To find the solution(s) of the given equation for 0<θ<2π:
∑m=16cosec(θ+4(m−1)π)cosec(θ+4mπ)=42
Let the general term be:
Tm=cosec(θ+4(m−1)π)cosec(θ+4mπ)=sin(θ+4(m−1)π)sin(θ+4mπ)1
Notice that the difference between the arguments is:
(θ+4mπ)−(θ+4(m−1)π)=4π
Multiplying and dividing by sin(4π)=21, we can express each term as:
sin(4π)Tm=sin(θ+4(m−1)π)sin(θ+4mπ)sin[(θ+4mπ)−(θ+4(m−1)π)]
Using the identity sin(A−B)=sinAcosB−cosAsinB:
21Tm=cot(θ+4(m−1)π)−cot(θ+4mπ)
Tm=2[cot(θ+4(m−1)π)−cot(θ+4mπ)]
Summing from m=1 to 6, the terms telescope:
∑m=16Tm=2∑m=16[cot(θ+4(m−1)π)−cot(θ+4mπ)]
=2[cotθ−cot(θ+46π)]
=2[cotθ−cot(23π+θ)]
Since cot(23π+θ)=−tanθ, this simplifies to:
∑m=16Tm=2(cotθ+tanθ)
Setting this equal to 42:
2(cotθ+tanθ)=42
cotθ+tanθ=4
Rewriting in terms of sinθ and cosθ:
sinθcosθ+cosθsinθ=4⟹sinθcosθcos2θ+sin2θ=4
sinθcosθ1=4⟹sin2θ2=4
sin2θ=21
Since 0<θ<2π, we have 0<2θ<π. Therefore:
2θ=6πor2θ=π−6π=65π
θ=12πorθ=125π
Thus, the correct options are C and D.