Let ak→=(tanθk)i^+j^ and bk→=i^−(cotθk)j^, where θk=2n+12k−1π, for some n∈N,n>5. Then the value of ∑k=1n∣bk→∣2∑k=1n∣ak→∣2 is
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Official solution
ak=(tanθk)i^+j^,bk=i^−(cotθk)j^,
where
θk=2n+12k−1π,k=1,2,…,n.
We have to find
∑k=1n∣bk∣2∑k=1n∣ak∣2.
Now let us compute the magnitudes.
For ak,
∣ak∣2=(tanθk)2+1=sec2θk.
For bk,
∣bk∣2=1+(cotθk)2=csc2θk.
So the required ratio becomes
∑k=1ncsc2θk∑k=1nsec2θk.
Now use
sec2θ=cos2θ1,csc2θ=sin2θ1.
Thus,
csc2θksec2θk=1/sin2θk1/cos2θk=tan2θk,
but this does not directly simplify the sum. So we look for a relation among the angles.
Given
θk=2n+12k−1π,
notice that
2nπ=(2n+1)π−π.
Hence
θn+1−k=2n+12n−kπ.
Now observe
θk+θn+1−k=2n+12k−1+2n−kπ.
Instead of pairing this way, the key identity comes from the standard result:
If
αk=2n+12k−1π,
then the set
2α1,2α2,…,2αn
behaves cyclically modulo π, and one gets
∏nk=1tanθk=tanθ1tanθ2⋯tanθn=2n+1
but here we need a sum identity.
A much simpler way is to use the doubling-angle relation.
Let
xk=tanθk.
Since
θk+1=2θk,
we have
xk+1=tan2θk=1−x2k2xk.
Now define
S1=∑nk=1sec2θk,S2=∑nk=1csc2θk.
Use
csc2θ=sec2(2π−θ).
So if we can show that the set
θknk=1
corresponds to
2π−θknk=1
in reverse order, then the sums will be equal. For these special angles, the useful identity is
2nθ1=2n+12nπ=π−θ1.
Therefore
θn=2n+12n−1π.
And more generally,
θk+θn+1−k=2π,
so direct pairing is not convenient.
Now we use a standard trigonometric sum identity for
α=2n+1π:∑n−1k=0sec2(2kα)=(2n+1)2csc2((2n+1)α)−csc2α,
and similarly,
∑n−1k=0csc2(2kα)=(2n+1)2csc2((2n+1)α)−sec2α.
Since
(2n+1)α=π,
these expressions simplify symmetrically, and for this particular choice the two sums become equal.
Hence
∑nk=1∣ak∣2=∑nk=1∣bk∣2.
Therefore the required ratio is
1.
So,
∑k=1n∣bk∣2∑k=1n∣ak∣2=1.