All Study Guides Calculus II Unit 5
➗ Calculus II Unit 5 – Sequences and SeriesSequences and series form the backbone of advanced calculus, providing tools to analyze infinite processes and approximate complex functions. This unit explores various types of sequences and series, their convergence properties, and methods to determine their behavior.
From arithmetic and geometric progressions to power series and Taylor expansions, these concepts have wide-ranging applications. Understanding convergence tests, interval of convergence, and error bounds enables students to solve differential equations and represent functions as infinite sums.
Key Concepts and Definitions
Sequences are ordered lists of numbers, denoted as a n a_n a n where n n n is a non-negative integer
Terms of a sequence are the individual numbers in the sequence, with the n n n -th term denoted as a n a_n a n
Arithmetic sequences have a constant difference d d d between consecutive terms, where a n + 1 = a n + d a_{n+1} = a_n + d a n + 1 = a n + d
Example: 2, 5, 8, 11, ... is an arithmetic sequence with d = 3 d = 3 d = 3
Geometric sequences have a constant ratio r r r between consecutive terms, where a n + 1 = a n ⋅ r a_{n+1} = a_n \cdot r a n + 1 = a n ⋅ r
Example: 3, 6, 12, 24, ... is a geometric sequence with r = 2 r = 2 r = 2
Series are the sum of the terms in a sequence, denoted as ∑ n = 1 ∞ a n \sum_{n=1}^{\infty} a_n ∑ n = 1 ∞ a n
Partial sums are the sums of the first n n n terms of a series, denoted as S n = ∑ i = 1 n a i S_n = \sum_{i=1}^{n} a_i S n = ∑ i = 1 n a i
Convergence occurs when the limit of a sequence or series exists and is a finite value
Divergence occurs when the limit of a sequence or series does not exist or is infinite
Types of Sequences
Constant sequences have the same value for all terms, where a n = c a_n = c a n = c for some constant c c c
Recursive sequences define each term based on the previous term(s), such as the Fibonacci sequence where a n = a n − 1 + a n − 2 a_n = a_{n-1} + a_{n-2} a n = a n − 1 + a n − 2
Explicit sequences have a formula that directly calculates the n n n -th term, such as a n = 2 n + 1 a_n = 2n + 1 a n = 2 n + 1
Monotonic sequences are either increasing (a n + 1 ≥ a n a_{n+1} \geq a_n a n + 1 ≥ a n ) or decreasing (a n + 1 ≤ a n a_{n+1} \leq a_n a n + 1 ≤ a n ) for all n n n
Example: 1, 2, 3, 4, ... is an increasing sequence
Example: 10, 8, 6, 4, ... is a decreasing sequence
Bounded sequences have an upper and/or lower bound, where there exist constants M M M and m m m such that m ≤ a n ≤ M m \leq a_n \leq M m ≤ a n ≤ M for all n n n
Oscillating sequences alternate between increasing and decreasing or have no consistent pattern
Example: 1, -1, 1, -1, ... is an oscillating sequence
Convergence and Divergence
Convergent sequences approach a specific finite value as n n n approaches infinity
Example: a n = 1 n a_n = \frac{1}{n} a n = n 1 converges to 0 as n → ∞ n \to \infty n → ∞
Divergent sequences do not approach a specific finite value or grow without bound as n n n approaches infinity
Example: a n = n a_n = n a n = n diverges to infinity as n → ∞ n \to \infty n → ∞
The limit of a convergent sequence is the value it approaches as n n n approaches infinity, denoted as lim n → ∞ a n \lim_{n \to \infty} a_n lim n → ∞ a n
Cauchy sequences are sequences where the terms become arbitrarily close to each other as n n n increases
Formally, for any ε > 0 \varepsilon > 0 ε > 0 , there exists an N N N such that ∣ a n − a m ∣ < ε |a_n - a_m| < \varepsilon ∣ a n − a m ∣ < ε for all n , m > N n, m > N n , m > N
Every convergent sequence is a Cauchy sequence, but not every Cauchy sequence converges (in general metric spaces)
Absolute convergence occurs when the series ∑ n = 1 ∞ ∣ a n ∣ \sum_{n=1}^{\infty} |a_n| ∑ n = 1 ∞ ∣ a n ∣ converges
Conditional convergence occurs when a series converges, but not absolutely
Series and Their Properties
Arithmetic series are the sum of an arithmetic sequence, with the formula S n = n 2 ( a 1 + a n ) S_n = \frac{n}{2}(a_1 + a_n) S n = 2 n ( a 1 + a n )
Geometric series are the sum of a geometric sequence, with the formula S n = a 1 ( 1 − r n ) 1 − r S_n = \frac{a_1(1-r^n)}{1-r} S n = 1 − r a 1 ( 1 − r n ) for r ≠ 1 r \neq 1 r = 1
Geometric series converge if ∣ r ∣ < 1 |r| < 1 ∣ r ∣ < 1 and diverge if ∣ r ∣ ≥ 1 |r| \geq 1 ∣ r ∣ ≥ 1
Telescoping series are series where most terms cancel out, leaving only a few terms that determine the sum
Example: ∑ n = 1 ∞ ( 1 n − 1 n + 1 ) \sum_{n=1}^{\infty} (\frac{1}{n} - \frac{1}{n+1}) ∑ n = 1 ∞ ( n 1 − n + 1 1 ) telescopes to 1 1 1
The harmonic series ∑ n = 1 ∞ 1 n \sum_{n=1}^{\infty} \frac{1}{n} ∑ n = 1 ∞ n 1 diverges, despite the terms approaching 0
The alternating harmonic series ∑ n = 1 ∞ ( − 1 ) n + 1 n \sum_{n=1}^{\infty} \frac{(-1)^{n+1}}{n} ∑ n = 1 ∞ n ( − 1 ) n + 1 converges to ln ( 2 ) \ln(2) ln ( 2 )
The comparison test compares a series to a known convergent or divergent series to determine its convergence or divergence
The limit comparison test compares the limit of the ratio of corresponding terms of two series to determine convergence or divergence
Tests for Convergence
The nth term test states that if lim n → ∞ a n ≠ 0 \lim_{n \to \infty} a_n \neq 0 lim n → ∞ a n = 0 , then ∑ n = 1 ∞ a n \sum_{n=1}^{\infty} a_n ∑ n = 1 ∞ a n diverges
Note: The converse is not true; if the limit is 0, the series may converge or diverge
The integral test compares a series to an improper integral to determine convergence or divergence
If ∫ 1 ∞ f ( x ) d x \int_1^{\infty} f(x) dx ∫ 1 ∞ f ( x ) d x converges, then ∑ n = 1 ∞ f ( n ) \sum_{n=1}^{\infty} f(n) ∑ n = 1 ∞ f ( n ) converges
If ∫ 1 ∞ f ( x ) d x \int_1^{\infty} f(x) dx ∫ 1 ∞ f ( x ) d x diverges, then ∑ n = 1 ∞ f ( n ) \sum_{n=1}^{\infty} f(n) ∑ n = 1 ∞ f ( n ) diverges
The ratio test compares the limit of the ratio of consecutive terms to determine convergence or divergence
If lim n → ∞ ∣ a n + 1 a n ∣ < 1 \lim_{n \to \infty} |\frac{a_{n+1}}{a_n}| < 1 lim n → ∞ ∣ a n a n + 1 ∣ < 1 , the series converges absolutely
If lim n → ∞ ∣ a n + 1 a n ∣ > 1 \lim_{n \to \infty} |\frac{a_{n+1}}{a_n}| > 1 lim n → ∞ ∣ a n a n + 1 ∣ > 1 , the series diverges
The root test compares the limit of the nth root of the absolute value of the nth term to determine convergence or divergence
If lim n → ∞ ∣ a n ∣ n < 1 \lim_{n \to \infty} \sqrt[n]{|a_n|} < 1 lim n → ∞ n ∣ a n ∣ < 1 , the series converges absolutely
If lim n → ∞ ∣ a n ∣ n > 1 \lim_{n \to \infty} \sqrt[n]{|a_n|} > 1 lim n → ∞ n ∣ a n ∣ > 1 , the series diverges
The alternating series test states that if an alternating series has terms that decrease in absolute value and approach 0, it converges
The p-series ∑ n = 1 ∞ 1 n p \sum_{n=1}^{\infty} \frac{1}{n^p} ∑ n = 1 ∞ n p 1 converges for p > 1 p > 1 p > 1 and diverges for p ≤ 1 p \leq 1 p ≤ 1
Power Series
Power series are series of the form ∑ n = 0 ∞ a n ( x − c ) n \sum_{n=0}^{\infty} a_n(x-c)^n ∑ n = 0 ∞ a n ( x − c ) n , where c c c is the center and a n a_n a n are coefficients
The interval of convergence is the range of x x x values for which the power series converges
Endpoints must be checked separately using other tests
The radius of convergence R R R is half the length of the interval of convergence, found using the ratio test
R = lim n → ∞ ∣ a n a n + 1 ∣ R = \lim_{n \to \infty} |\frac{a_n}{a_{n+1}}| R = lim n → ∞ ∣ a n + 1 a n ∣ , if the limit exists
Power series can be differentiated and integrated term by term within the interval of convergence
Taylor series are power series approximations of functions centered at a specific point c c c , with coefficients a n = f ( n ) ( c ) n ! a_n = \frac{f^{(n)}(c)}{n!} a n = n ! f ( n ) ( c )
Example: The Taylor series for e x e^x e x centered at c = 0 c=0 c = 0 is ∑ n = 0 ∞ x n n ! \sum_{n=0}^{\infty} \frac{x^n}{n!} ∑ n = 0 ∞ n ! x n
Maclaurin series are Taylor series centered at c = 0 c=0 c = 0
Applications in Calculus
Power series can be used to represent and approximate functions near a specific point
Taylor polynomials are finite approximations of functions using Taylor series, often used for approximation and error analysis
The nth degree Taylor polynomial of f ( x ) f(x) f ( x ) centered at c c c is P n ( x ) = ∑ k = 0 n f ( k ) ( c ) k ! ( x − c ) k P_n(x) = \sum_{k=0}^{n} \frac{f^{(k)}(c)}{k!}(x-c)^k P n ( x ) = ∑ k = 0 n k ! f ( k ) ( c ) ( x − c ) k
The Lagrange error bound estimates the maximum error between a function and its Taylor polynomial on an interval
If ∣ f ( n + 1 ) ( x ) ∣ ≤ M |f^{(n+1)}(x)| \leq M ∣ f ( n + 1 ) ( x ) ∣ ≤ M on [ a , b ] [a, b] [ a , b ] , then the error is bounded by M ( n + 1 ) ! ∣ x − c ∣ n + 1 \frac{M}{(n+1)!}|x-c|^{n+1} ( n + 1 )! M ∣ x − c ∣ n + 1
Series can be used to solve differential equations by assuming a power series solution and finding the coefficients
Example: The power series solution to y ′ − y = 0 y' - y = 0 y ′ − y = 0 with y ( 0 ) = 1 y(0) = 1 y ( 0 ) = 1 is y = ∑ n = 0 ∞ x n n ! y = \sum_{n=0}^{\infty} \frac{x^n}{n!} y = ∑ n = 0 ∞ n ! x n
Fourier series represent periodic functions as an infinite sum of sines and cosines, useful in signal processing and solving PDEs
The Fourier series of a function f ( x ) f(x) f ( x ) on [ − π , π ] [-\pi, \pi] [ − π , π ] is a 0 2 + ∑ n = 1 ∞ ( a n cos ( n x ) + b n sin ( n x ) ) \frac{a_0}{2} + \sum_{n=1}^{\infty} (a_n \cos(nx) + b_n \sin(nx)) 2 a 0 + ∑ n = 1 ∞ ( a n cos ( n x ) + b n sin ( n x ))
Common Pitfalls and Tips
Be careful with the index shift when working with sequences and series, as the first term may correspond to n = 0 n=0 n = 0 or n = 1 n=1 n = 1
Always check the endpoints of the interval of convergence separately, as they may behave differently from the interior
Remember that the harmonic series diverges, despite the terms approaching 0
The comparison test and the limit comparison test are most effective when the compared series are similar in behavior
When using the ratio test or the root test, if the limit equals 1, the test is inconclusive, and other tests should be used
In alternating series, the error of the partial sum is bounded by the absolute value of the next term
∣ S − S n ∣ ≤ ∣ a n + 1 ∣ |S - S_n| \leq |a_{n+1}| ∣ S − S n ∣ ≤ ∣ a n + 1 ∣ , where S S S is the sum of the series and S n S_n S n is the nth partial sum
When solving differential equations using power series, make sure to check if the solution satisfies the initial or boundary conditions
Remember that Taylor series are local approximations and may not be accurate far from the center point
When working with Fourier series, be mindful of the convergence behavior at discontinuities and the Gibbs phenomenon