To evaluate the summation
S=∑k=113sin(4π+6(k−1)π)sin(4π+6kπ)1
Let us define θk=4π+6kπ.
The difference between two consecutive terms in the argument is constant:
θk−θk−1=(4π+6kπ)−(4π+6(k−1)π)=6π
Taking the sine on both sides, we get:
sin(θk−θk−1)=sin(6π)=21
We can rewrite the general term Tk of the series by multiplying and dividing by sin(6π):
Tk=sinθk−1sinθk1=sin(6π)1⋅sinθk−1sinθksin(θk−θk−1)
Using the sine subtraction formula sin(A−B)=sinAcosB−cosAsinB, we obtain:
sinθk−1sinθksin(θk−θk−1)=sinθk−1sinθksinθkcosθk−1−cosθksinθk−1=cotθk−1−cotθk
Since sin(6π)1=2, the term Tk simplifies to:
Tk=2(cotθk−1−cotθk)
Now, substituting Tk into the summation yields a telescoping series:
S=∑k=113Tk=2∑k=113(cotθk−1−cotθk)=2(cotθ0−cotθ13)
Next, we calculate the required angles θ0 and θ13:
For k=0:
θ0=4π⟹cotθ0=cot(4π)=1
For k=13:
θ13=4π+613π=2π+(4π+6π)=2π+125π
Using the periodicity of the cotangent function:
cotθ13=cot(2π+125π)=cot(125π)=tan(12π)=2−3
Substituting these values back into the telescoping sum:
S=2[1−(2−3)]=2(1−2+3)=2(3−1)