The Geometry of Symmetry
A Journey into Complex Sums
Welcome, student. Today, we are not just solving a summation; we are uncovering a hidden symmetry in the unit circle. When you look at the expression ∑k=1n−1(n−k)cosn2kπ, you might see a daunting trigonometric series.
But I want you to see something else. I want you to see vectors. I want you to see the roots of unity dancing around the origin.
Phase 1
The Complex Transformation
Whenever you see a trigonometric sum where the angles are in an arithmetic progression, your intuition should immediately scream: "Complex Numbers!" Because trigonometry is just the projection of complex rotation.
Let us define z=ein2π. This z is the primitive n-th root of unity. By Euler's formula, z=cosn2π+isinn2π.
Our target sum is the real part of a complex sum
S. Let us define:
S=k=1∑n−1(n−k)zk
Notice that Re(S)=∑k=1n−1(n−k)Re(zk)=∑k=1n−1(n−k)cosn2kπ. We have successfully translated our problem from the messy world of cosines into the clean, algebraic world of complex powers.
Phase 2
The Decomposition
Now, let us expand
S. We can distribute the
(n−k) term:
S=nk=1∑n−1zk−k=1∑n−1kzk
Let us call these two parts S1 and S2. For S1, we recall the beautiful property of the roots of unity: the sum of all n roots is zero, i.e., ∑k=0n−1zk=0.
Since our sum S1 starts from k=1, we are missing the k=0 term, which is z0=1. Thus, ∑k=1n−1zk=−1. This simplifies S to S=−n−S2.
Phase 3
The AGP Battle
Now, we face S2=∑k=1n−1kzk. This is an Arithmetico-Geometric Progression. To solve it, we use the "shift and subtract" method.
We write
S2=z+2z2+3z3+⋯+(n−1)zn−1. Then, we multiply by
z:
zS2=z2+2z3+⋯+(n−2)zn−1+(n−1)zn
Subtracting these two equations:
S2(1−z)=z+z2+z3+⋯+zn−1−(n−1)zn
Since
zn=1, the last term is simply
−(n−1). The geometric series
z+z2+⋯+zn−1 is again
−1. Thus:
S2(1−z)=−1−(n−1)=−n
This gives us S2=1−z−n=z−1n.
Phase 4
The Half-Angle Magic
We are at the final stretch. We have
S=−n−S2=−n−z−1n. Simplifying this, we get:
S=−n(1+z−11)=−n(z−1z)
To extract the real part, we use the half-angle trick. Let
θ=n2π. Then:
z−1z=eiθ−1eiθ
Multiplying numerator and denominator by
e−iθ/2, we get:
eiθ/2−e−iθ/2eiθ/2=2isin(θ/2)cos(θ/2)+isin(θ/2)=21−2icot(θ/2)
Finally, S=−n(21−2icot(nπ)). The real part is clearly −2n.
We have arrived at the destination. The complexity collapses into a simple constant. This is the beauty of JEE mathematics—the most complex problems often yield the most elegant, simple truths.