The Limit as a Gateway to Elegance
Welcome, fellow traveler of the mathematical landscape. Today, we are going to dissect a limit problem that, at first glance, might seem like a chaotic mess of trigonometric functions.
But as we peel back the layers, you will see that it is actually a beautifully choreographed dance of identities and standard limits. Let us embark on this journey together.
Phase 1
The Indeterminate Trap
We begin, as we always do, by testing the waters. We are given the limit:
L=θ→0limsin(2πsin2θ)tan(πcos2θ)
When we substitute θ=0, we find that cos(0)=1, so the numerator becomes tan(π), which is 0. In the denominator, sin(0)=0, so we get sin(0), which is also 0.
We have arrived at the classic 00 indeterminate form. This is not a dead end; it is an invitation to manipulate the expression into something more revealing.
Phase 2
The Trigonometric Bridge
Look closely at the arguments of our functions. The numerator has cos2θ, and the denominator has sin2θ. This mismatch is the core of the problem.
To use our standard limit theorems, we need the arguments to be consistent. We need a bridge between cosine and sine. That bridge is the fundamental identity:
By substituting this into our numerator, we transform the expression into a language of sines. Our limit now looks like this:
L=θ→0limsin(2πsin2θ)tan(π(1−sin2θ))
Distributing the π, we get tan(π−πsin2θ). Now, we are getting somewhere!
Phase 3
The Allied Angle Transformation
Here is where we must be precise. We have tan(π−A), where A=πsin2θ. Recall the allied angle property: tan(π−A)=−tanA.
This is a crucial step. Because π−A lies in the second quadrant, the tangent function is negative. Applying this, our numerator simplifies to −tan(πsin2θ).
Our limit is now:
L=θ→0limsin(2πsin2θ)−tan(πsin2θ)
Notice how both arguments, πsin2θ and 2πsin2θ, now approach 0 as θ→0. This is exactly what we need to invoke our standard limits.
Phase 4
The Symphony of Standard Limits
We know that limx→0xtanx=1 and limx→0xsinx=1. To force our expression into this form, we multiply and divide by the arguments:
L=θ→0lim−(πsin2θtan(πsin2θ))⋅(sin(2πsin2θ)2πsin2θ)⋅2πsin2θπsin2θ
As θ→0, the first term approaches 1, and the second term approaches 1. We are left with the constant ratio:
L=−1⋅1⋅θ→0lim2πsin2θπsin2θ
The πsin2θ terms cancel out perfectly, leaving us with −21.
Conclusion
And there it is. Through careful identity substitution and the application of standard limits, we have tamed the expression.
The final answer is −21. Remember, in JEE Advanced, it is not just about getting the answer; it is about understanding the path. Keep practicing, keep questioning, and keep falling in love with the logic behind the math.