The Beauty of Limits
A Journey into Calculus
Limits are the heartbeat of calculus. They allow us to peer into the behavior of functions as they approach a point, even when the function itself might be undefined or indeterminate at that exact location.
Today, we are going to tackle a problem that looks intimidating at first glance:
It is a classic JEE Advanced problem that tests not just your algebraic skills, but your ability to see the underlying structure of trigonometric functions.
Phase 1
The Indeterminate Trap
Whenever you face a limit, your first instinct should always be to check the form. Let's substitute x=0 into our expression.
The denominator, x4, clearly approaches 0. In the numerator, we have sin2(πcos40). Since cos0=1, this becomes sin2(π⋅14)=sin2(π)=0.
We have arrived at a 00 indeterminate form. This is our green light to start simplifying.
Phase 2
The Trigonometric Bridge
We have a sin2θ term, which is often difficult to handle directly in a limit. We need to linearize it.
The identity sin2θ=21−cos(2θ) is our best friend here. By setting θ=πcos4x, our expression transforms into:
x→0lim2x41−cos(2πcos4x)
Now, we are dealing with a cosine function, which is much easier to manipulate using standard limits.
Phase 3
The Algebraic Dance
We still have that cos4x inside the cosine. Since we are working with x→0, we want to move toward sine functions, because we know limx→0xsinx=1.
We use the identity cos2x=1−sin2x, which means cos4x=(1−sin2x)2. Expanding this, we get 1−2sin2x+sin4x.
Multiplying by 2π, the argument of our cosine becomes 2π−4πsin2x+2πsin4x.
Here is where the magic happens. Using the periodicity property cos(2π−θ)=cosθ, we can ignore the 2π and simplify the argument to 4πsin2x−2πsin4x.
Our limit now looks like:
x→0lim2x41−cos(4πsin2x−2πsin4x)
Phase 4
The Final Convergence
We are almost there! We use the identity 1−cosα=2sin2(2α).
Applying this to our numerator, we get 2sin2(2πsin2x−πsin4x). The 2 in the numerator cancels with the 2 in the denominator, leaving us with:
x→0limx4sin2(2πsin2x−πsin4x)
To finish, we use the standard limit limu→0usinu=1. We multiply and divide by the square of the argument, (2πsin2x−πsin4x)2.
The limit becomes:
x→0limx4(2πsin2x−πsin4x)2
Factoring out πsin2x, we get:
x→0limx4π2sin4x(2−sin2x)2
Since xsinx→1, this simplifies to π2⋅14⋅(2−0)2=4π2.
And there it is! Through careful application of identities and standard limits, we have unraveled the complexity to find the answer: 4π2.