Expanding the sum: S=2[(cotA1−cotA2)+(cotA2−cotA3)+⋯+(cotA13−cotA14)].
Notice the cancellation of intermediate terms.
Cancelling Intermediate Terms
Intermediate terms cancel out:
(cotA1−cotA2)+(cotA2−cotA3)+…
This leaves only the first and last terms.
Final Surviving Terms
Only the first and last terms survive:
S=2[cotA1−cotA14]
Evaluating the Angles
Calculate the boundary angles:
A1=4π+(1−1)6π=4π
A14=4π+(14−1)6π=4π+613π=2π+125π
Calculating Cotangent Values
Evaluate the cotangent values:
cotA1=cot(4π)=1
cotA14=cot(2π+125π)=cot(75∘)=2−3
Final Sum Calculation
Substitute back into the sum expression:
S=2[1−(2−3)]
S=2[1−2+3]=2[3−1]
S=23−2
Finding a and b
Compare 23−2 with a3+b:
We get a=2 and b=−2.
Calculate a2+b2=22+(−2)2=4+4=8.
The final answer is 8.
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The Sigma Insight: Trigonometric Ratios and Identities
Solution Diagram
The Art of the Telescoping Series
A Journey Through Trigonometry
Welcome, future engineers. Today, we are going to dismantle a problem that, at first glance, looks like a chaotic mess of sines and angles. You see a summation from r=1 to 13, and the denominator is a product of two sine functions.
Your instinct might be to panic, to try and expand everything, or to look for a complex identity. But stop. Take a breath. In the world of JEE Advanced, complexity is often just a mask for elegance. Let us peel back that mask.
Phase 1
Decoding the Anatomy
First, let us look at the angles. We define Ar=4π+(r−1)6π. The term following it is Ar+1=4π+r6π.
Now, calculate the difference:
Ar+1−Ar=(4π+6rπ)−(4π+6(r−1)π)
The 4π terms vanish, and we are left with:
Ar+1−Ar=6rπ−6(r−1)π=6π
This is the heartbeat of the problem. The difference is constant! Whenever you see a product of trigonometric functions in the denominator, and the difference between the angles is constant, you are dealing with a telescoping series.
Phase 2
The Telescoping Magic
We need to transform our general term Tr=sin(Ar)sin(Ar+1)1 into something that can collapse. We use the "clever one" trick. We multiply and divide by sin(6π).
Because sin(6π)=sin(Ar+1−Ar), this allows us to rewrite the numerator using the sine subtraction identity: sin(A−B)=sinAcosB−cosAsinB.
Look at the terms! The −cotA2 from the first bracket is annihilated by the +cotA2 from the second. This chain reaction continues, consuming every intermediate term.
This is the "telescoping" effect—the series collapses like a folding telescope, leaving only the first and the last terms standing:
S=2[cotA1−cotA14]
Phase 4
The Final Tally
We are almost there. We just need to evaluate the boundary angles. For r=1, A1=4π.
For r=14:
A14=4π+136π=4π+2π+6π=2π+125π
We know cot(4π)=1. For cot(2π+125π), the 2π is just a full rotation, so we are looking at cot(75∘), which is 2−3.
Substituting these back:
S=2[1−(2−3)]=2[3−1]=23−2
Comparing this to a3+b, we find a=2 and b=−2. The final answer, a2+b2, is:
22+(−2)2=4+4=8
You have conquered the beast. Remember, in JEE, it is not about brute force; it is about finding the pattern and letting the math do the work for you.