Analyzing the Setup
Welcome, fellow traveler on the path to JEE mastery. Today, we are not just solving a differential equation; we are uncovering the hidden rhythm of a physical system.
When you look at the equation
do not see just symbols and variables. See a system that is being pushed by an external force—the cosine wave—while simultaneously trying to settle down, represented by the 12y term. This is the essence of a first-order linear differential equation, and it is a beautiful piece of mathematical architecture.
Phase 1
The Integrating Factor—Our Magic Key
Every great journey begins with identifying the terrain. Our equation is in the standard form
Here, P(x)=12 and Q(x)=cos(12πx).
The integrating factor, or IF, is the key that unlocks this door. It is defined as e∫P(x)dx. Substituting our constant P(x)=12, we get
This e12x is the 'multiplier' that will transform our complex equation into a simple derivative of a product. When we multiply the entire equation by e12x, the left side becomes the derivative of y⋅e12x. It is elegant, isn't it? The complexity collapses into a single, manageable derivative.
Phase 2
The Dance of Integration
Now, we face the heart of the problem: ∫e12xcos(12πx)dx. This is where many students feel a shiver of fear. But fear not!
We have a standard formula for this exact integral:
∫eaxcos(bx)dx=a2+b2eax[acos(bx)+bsin(bx)]
By identifying a=12 and b=12π, we can bypass the tedious process of integration by parts. Substituting these values, we obtain the integral. It is a long expression, yes, but it is just a sequence of algebraic steps. We are simply evaluating the interaction between the exponential growth and the trigonometric oscillation.
Phase 3
Finding the Particular Solution
After integrating, we have our general solution:
y(x)=K[12cos(12πx)+12πsin(12πx)]+Ce−12x
But we are not finished. We have an initial condition: y(0)=0. This is our anchor.
By plugging in x=0, we find that C=−12K. This constant C is the 'memory' of the system—it represents the initial state that influences the future trajectory. With C determined, we have the complete, particular solution. Look at it closely. It is a combination of a steady-state oscillation and a transient decay.
Phase 4
The Qualitative Revelation
Finally, let us analyze the behavior. Why is it not periodic? Because of the term Ce−12x.
As x grows, this term dies away, but it is never zero for finite x. It prevents the function from ever repeating its values exactly. Why is it not monotonic? Because the sine and cosine terms force the function to oscillate.
And the most thrilling part? As x→∞, the transient term vanishes, and the function becomes a pure sine wave. This means that for any horizontal line y=β within the amplitude of this wave, the curve will cross it infinitely many times. You have just analyzed the long-term stability of a dynamic system. You have looked into the heart of the equation and understood its soul. Keep this intuition, and no differential equation will ever intimidate you again.