Second Order Linear Differential Equation

The second-order linear differential equation involves the second derivative of function. It is crucial in many areas of physics and engineering, such as mechanical vibrations, electrical circuits, and heat conduction. The general form of a second-order linear differential equation is:

a(x) \frac{d^2y}{dx^2} + b(x) \frac{dy}{dx} + c(x) y = g(x)

Types of Second Order Linear Differential Equation

There are two types of second order linear differential equations: Homogeneous Equation, and Non-Homogeneous Equation.

Homogeneous Equation

A homogeneous equation in the context of differential equations can refer to two related but distinct concepts depending on the context: homogeneity in algebraic terms and homogeneity concerning differential equations.

General Form of Equation: These equations are of the form:

A(x)y" + B(x)y' + C(x)y = 0

where y'=(dy/dx) and A(x), B(x) and C(x) are functions of independent variable 'x'. For the purpose of this article we will learn how to solve the equation where all the above three functions are constants.

Properties:(I) Suppose g(x) is a solution of the homogeneous equation. We will prove that 'cg(x)' is also a solution, where c is a constant.

Ag"+Bg'+Cg = 0            (1)
Now, A(cg)" + B(cg)' + Cg 
= cAg" + cBg' + Cg
= c(Ag" + Bg' + Cg)
= c(0)    [From (1)]
= 0

Hence, 'cg(x)' is also a solution.

(II)

Suppose h(x) is also a solution along with g(x).We will prove that 'h(x)+g(x)' is also a solution.

Ag"+Bg'+Cg = 0            (1)
Ah"+Bh'+Ch = 0            (2)
Now, A(h+g)" + B(h+g)' + C(h+g)
= A(h"+g") + B(h'+g') + C(h+g)
= (Ah" + Bh' + Ch) + (Ag" + Bg' + Cg)
= 0 + 0               [From (1) and (2)]
= 0

(III)

From I and II we can say that the general solution of a homogeneous equation is:

'kg(x) + ch(x)'

where 'k' and 'c' are arbitrary constants.

Solving Homogeneous Equations: The basic step is of course is to 'guess' the function which satisfies the equation. But in this case I have done this for you. The first step involves assuming, rx where 'r' is some real number(may be complex also as we will see!). So,

 Ar2erx + Berxr + Cerx = 0
(erx)(Ar2 + Br  + C) = 0    [Taking erx common from all the terms]
Ar2 + Br + C = 0    [As erx cannot be zero]

Based on above equation 3 cases arise:

(I)

If both roots are real, say r

₁

and r

₂

, then the solution will be

f(x) = c1(er1x) + c2(er2x)

(II)

If the roots are complex then they must be conjugate as the coefficients of the quadratic equation are real.

Let r1 = a1 + ia2, r2 = a1 - ia2 

where 'i' is iota, i.e., 'i' is square root of (-1). So, the general solution will be:

f(x) = c1er1x + c2er2x 

which if you will simplify will look like:

f(x) = ea1x(k1cos(a2x) + k2sin(a2x)) 

[ I hope you know e

^it

= cos(t) + isin(t), Also k

₁

and k

₂

are different from c

₁

and c

₂

]. I also encourage you to find the relation between k

₁

and k

₂

and c

₁

and c

₂

.

(III)

If the roots are repeated, then y = ce

^rx

is not the general solution but only a particular solution. So what to do? Hence again assume,

y = p(x)erx 

where 'r' is the root that you got in the above equation. By solving you will get that

p(x)=c1x + c2 

Hence your general solution will look like,

y = (c1x + c2)erx 

These examples will give you clarity:

Example-1:

y" + 5y' + 6y = 0

Assume y = e

^rx

.Putting this in the equation, we finally get:

r2 + 5r + 6 = 0
(r+2)(r+3) = 0
r = (-2)  OR  r = (-3)

So,

r1 = (-2) and r2 = (-3) 

Since both are real the general solution will be:

y = c1e(-2x) + c2e(-3x)

Example-2:

y" + y' + y = 0

Again assume y = r

^rx

and solve for 'r'. Your 'r' will look something like this:

r1 = (-1/2) + i(-sqrt(3)/2)   
and  r2 = (-1/2) - i(-sqrt(3)/2)
So, 
a1 = (-1/2)  
and  a2 = (sqrt(3)/2)

Hence the general solution will look like this:

y = e(-x/2)(c1cos(x√(3)/2) + c2sin(x√(3)/2))

Example-3:

y" + 4y' + 4y = 0

Again assume y = r

^rx

and solve for 'r'. The 'particular solution will be:

y = ce2x

Assume

y = p(x)e

^2x

.Putting it in the differential equation will give you:

p" = 0 which implies
p'= c2 which again implies
p = c1x + c2

Hence the general solution will be:

y = (c1x + c2)e2x