Calculus Lecture Notes: Infinite Series and Convergence Criteria

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Vocabulary flashcards covering the definitions, key convergence theorems, criteria, and classic examples of infinite series.

18 Terms

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Series

The sum of the infinitely many terms of a sequence (an)(a_n), denoted as ∑n=1+∞an\sum_{n=1}^{+\infty} a_n and formally defined as the sequence of its partial sums (sn)(s_n).

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Partial Sums

The sequence (sn)(s_n) formed by summing a finite number of terms of a sequence (an)(a_n), where s1=a1s_1 = a_1 and sn=sn−1+an=a1+a2+⋯+ans_n = s_{n-1} + a_n = a_1 + a_2 + \dots + a_n.

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Convergent Series

A series ∑n=1+∞an\sum_{n=1}^{+\infty} a_n whose sequence of partial sums (sn)(s_n) has a finite limit SS as n→+∞n \to +\infty, written as ∑n=1+∞an=S\sum_{n=1}^{+\infty} a_n = S.

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Irregular Series

A series ∑n=1+∞an\sum_{n=1}^{+\infty} a_n for which the sequence of partial sums (sn)(s_n) is irregular, meaning lim⁡n→+∞sn\lim_{n \to +\infty} s_n does not exist.

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Mengoli Series

The series given by ∑n=1+∞1n(n+1)=11⋅2+12⋅3+13⋅4+…\sum_{n=1}^{+\infty} \frac{1}{n(n+1)} = \frac{1}{1 \cdot 2} + \frac{1}{2 \cdot 3} + \frac{1}{3 \cdot 4} + \dots, which converges and has a sum equal to 11.

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Geometric Series

A series with ratio qq of the form ∑n=0+∞qn=1+q+q2+q3+…\sum_{n=0}^{+\infty} q^n = 1 + q + q^2 + q^3 + \dots, whose partial sum equals sn=1−qn+11−qs_n = \frac{1-q^{n+1}}{1-q} for q≠1q \neq 1.

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Convergence Behavior of Geometric Series

The geometric series ∑n=0+∞qn\sum_{n=0}^{+\infty} q^n converges to 11−q\frac{1}{1-q} if ∣q∣<1|q| < 1, diverges to +∞+\infty if q≥1q \ge 1, and is irregular if q≤−1q \le -1.

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Harmonic Series

The series ∑n=1+∞1n=1+12+13+14+…\sum_{n=1}^{+\infty} \frac{1}{n} = 1 + \frac{1}{2} + \frac{1}{3} + \frac{1}{4} + \dots, which is divergent to +∞+\infty.

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Necessary Condition for Convergence

Theorem 407 stating that if the series ∑n=0+∞an\sum_{n=0}^{+\infty} a_n converges, then lim⁡n→+∞an=0\lim_{n \to +\infty} a_n = 0; if ana_n does not converge to 00, the series cannot converge.

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Regularity Test for Positive Series

Proposition 409 stating that each series with positive terms (an≥0a_n \ge 0) is regular (either convergent or positively divergent), and it converges if and only if its sequence of partial sums is bounded from above.

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Generalized Harmonic Series

The series ∑n=1+∞1nα\sum_{n=1}^{+\infty} \frac{1}{n^\alpha} with α∈R\alpha \in \mathbb{R}, which converges for α>1\alpha > 1 and diverges to +∞+\infty for α≤1\alpha \le 1.

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Asymptotic Comparison Criterion

Proposition 417 stating that if ∑n=0+∞an\sum_{n=0}^{+\infty} a_n and ∑n=0+∞bn\sum_{n=0}^{+\infty} b_n are two series with strictly positive terms and an∼bna_n \sim b_n, then both series have the same character (both converge or both diverge to +∞+\infty).

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Comparison Criterion

Proposition 410 stating that for two series with positive terms where an≤bna_n \le b_n eventually: if ∑an\sum a_n diverges positively, then ∑bn\sum b_n diverges positively; if ∑bn\sum b_n converges, then ∑an\sum a_n converges.

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Logarithmic Generalized Harmonic Series

The series ∑n=2+∞1nαln⁡β(n)\sum_{n=2}^{+\infty} \frac{1}{n^\alpha \ln^\beta(n)}, which converges for α>1\alpha > 1 with any β∈R\beta \in \mathbb{R} as well as for α=1\alpha = 1 and β>1\beta > 1, and diverges for α<1\alpha < 1 with any β∈R\beta \in \mathbb{R} as well as for α=1\alpha = 1 and β≤1\beta \le 1.

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Exponential Series

The power series defined by ∑n=0+∞xnn!=ex\sum_{n=0}^{+\infty} \frac{x^n}{n!} = e^x for every x∈Rx \in \mathbb{R}, which gives ∑n=0+∞1n!=e\sum_{n=0}^{+\infty} \frac{1}{n!} = e when x=1x = 1.

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Absolute Convergence

Definition 429 stating that a series ∑n=0+∞an\sum_{n=0}^{+\infty} a_n is absolutely convergent if the series of its absolute values, ∑n=0+∞∣an∣\sum_{n=0}^{+\infty} |a_n|, converges.

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Absolute Convergence Theorem

Theorem 430 stating that if a series converges absolutely, then it converges.

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Alternating Harmonic Series Sum

Proposition 435 stating that the alternating series ∑n=1+∞(−1)n+1n=1−12+13−14+…\sum_{n=1}^{+\infty} \frac{(-1)^{n+1}}{n} = 1 - \frac{1}{2} + \frac{1}{3} - \frac{1}{4} + \dots converges to ln⁡(2)\ln(2).