Summation of Algebraic & Trigonometric Series
Mathematical Induction, Telescoping Differences, AGP Closed Forms, Partial Fractions & C + iS Phasors
§5.1 Mathematical Induction & Polynomial Power Sums
1. The Axiom of Mathematical Induction
The Principle of Mathematical Induction is fundamentally equivalent to the Well-Ordering Principle of the natural numbers $\mathbb{N}$:
- Weak Induction: If a proposition $P(n)$ is true for $n = 1$, and for every $k \ge 1$ the truth of $P(k)$ implies $P(k+1)$, then $P(n)$ is true for all $n \in \mathbb{N}$.
- Strong Induction: If $P(1)$ is true, and the truth of $P(1), P(2), \dots, P(k)$ collectively implies $P(k+1)$, then $P(n)$ is true for all $n \in \mathbb{N}$.
2. Canonical Power Sum Identities
Inductive proofs establish the classic closed forms for integer power sums:
§5.2 Finite Differences & The Telescoping Sum Method
1. The Difference Operator $\Delta$
For a sequence $f(n)$, the forward difference operator is defined by: $$\mathbf{\Delta f(n) \equiv f(n+1) - f(n)}$$ The Fundamental Theorem of Summation Calculus states that the sum of differences telescopes: $$\mathbf{\sum_{k=1}^n \Delta f(k) = \sum_{k=1}^n [f(k+1) - f(k)] = f(n+1) - f(1)}$$ All intermediate terms cancel pairwise, leaving only the boundary evaluations!
2. Factorial Polynomials
We define the falling factorial polynomial of degree $r$: $$n^{(r)} \equiv n(n-1)(n-2)\cdots(n-r+1)$$ Its forward difference mirrors standard polynomial differentiation: $$\Delta [n^{(r)}] = (n+1)^{(r)} - n^{(r)} = r \, n^{(r-1)}$$ Thus, summation follows the discrete power rule: $$\mathbf{\sum_{k=1}^n k^{(r)} = \frac{(n+1)^{(r+1)} - 1^{(r+1)}}{r + 1} = \frac{(n+1)^{(r+1)}}{r + 1}}$$ Any polynomial can be converted to factorial powers via Stirling numbers of the second kind, rendering summation algorithmic!
§5.3 Arithmetico-Geometric Progressions (AGP)
1. Definition of an AGP
An Arithmetico-Geometric Progression is a sequence whose $k$-th term is the product of corresponding terms of an Arithmetic Progression ($a, a+d, a+2d, \dots$) and a Geometric Progression ($1, r, r^2, \dots$): $$\mathbf{u_k = [a + (k-1)d] r^{k-1}}$$ The finite sum to $n$ terms is: $$S_n = a + (a + d)r + (a + 2d)r^2 + \dots + [a + (n-1)d]r^{n-1}$$
2. Closed-Form Derivation
Multiply $S_n$ by the common ratio $r$: $$r S_n = ar + (a + d)r^2 + \dots + [a + (n-2)d]r^{n-1} + [a + (n-1)d]r^n$$ Subtracting this equation from $S_n$: $$(1 - r)S_n = a + d[r + r^2 + \dots + r^{n-1}] - [a + (n-1)d]r^n$$ The bracketed terms form a standard finite geometric series with sum $\frac{r(1 - r^{n-1})}{1 - r}$: $$(1 - r)S_n = a + \frac{dr(1 - r^{n-1})}{1 - r} - [a + (n-1)d]r^n$$ Dividing by $(1 - r)$ yields the exact closed form: $$\mathbf{S_n = \frac{a}{1 - r} + \frac{dr(1 - r^{n-1})}{(1 - r)^2} - \frac{[a + (n-1)d]r^n}{1 - r}}$$
3. Sum to Infinity
For $|r| < 1$, as $n \to \infty$, $r^n \to 0$ and $n r^n \to 0$. The infinite sum simplifies to: $$\mathbf{S_\infty = \frac{a}{1 - r} + \frac{dr}{(1 - r)^2}}$$
§5.4 Summation of Series by Partial Fraction Decomposition
1. The Method of Partial Fractions for Series
When terms of an infinite series are reciprocal products of linear factors, we decompose each term $u_k$ into partial fractions to induce telescoping cancellation: $$u_k = \frac{1}{(k + a)(k + b)} = \frac{1}{b - a} \left[ \frac{1}{k + a} - \frac{1}{k + b} \right]$$ Summing from $k = 1$ to $n$: $$S_n = \frac{1}{b - a} \sum_{k=1}^n \left( \frac{1}{k + a} - \frac{1}{k + b} \right)$$ Depending on the shift $b - a$, intermediate terms cancel, leaving a finite number of uncancelled boundary fractions.
2. Higher-Order Factor Decompositions
For three factors in arithmetic progression: $$u_k = \frac{1}{(a k + b)(a(k+1) + b)(a(k+2) + b)} = \frac{1}{2a} \left[ \frac{1}{(ak+b)(a(k+1)+b)} - \frac{1}{(a(k+1)+b)(a(k+2)+b)} \right]$$ Defining $v_k = \frac{1}{(ak+b)(a(k+1)+b)}$, we observe that $u_k = \frac{1}{2a}[v_k - v_{k+1}]$. The sum to $n$ terms telescopes directly: $$\sum_{k=1}^n u_k = \frac{1}{2a}[v_1 - v_{n+1}]$$ and as $n \to \infty$, $v_{n+1} \to 0$, giving the exact limit $S_\infty = \frac{v_1}{2a}$!
§5.5 Summation of Trigonometric Series via the $C + iS$ Method
1. The Complex Phasor Coupling Technique
To sum a cosine series $C = \sum_{k=0}^{n-1} a_k \cos(\theta_k)$ and sine series $S = \sum_{k=0}^{n-1} a_k \sin(\theta_k)$, we form the complex linear combination: $$\mathbf{C + iS = \sum_{k=0}^{n-1} a_k [\cos(\theta_k) + i\sin(\theta_k)] = \sum_{k=0}^{n-1} a_k e^{i\theta_k}}$$ This converts trigonometric sums into geometric or binomial series in the complex domain! After evaluating $C + iS$ in closed form, equating real parts recovers $C$, and equating imaginary parts recovers $S$.
2. Sum of Sines and Cosines in Arithmetic Progression
Let $\theta_k = \alpha + k\beta$: $$C + iS = \sum_{k=0}^{n-1} e^{i(\alpha + k\beta)} = e^{i\alpha} \sum_{k=0}^{n-1} (e^{i\beta})^k = e^{i\alpha} \frac{1 - e^{in\beta}}{1 - e^{i\beta}}$$ Factoring out half-angles: $$1 - e^{in\beta} = -e^{in\beta/2}(e^{in\beta/2} - e^{-in\beta/2}) = -2i e^{in\beta/2}\sin(n\beta/2)$$ $$1 - e^{i\beta} = -2i e^{i\beta/2}\sin(\beta/2)$$ Dividing: $$C + iS = e^{i\alpha} \frac{-2i e^{in\beta/2}\sin(n\beta/2)}{-2i e^{i\beta/2}\sin(\beta/2)} = \frac{\sin(n\beta/2)}{\sin(\beta/2)} e^{i\left(\alpha + \frac{n-1}{2}\beta\right)}$$ Equating real and imaginary parts gives the famous closed forms:
Step-by-Step Solved Examination Problems
Comprehensive analytical derivations, multi-tier solutions (Foundational, Intermediate Exam, and Honors/Proof Challenge) with complete line-by-line verification.
Evaluate the sum of the first $n$ terms of the arithmetico-geometric series $S_n = 1\cdot 2 + 2\cdot 2^2 + 3\cdot 2^3 + \dots + n\cdot 2^n$.
Shift by the common ratio $r = 2$.
Subtracting aligns terms with unit differences.
Multiply by $-1$ to isolate $S_n$.
\mathbf{S_n = (n - 1)2^{n+1} + 2}.
Find the sum to $n$ terms and the infinite sum of the series $S = \sum_{k=1}^\infty \frac{1}{(2k-1)(2k+1)(2k+3)}$.
Split the three-factor denominator into differences of two-factor denominators.
All interior terms cancel out pairwise.
The terminal boundary term approaches zero as $n \to \infty$.
\mathbf{S_n = \frac{1}{12} - \frac{1}{4(2n+1)(2n+3)}}, \qquad \mathbf{S_\infty = \frac{1}{12}}.
Use the complex $C + iS$ method to evaluate $C = \sum_{k=0}^n \binom{n}{k} \cos(k\theta)$ and $S = \sum_{k=0}^n \binom{n}{k} \sin(k\theta)$, and prove that $C = 2^n \cos^n(\theta/2) \cos(n\theta/2)$.
Combine the real cosine and imaginary sine sums.
The sum matches the binomial expansion of $(1 + z)^n$ where $z = e^{i\theta}$.
Factor $e^{i\theta/2}$ from the base to convert to polar form.
Real part yields $C$, and imaginary part yields $S$.
\mathbf{C = 2^n \cos^n(\theta/2) \cos(n\theta/2)}, \qquad \mathbf{S = 2^n \cos^n(\theta/2) \sin(n\theta/2)}.