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Chapter 5 • Theory & Derivations

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:

$$\mathbf{S_1(n) = \sum_{k=1}^n k = \frac{n(n+1)}{2}}$$ $$\mathbf{S_2(n) = \sum_{k=1}^n k^2 = \frac{n(n+1)(2n+1)}{6}}$$ $$\mathbf{S_3(n) = \sum_{k=1}^n k^3 = \left[\frac{n(n+1)}{2}\right]^2 = [S_1(n)]^2}$$
The remarkable identity $S_3(n) = [S_1(n)]^2$ (Nicomachus's Theorem) states that the sum of the first $n$ cubes equals the square of the sum of the first $n$ integers.

§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:

$$\mathbf{C = \sum_{k=0}^{n-1} \cos(\alpha + k\beta) = \frac{\sin(n\beta/2)}{\sin(\beta/2)} \cos\left(\alpha + \frac{n-1}{2}\beta\right)}$$ $$\mathbf{S = \sum_{k=0}^{n-1} \sin(\alpha + k\beta) = \frac{\sin(n\beta/2)}{\sin(\beta/2)} \sin\left(\alpha + \frac{n-1}{2}\beta\right)}$$

TIERED UNIVERSITY HONORS PROBLEMS

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.

Foundational Mechanics Example 5.1: Finite Arithmetico-Geometric Series Evaluation

Evaluate the sum of the first $n$ terms of the arithmetico-geometric series $S_n = 1\cdot 2 + 2\cdot 2^2 + 3\cdot 2^3 + \dots + n\cdot 2^n$.

Step 1: Identify Parameters and Multiply by Common Ratio
$$a = 1, \quad d = 1, \quad r = 2 \\ S_n = 1\cdot 2^1 + 2\cdot 2^2 + 3\cdot 2^3 + \dots + n\cdot 2^n \\ 2 S_n = 1\cdot 2^2 + 2\cdot 2^3 + \dots + (n-1)\cdot 2^n + n\cdot 2^{n+1}$$

Shift by the common ratio $r = 2$.

Step 2: Subtract the Shifted Series
$$S_n - 2S_n = 2^1 + (2^2 + 2^3 + \dots + 2^n) - n\cdot 2^{n+1} \\ -S_n = \sum_{k=1}^n 2^k - n\cdot 2^{n+1}$$

Subtracting aligns terms with unit differences.

Step 3: Evaluate the Geometric Sum and Solve for Sₙ
$$\sum_{k=1}^n 2^k = \frac{2(2^n - 1)}{2 - 1} = 2^{n+1} - 2 \\ -S_n = (2^{n+1} - 2) - n\cdot 2^{n+1} = (1 - n)2^{n+1} - 2 \\ S_n = (n - 1)2^{n+1} + 2$$

Multiply by $-1$ to isolate $S_n$.

Final Answer & Physical Insight

\mathbf{S_n = (n - 1)2^{n+1} + 2}.

Intermediate University Exam Example 5.2: Telescoping Partial Fraction Infinite Series

Find the sum to $n$ terms and the infinite sum of the series $S = \sum_{k=1}^\infty \frac{1}{(2k-1)(2k+1)(2k+3)}$.

Step 1: Decompose the General Term into Partial Differences
$$u_k = \frac{1}{(2k-1)(2k+1)(2k+3)} \\ \text{Difference between outer factors: } (2k+3) - (2k-1) = 4 \\ u_k = \frac{1}{4} \left[ \frac{(2k+3) - (2k-1)}{(2k-1)(2k+1)(2k+3)} \right] = \frac{1}{4} \left[ \frac{1}{(2k-1)(2k+1)} - \frac{1}{(2k+1)(2k+3)} \right]$$

Split the three-factor denominator into differences of two-factor denominators.

Step 2: Form the Telescoping Sum
$$v_k = \frac{1}{(2k-1)(2k+1)} \implies u_k = \frac{1}{4}[v_k - v_{k+1}] \\ S_n = \sum_{k=1}^n u_k = \frac{1}{4}[v_1 - v_{n+1}] = \frac{1}{4}\left[ \frac{1}{1\cdot 3} - \frac{1}{(2n+1)(2n+3)} \right] = \frac{1}{12} - \frac{1}{4(2n+1)(2n+3)}$$

All interior terms cancel out pairwise.

Step 3: Evaluate the Infinite Limit
$$S_\infty = \lim_{n \to \infty} S_n = \frac{1}{12} - 0 = \frac{1}{12}$$

The terminal boundary term approaches zero as $n \to \infty$.

Final Answer & Physical Insight

\mathbf{S_n = \frac{1}{12} - \frac{1}{4(2n+1)(2n+3)}}, \qquad \mathbf{S_\infty = \frac{1}{12}}.

Honors / Proof Challenge Example 5.3: Binomial Trigonometric Sums via the C + iS Method

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 $C = 2^n \cos^n(\theta/2) \cos(n\theta/2)$.

Step 1: Set Up the Complex Linear Combination C + iS
$$C + iS = \sum_{k=0}^n \binom{n}{k} [\cos(k\theta) + i\sin(k\theta)] = \sum_{k=0}^n \binom{n}{k} (e^{i\theta})^k$$

Combine the real cosine and imaginary sine sums.

Step 2: Apply the Binomial Theorem
$$C + iS = (1 + e^{i\theta})^n$$

The sum matches the binomial expansion of $(1 + z)^n$ where $z = e^{i\theta}$.

Step 3: Factor Half-Angles and Apply Euler's Formula
$$1 + e^{i\theta} = e^{i\theta/2}(e^{-i\theta/2} + e^{i\theta/2}) = e^{i\theta/2}[2\cos(\theta/2)] = 2\cos(\theta/2) e^{i\theta/2} \\ (1 + e^{i\theta})^n = [2\cos(\theta/2) e^{i\theta/2}]^n = 2^n \cos^n(\theta/2) e^{i n\theta/2} \\ = 2^n \cos^n(\theta/2) [\cos(n\theta/2) + i\sin(n\theta/2)]$$

Factor $e^{i\theta/2}$ from the base to convert to polar form.

Step 4: Equate Real and Imaginary Parts
$$C = 2^n \cos^n(\theta/2) \cos(n\theta/2) \quad \blacksquare \\ S = 2^n \cos^n(\theta/2) \sin(n\theta/2)$$

Real part yields $C$, and imaginary part yields $S$.

Final Answer & Physical Insight

\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)}.