difference methods for two-point boundary value problems involving high order differential equations. BIT Numer. Math.

**19**(1), 27â€“33 (1979)Dehghan, M., Lakestani, M.: Numerical solution of nonlinear system of second-order boundary value problems using cubic B-spline scaling functions. Int. J. Comput. Math.

**85**(9), 1455â€“1461 (2008)Ejaz, S.T., Mustafa, G., Khan, F.: Subdivision schemes based collocation algorithms for solution of fourth order boundary value problems. Math. Probl. Eng.

**2015**, Article ID 240138 (2015)El-Gamel, M., Cannon, J., Zayed, A.: Sinc-Galerkin method for solving linear sixth-order boundary-value problems. Math. Comput.

**73**(247), 1325â€“1343 (2004)Glatzmaier, G.A.: Numerical simulations of stellar convective dynamos III. At the base of the convection zone. Geophys. Astrophys. Fluid Dyn.

**31**(1â€“2), 137â€“150 (1985)Gupta, Y., Kumar, M.: B-spline method for solution of linear fourth order boundary value problem. Can. J. Comput. Math. Nat. Sci. Eng. Med.

**2**(7), 166â€“169 (2011)Hakeem, A., Rehman, S., Pervaiz, A., Iqbal, M.: Non-polynomial cubic spline approach for numerical approximation of second order linear Kleinâ€“Gordon equation. Pak. J. Sci.

**67**(4), 377â€“382 (2015)He, J.-H.: Variational approach to the sixth-order boundary value problems. Appl. Math. Comput.

**143**(2), 537â€“538 (2003)Kanwal, G., Ghaffar, A., Hafeezullah, M.M., Manan, S.A., Rizwan, M., Rahman, G.: Numerical solution of 2-point boundary value problem by subdivision scheme. Commun. Math. Appl.

**10**(1), 19â€“29 (2019)Khalid, A, Naeem, M.N.: Cubic B-spline solution of nonlinear sixth order boundary value problems. Punjab Univ. J. Math.

**50**(4), 91â€“103 (2018)Khan, A., Sultana, T.: Parametric quintic spline solution for sixth order two point boundary value problems. Filomat

**26**(6), 1233â€“1245 (2012)Kumar, M., Gupta, Y.: Methods for solving singular boundary value problems using splines: a review. J. Appl. Math. Comput.

**32**(1), 265â€“278 (2010)Lang, F.-G., Xu, X.-P.: A new cubic B-spline method for linear fifth order boundary value problems. J. Appl. Math. Comput.

**36**(1), 101â€“116 (2011)Loghmani, G., Ahmadinia, M.: Numerical solution of sixth order boundary value problems with sixth degree B-spline functions. Appl. Math. Comput.

**186**(2), 992â€“999 (2007)Lucas, T.R.: Error bounds for interpolating cubic splines under various end conditions. SIAM J. Numer. Anal.

**11**(3), 569â€“584 (1974)Manan, S.A., Ghaffar, A., Rizwan, M., Rahman, G., Kanwal, G.: A subdivision approach to the approximate solution of 3rd order boundary value problem. Commun. Math. Appl.

**9**(4), 499â€“512 (2018)Mustafa, G., Abbas, M., Ejaz, S.T., Ismail, A.I.M., Khan, F.: A numerical approach based on subdivision schemes for solving non-linear fourth order boundary value problems. J. Comput. Anal. Appl.

**23**(4), 607â€“623 (2017)Mustafa, G., Ejaz, S.T.: Numerical solution of two-point boundary value problems by interpolating subdivision schemes. Abstr. Appl. Anal.

**2014**, Article ID 721314 (2014)Noor, M.A., Mohyud-Din, S.T.: Variational iteration technique for solving linear and nonlinear sixth order boundary value problems. Int. J. Comput. Appl. Math.

**2**, 163â€“172 (2007)Noor, M.A., Mohyud-Din, S.T.: Homotopy perturbation method for solving sixth-order boundary value problems. Comput. Math. Appl.

**55**(12), 2953â€“2972 (2008)Noor, M.A., Noor, K.I., Mohyud-Din, S.T.: Variational iteration method for solving sixth-order boundary value problems. Commun. Nonlinear Sci. Numer. Simul.

**14**(6), 2571â€“2580 (2009)Pervaiz, A., Ahmad, A., Zafar, Z., Ahmad, M.: Numerical solution of sixth order BVPs by applying non-polynomial spline method. Pak. J. Sci.

**66**(2), 110â€“116 (2014)Schalkoff, R.J.: Artificial Neural Networks, vol. 1. McGraw-Hill, New York (1997)

Siddiqi, S.S., Akram, G.: Septic spline solutions of sixth-order boundary value problems. J. Comput. Appl. Math.

**215**(1), 288â€“301 (2008)Siddiqi, S.S., Akram, G., Nazeer, S.: Quintic spline solution of linear sixth-order boundary value problems. Appl. Math. Comput.

**189**(1), 887â€“892 (2007)Tirmizi, I.A., Khan, M.A.: Non-polynomial splines approach to the solution of sixth-order boundary-value problems. Appl. Math. Comput.

**195**(1), 270â€“284 (2008)Toomre, J., Zahn, J.-P., Latour, J., Spiegel, E.: Stellar convection theory. IIâ€”Single-mode study of the second convection zone in an A-type star. Astrophys. J.

**207**, 545â€“563 (1976)Twizell, E.: Numerical methods for sixth-order boundary value problems. In: Numerical Mathematics Singapore 1988, pp.Â 495â€“506. Springer, Berlin (1988)

Twizell, E., Boutayeb, A.: Numerical methods for the solution of special and general sixth-order boundary-value problems, with applications to Benard layer eigenvalue problems. Proc. R. Soc. Lond., Ser. A, Math. Phys. Eng. Sci.

**431**, 433â€“450 (1990)Ullah, I., Khan, H., Rahim, M.T.: Numerical solutions of fifth and sixth order nonlinear boundary value problems by Daftardar Jafari method. J. Comput. Eng.

**2014**, Article ID 286039 (2014)Wazwaz, A.-M.: The numerical solution of sixth-order boundary value problems by the modified decomposition method. Appl. Math. Comput.

**118**(2), 311â€“325 (2001)

### Acknowledgements

The authors are very thankful to the reviewer for comments and suggestions, and this work was supported by the last authorâ€™s (S. Jain) research grant under the SERB Project Number: MTR/2017/000194.

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Khalid, A., Naeem, M.N., Agarwal, P. *et al.* Numerical approximation for the solution of linear sixth order boundary value problems by cubic B-spline.
*Adv Differ Equ* **2019**, 492 (2019). https://doi.org/10.1186/s13662-019-2385-9

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DOI: https://doi.org/10.1186/s13662-019-2385-9

### MSC

- 34K10
- 34K28
- 42A10
- 65D05
- 65D07

### Keywords

- Linear sixth order BVPs
- Numerical approximation
- Cubic B-spline
- Absolute relative error