Analyzing the Setup
The beauty of trigonometric symmetry often lies in simplification. We are tasked with evaluating the expression:
At first glance, this appears to be a complex collection of ratios. However, the secret to solving it lies in the art of unification.
The Strategy of Unification
The first step in any complex trigonometric problem is to reduce the number of variables. We currently have both tanA and cotA present.
Since we know that cotA=tanA1, our strategy is to convert everything into terms of tanA. Substituting this identity into our expression yields:
1−tanA1tanA+1−tanAtanA1
The Algebraic Trap
Now, let us simplify the terms. For the first term, the denominator 1−tanA1 simplifies to tanAtanA−1.
When we invert the fraction, the first term becomes:
For the second term, the tanA in the numerator drops to the denominator, resulting in tanA(1−tanA)1.
Many students stumble here. Notice that the denominators (tanA−1) and (1−tanA) are negatives of each other. By factoring out a −1 from the second term, we align them:
tanA−1tan2A−tanA(tanA−1)1
We now have a common denominator of tanA(tanA−1).
The Hidden Identity
Combining the fractions, the numerator becomes tanA⋅tan2A−1, which is tan3A−1. We are now looking at:
The numerator is a difference of cubes, a3−b3, where a=tanA and b=1. Using the identity a3−b3=(a−b)(a2+ab+b2), we rewrite the numerator as:
The (tanA−1) term cancels out perfectly from the numerator and the denominator. We are left with:
The Final Polish
By splitting the fraction, we obtain:
tanAtan2A+tanAtanA+tanA1=tanA+1+cotA
To reach the final form, we convert back to sinA and cosA:
1+cosAsinA+sinAcosA=1+sinAcosAsin2A+cos2A
Since sin2A+cos2A=1, the expression simplifies to:
A seemingly chaotic expression has been reduced to a simple, elegant result.