Expanding the sum: S=2[(cotA1−cotA2)+(cotA2−cotA3)+⋯+(cotA13−cotA14)]
After telescoping: S=2[cotA1−cotA14]
Evaluate Boundary Terms
Calculate A1=4π+0=4π⟹cotA1=1
Calculate A14=4π+613π=4π+2π+6π
Using periodicity: cotA14=cot(4π+6π)=cot(125π)
Note: cot(75∘)=2−3
Final Calculation
Substitute values into the sum: S=2[1−(2−3)]
Simplify the expression: S=2[1−2+3]=2[3−1]
Final Answer:2(3−1)
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The Sigma Insight: Trigonometric Ratios and Identities
Analyzing the Setup
When you encounter a summation like
S=k=1∑13sin(4π+6(k−1)π)sin(4π+6kπ)1
it is natural to feel intimidated. However, the structure of the denominator—a product of two sine functions—is a classic signature of a telescoping series.
Let us define the angles as Ak=4π+6(k−1)π and Ak+1=4π+6kπ.
The difference between these angles is constant:
Ak+1−Ak=(4π+6kπ)−(4π+6(k−1)π)=6π
The Master Equation
This constant difference is the heartbeat of the problem. We utilize the trigonometric identity:
sinAsinBsin(B−A)=cotA−cotB
To apply this, we multiply and divide the general term Tk by sin(6π). Since sin(6π)=21, dividing by it is equivalent to multiplying by 2:
Tk=2⋅sinAksinAk+1sin(Ak+1−Ak)
Applying the identity, the expression simplifies beautifully:
Tk=2(cotAk−cotAk+1)
The Telescoping Collapse
Now, we evaluate the summation S=∑k=113Tk. Writing out the terms reveals the rhythmic cancellation: