Solving the Second Order Linear Differential Equation using the Power Series Method
The Power Series Method requires no introduction. It is one of the most powerful methods of analyzing functions or solving differential equations. Solving this differential equation using the power series will circumnavigate the use of complex numbers thus providing a much more ''physical" understanding of the concepts involved. They also provide insight about an important and alternate definition of the sine and the cosine functions, the so called "Taylor Series" expansion of the sine and the cosine functions. They show how sinusoids are related to infinite series also. So, the overall impression of the Power Series Method is that it is a versatile and a powerful method for solving differential equations.
We always strive to explain nature and its phenomena in a deterministic and a well defined, logical manner. We use mathematics as the guardrail of our understanding to achieve this endeavor. To explain the various natural laws mathematically, differential equation arises and so we have developed various methods to solve the same. One the most interesting phenomena that has received ample well deserved mathematical attention is oscillation, more precisely, sinusoidal oscillations. We shall see how they arise as a consequence of simple physical laws and shall use one of the methods to study them.
The most basic form of oscillation, the Simple Harmonic Motion arises from simple systems such as a spring and a mass on a frictionless suitable support. The most empirical law dealing with such systems is the Hooke's Law which states that the restoring force exerted by a stretched spring is directly proportional to the elongation or the change in length of the spring.
Expressing this law mathematically-
where 'm' is the mass, 'x' is the position of the mass, 'k' is the spring constant and 't' is the time. The left-hand side of the expression originates from Newton's 2nd Law, the right-hand side from Hooke's Law. The negative sign indicates that the force is restoring in nature.That's all the differentiation we had to do. Now, we equate the left and the right sides of the equation.

Taking the coefficients common-
The upper series is the Taylor Series Expansion of the Cosine Function. The lower one is the Expansion of the Sine Function. Thus Trigonometric Functions can be expressed as an infinite summation of polynomials with appropriate coefficients. This also shows the oscillatory nature of the solution to the Differential Equation being solved.








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