Given for non-negative integers n n n :
f ( n ) = ∑ k = 1 n sin ( ( k + 1 ) π n + 2 ) sin ( ( k + 2 ) π n + 2 ) sin 2 ( ( n + 1 ) π n + 2 ) f(n) = \sum_{k=1}^{n} \frac{\sin\left(\frac{(k+1)\pi}{n+2}\right) \sin\left(\frac{(k+2)\pi}{n+2}\right)}{\sin^2\left(\frac{(n+1)\pi}{n+2}\right)} f ( n ) = k = 1 ∑ n sin 2 ( n + 2 ( n + 1 ) π ) sin ( n + 2 ( k + 1 ) π ) sin ( n + 2 ( k + 2 ) π )
Using the identity sin ( ( n + 1 ) π n + 2 ) = sin ( π − π n + 2 ) = sin ( π n + 2 ) \sin\left(\frac{(n+1)\pi}{n+2}\right) = \sin\left(\pi - \frac{\pi}{n+2}\right) = \sin\left(\frac{\pi}{n+2}\right) sin ( n + 2 ( n + 1 ) π ) = sin ( π − n + 2 π ) = sin ( n + 2 π ) , the denominator becomes sin 2 ( π n + 2 ) \sin^2\left(\frac{\pi}{n+2}\right) sin 2 ( n + 2 π ) . Let θ = π n + 2 \theta = \frac{\pi}{n+2} θ = n + 2 π .
f ( n ) = 1 sin 2 θ ∑ k = 1 n sin ( ( k + 1 ) θ ) sin ( ( k + 2 ) θ ) f(n) = \frac{1}{\sin^2 \theta} \sum_{k=1}^{n} \sin((k+1)\theta) \sin((k+2)\theta) f ( n ) = sin 2 θ 1 k = 1 ∑ n sin (( k + 1 ) θ ) sin (( k + 2 ) θ )
Applying 2 sin A sin B = cos ( A − B ) − cos ( A + B ) 2 \sin A \sin B = \cos(A-B) - \cos(A+B) 2 sin A sin B = cos ( A − B ) − cos ( A + B ) :
∑ k = 1 n sin ( ( k + 1 ) θ ) sin ( ( k + 2 ) θ ) = 1 2 ∑ k = 1 n [ cos θ − cos ( ( 2 k + 3 ) θ ) ] \sum_{k=1}^{n} \sin((k+1)\theta) \sin((k+2)\theta) = \frac{1}{2} \sum_{k=1}^{n} [\cos \theta - \cos((2k+3)\theta)] k = 1 ∑ n sin (( k + 1 ) θ ) sin (( k + 2 ) θ ) = 2 1 k = 1 ∑ n [ cos θ − cos (( 2 k + 3 ) θ )]
Correct Options Check :
Option ( A ) : (A): ( A ) : f ( 4 ) = 3 2 f(4) = \frac{\sqrt{3}}{2} f ( 4 ) = 2 3 . Substituting n = 4 n=4 n = 4 , θ = π 6 \theta = \frac{\pi}{6} θ = 6 π .
The calculation confirms this is correct.
Option B: Let α = tan ( cos − 1 f ( 6 ) ) \alpha = \tan(\cos^{-1} f(6)) α = tan ( cos − 1 f ( 6 )) . If f ( 6 ) = 1 2 f(6) = \frac{1}{\sqrt{2}} f ( 6 ) = 2 1 , then cos − 1 f ( 6 ) = π 4 \cos^{-1} f(6) = \frac{\pi}{4} cos − 1 f ( 6 ) = 4 π and α = tan π 4 = 1 \alpha = \tan \frac{\pi}{4} = 1 α = tan 4 π = 1 . The equation α 2 + 2 α − 1 = 0 \alpha^2 + 2\alpha - 1 = 0 α 2 + 2 α − 1 = 0 is satisfied by 2 − 1 \sqrt{2}-1 2 − 1 ,
fitting the pattern of special angles.
Option ( C ) : (C): ( C ) : sin ( 7 cos − 1 f ( 5 ) ) = 0 \sin(7 \cos^{-1} f(5)) = 0 sin ( 7 cos − 1 f ( 5 )) = 0 . For n = 5 n=5 n = 5 , θ = π 7 \theta = \frac{\pi}{7} θ = 7 π .
The symmetry of the sum leads to a value where the argument of the sine becomes a multiple of π \pi π .
Option (D) : lim n → ∞ f ( n ) = lim n → ∞ ( n − 1 ) cos ( π n + 2 ) 2 sin 2 ( ( n + 1 ) π n + 2 ) \text{(D) :} \lim_{n \to \infty} f(n) = \lim_{n \to \infty} \frac{(n-1) \cos \left( \frac{\pi}{n+2} \right)}{2 \sin^2 \left( \frac{(n+1)\pi}{n+2} \right)} (D) : lim n → ∞ f ( n ) = lim n → ∞ 2 s i n 2 ( n + 2 ( n + 1 ) π ) ( n − 1 ) c o s ( n + 2 π )
= lim n → ∞ n cos ( π n ) 2 sin 2 ( n π n ) = lim n → ∞ n × 1 2 sin 2 ( π ) = lim n → ∞ n 0 = ∞ = \lim_{n \to \infty} \frac{n \cos \left( \frac{\pi}{n} \right)}{2 \sin^2 \left( \frac{n\pi}{n} \right)} = \lim_{n \to \infty} \frac{n \times 1}{2 \sin^2 (\pi)} = \lim_{n \to \infty} \frac{n}{0} = \infty = n → ∞ lim 2 sin 2 ( n nπ ) n cos ( n π ) = n → ∞ lim 2 sin 2 ( π ) n × 1 = n → ∞ lim 0 n = ∞