Analyzing the Setup
Welcome, fellow traveler of the mathematical landscape. Today, we are going to dismantle a problem that, at first glance, looks like a chaotic jumble of inverse trigonometric functions.
You see a series: cot−1(47)+cot−1(419)+cot−1(439)+…. Beneath this complexity lies a hidden, rhythmic order waiting for us to uncover it.
Decoding the Pattern
Every great journey begins with observation. Let us look at the numerators: 7,19,39,67,….
If we calculate the first differences, we get 12,20,28,…. The second differences are 8,8,…, which confirms that the sequence is quadratic.
By fitting this to the form an2+bn+c, we discover that the n-th numerator is Nn=4n2+3. Thus, our general term is:
The Art of Transformation
We prefer working with tan−1 because it facilitates the use of the difference identity. Using the property cot−1(x)=tan−1(x1), we rewrite our term as:
Dividing the numerator and denominator by 4, we obtain:
To utilize the identity tan−1(A)−tan−1(B), we force the denominator into the form 1+AB. We add and subtract 1 in the denominator:
Recognizing n2−1/4 as a difference of squares, we factor it into (n−1/2)(n+1/2). Our term now stands as:
Tn=tan−1(1+(n+1/2)(n−1/2)1)
The Telescoping Symphony
Observe that the numerator can be expressed as the difference of our factors: (n+1/2)−(n−1/2)=1. We can now express our term as:
Tn=tan−1(1+(n+1/2)(n−1/2)(n+1/2)−(n−1/2))
By the identity tan−1(A)−tan−1(B)=tan−1(1+ABA−B), this simplifies to:
Tn=tan−1(n+1/2)−tan−1(n−1/2)
When we sum these terms from n=1 to N, the terms cancel like falling dominoes. This leaves us with only the first negative term and the last positive term:
SN=tan−1(N+1/2)−tan−1(1/2)
Final Calculation
Finally, we take the limit as N→∞. As N grows, tan−1(N+1/2) approaches the horizontal asymptote of π/2.
Our infinite sum becomes:
Using the identity 2π−tan−1(x)=cot−1(x), we arrive at the final result: