International Journal of Technology and Emerging Research
DOI: 10.64823/ijter.2605033
An equation involving derivatives of one or more dependent variable with respect to one or more independent variables is called differential equation[1].The second order linear differential equations with constant coefficient which is non homogeneous have the general form: where are constants and is any non zero function . A differential equation with constant coefficients is said to be the one when the dependent variable and its derivatives occur in it in the first degree and are not multiplied together[2].When f(x) becomes zero then it becomes the corresponding homogeneous form of the non homogeneous equation .It has several applications in real world phenomena across physics , engineering, and economics .The comparative study of analytical methods as well as analytic and numeric methods are already has been discussed but this paper focuses on the edge or failure cases and the limitations of the two methods that is method of undetermined coefficients and variation of parameter.
In this section , first we discuss the working method of both the methods that is the method of undetermined coefficients and variation of parameters. The general form of second order linear differential equation with constant coefficients is given by:
The general solution is always the sum of complementary solution(obtained by the corresponding homogeneous part of the given non homogeneous equation) and particular solution(on which the method primarily focuses) For Complementary Solution: Solve the corresponding homogeneous equation by using characteristic equation method, which is foundational method for both the methods.
We formulate the initial guess depending upon the nature of the forcing function .Compare the complementary solution with initial guess, if it do not overlaps with complementary solution then initial guess becomes the particular solution. But if it overlaps with complementary multiply it with suitable power of x to establish linear independence. Substitute the modified initial guess solution into the given differential equation. Equating the coefficients of like term leads to an algebraic set of equation that enables to obtain the unknown constant and hence the particular solution.
Variation of parameters is a general method for finding the particular solution of non-homogeneous linear differential equations with constant coefficients. This method can be applied to non-homogeneous equations even when the forcing function is not simple enough to apply the undetermined coefficient method.
Assume that and are the two linearly independent solutions of the corresponding homogeneous equation. The particular solution of the non-homogeneous differential equation is written as
To simplify calculations, the auxiliary equations: and are used. They form a system of simultaneous linear algebraic equations inand .Solving the above system yields and . Using the Wronskian determinant,
W(y1 , y2) =
the expressions for and are derived. Then, the resulting expressions are integrated to find and .
Substituting the expressions for and in the assumed solution formula gives the particular solution. Hence, this method involves finding integrals.
In conclusion, this is a general approach to finding the particular solution of non-homogeneous differential equations; however, it involves complex integrals.
Applicability of this method only depends upon the nature of the forcing functions which means it is applicable to a set of functions whose derivate is same as the function itself as polynomials , exponential functions and trigonometric functions. This method is not applicable to all trigonometric functions but only to and .To show the limitations of the method ,consider the case where the forcing function, . Following are the reasons possible due to which the method limits itself for :
As the method of undetermined coefficients is applicable for the forcing function which involves and so we can write. But it voilates the condition that the forcing function should belongs to a finite dimensional family of functions and also derivatives belong to the same family.
For example ,forcing functions like , polynomials, and exponential satisfy this property and the method of undetermined coefficients is applicable on these forcing functions.
The derivatives of produces infinitely many forms and it does not belong the same family to belongs. But in case of and this is not the case.
which can be written as finite linear combination. But in case of , this is not possible, because
,
and so on.
With the successive derivatives ,which involves the powers of and . Hence, cannot be expressed as linear combination of its derivatives.
If we keep in mind the perspective of power series expansions , functions like and have maclaurin series that converge for all real values and show predictable derivative behavior . But in contrast, series of has a limited radius of convergence and leads to more complex derivatives.
There is no singularities in and which is clear from their respective series:
+……..
-……..
+……
The maclaurin series converges of for. The series has finite radius of convergence and derivatives generate increasingly complex expressions.
This method needs the wronskian of the complementary solution and the wronskian should be non-zero and if the wronskian vanishes then the method fails completely as variation of parameters require linearly independent solutions. But it always works for linear differential equation with constant coefficients. For linear differential equation with variable coefficients, singularities can appear and in those cases wronskian vanishes and the method fails completely.
For example: The complementary solution is
W(y1 , y2) =
W(y1 ,y2) =
W(y1 ,y2) = x·1 −x·1 = 0
We can see that here the wronskian vanishes and hence the method of variation of parameters become inapplicable in case of linear differential equation with variable coefficients.
Method of variation of parameter involves integration as an important step, and sometimes the integration becomes complicated. The integral requires more time and the computational efficiency is less. This method does not fails technically but surely has limitation as compared to other methods.
For example, , the complementary solution is Now integrals for method of variation of parameters;
W(y1 , y2) =
W(y1 , y2) =
W(y1 , y2) = -2 ≠ 0 and hence,
which is solvable but again it will take more time to solve as integration involves the method of integration by parts.
Finding complementary solution is the first step to find the complete solution of the linear differential equation with constant coefficients. If the corresponding homogeneous equation cannot be solved then we cannot even start the method of variation of parameters as this method lacks the initial structure.
Method of variation works almost for every function but sometimes it provides a solution with non elementary integral such as error function is not elementary.
For example:,then the complementary solutions are and W=1.
&
On solving these integrals, integrals cannot be expressed in elementary form but give
rise to the error function .
This method is only applicable for linear differential equations as it depends upon the linear combination of complementary solution and the superposition principle does not hold for non linear differential equations and thus the method fails for non linear equations.
For example: y′′ +y2 = x, here y2 represents the non linear term and hence there is no complementary solution . Thus variation of parameters cannot be applied to it.
Method of undetermined coefficients and method of variation of parameters differs from each other in many aspects but both the methods limits itself at one common point that is dependency on complementary solution to get the complete solution. Following are the few aspects in which both the methods differs from each other which helps in the applicability of both the methods in different situations:
Aspect | Method of undetermined coefficients | Method of variation of parameters |
Forcing Function | Applicable to some limited functions such as , polynomials,. | There is no restrictions on forcing functions. |
Computation | No computational complexity as there is no integration involved. | Computational complexity arises due to integrals which cannot expressed as elementary functions. |
Generality | No computational complexity as there is no integration involved. | It can be applied to linear differential equations with constant and variable coefficients. |
Equation type | Linear differential equation with constant coefficients only. | It can be applicable to linear equations with variable coefficients. |
Wronskian | No requirement of wronskian. | Finding a nonzero wronskian is an efficient step. |
Solution Assumption | It requires an initial guess to form solution and hence for complete solution. | No assumed initial guess is required. |
In this paper, we investigated the limitations and inapplicability cases of the Method of undetermined coefficients and variation of parameters. Both the methods have dependence on characteristic equation method for the complementary solution. This analysis shows that method of undetermined coefficients is computationally more efficient than Method of variation of parameters but has a key limitation depending upon the forcing function. On the other hand, Method of variation of parameter provides a more general approach and applicable to wider ranges of the function accompanied with a computational complexity for some integrals that may be complicated or not directly solvable in simpler terms. Thus, neither method is superior to each other, their applicability depends on the need situation. Instead their usefulness depends upon the specific features of the differential equation. The comparative perspective clarifies the functional limits of the two methods but creates a thoughtful approach to solve linear differential equations.