University Mathematics II Compendium: From Infinite Series to Multivariable Calculus

Book Metadata and Author Information

  • Title: University Mathematics II (2017).

  • Target Courses: Applied Mathematics II, Calculus II, and Calculus of Functions of Several Variables.

  • Authors: Addisu W/Meskel (M.Sc.), Bizuneh Minda (M.Sc.), Getachew Bitew (M.Sc.), Temesgen Alemu (M.Sc.), and Tilahun Esayiyas (M.Sc.).

  • Affiliation: Lecturers of Mathematics at Addis Ababa University, Ethiopia.

  • Previous Work: University Mathematics I.

  • Publication Date: January, 2017.

  • Content Summary: The material contains two main parts:     * Part I: Infinite Series: Chapters 1–3 covering Sequences and Series, Power Series, and Fourier Series.     * Part II: Calculus of Functions of Several Variables: Chapters 4–7 covering Preliminaries, Limits and Continuity, Partial Derivatives and Applications, and Multiple Integrals.

Chapter 1: Sequences and Series

1.1 Definition of a Sequence

  • General Definition: A sequence is an ordered collection of objects or events with an identified first, second, and third member.

  • Mathematical Definition (1.1.1): A sequence is a function from the set of integers greater than or equal to some integer m0m_0 (usually 0 or 1) into a nonempty set XX.

  • Real Sequence: If the range is a subset of real numbers (RR), it is a sequence of real numbers. This chapter focuses exclusively on real sequences.

  • Notation:     * General term: ana_n in place of a(n)a(n).     * Terms: a1,a2,a3,,an,a_1, a_2, a_3, \dots, a_n, \dots     * Ordered pairs representation: (1,a1),(2,a2),,(n,an),{(1, a_1), (2, a_2), \dots, (n, a_n), \dots}.     * Shorthand: an{a_n} or ann=1{a_n}_{n=1}^{\infty}.

  • Description Methods:     1. Listing: Writing the first few terms (e.g., 2,4,6,8,{2, 4, 6, 8, \dots} where an=2na_n = 2n).     2. Defining Formula: Giving a specific rule for ana_n. For an=2nn1a_n = \frac{2^n}{n-1}, the smallest value is n=2n=2.     3. Recursive Definition: Defining a term using preceding terms (recurrence).         * Positive odd numbers: a1=1a_1 = 1 and an+1=an+2,n1a_{n+1} = a_n + 2, \forall n \ge 1.         * Fibonacci Sequence: 1,1,2,3,5,8,13,21,34,1, 1, 2, 3, 5, 8, 13, 21, 34, \dots s.t. a1=a2=1a_1 = a_2 = 1 and an+2=an+1+an,n2a_{n+2} = a_{n+1} + a_n, \forall n \ge 2.     4. Verbally: For cases with no obvious pattern, like the sequence of prime numbers.

  • Special Types:     * Stationary Sequence: an=an+1a_n = a_{n+1} for all natural numbers nn.     * Equality: an=bn{a_n} = {b_n} if an=bn,na_n = b_n, \forall n.

  • Graph of a Sequence: Consists of isolated points on a coordinate plane with coordinates (n0,an0),(n1,an1),(n_0, a_{n_0}), (n_1, a_{n_1}), \dots.

1.2 Convergence and Divergence of Sequences

  • Formal Definition (1.2.1): A sequence an{a_n} has the limit LL if for every \varepsilon > 0, there exists a positive integer NN (dependent on ε\varepsilon) such that for every n > N, |a_n - L| < \varepsilon.     * Notation: limnan=L\lim_{n \to \infty} a_n = L or anLa_n \to L as nn \to \infty.     * A sequence is convergent if the limit exists; otherwise, it is divergent.

  • Geometric Representation: The points (n,an)(n, a_n) must lie between the horizontal lines y=L+εy = L + \varepsilon and y=Lεy = L - \varepsilon for all n > N.

  • Theorem 1.2.1: If f(n)=anf(n) = a_n for a real-valued function ff, then limxf(x)=L    limnan=L\lim_{x \to \infty} f(x) = L \implies \lim_{n \to \infty} a_n = L.     * Caution: The converse is not always true. Example: cos(2πn)1\cos(2\pi n) \to 1, but limxcos(2πx)\lim_{x \to \infty} \cos(2\pi x) does not exist.

  • Types of Divergent Sequences:     * Diverge to \infty: \forall M > 0, \exists N \text{ s.t. } n > N \implies a_n > M.     * Diverge to -\infty: \forall m > 0, \exists N \text{ s.t. } n > N \implies a_n < m.     * Oscillating: Sequences that diverge but not to ±\pm\infty.

  • Null Sequence: A sequence that converges to zero.

  • Geometric Sequences: The sequence crn{cr^n} converges if -1 < r \le 1.     * Limit is 0 if -1 < r < 1.     * Limit is cc if r=1r = 1.

Chapter 2: Power Series

  • Definition (2.0.1): A power series in (xa)(x-a) is a series of the form:     n=0cn(xa)n=c0+c1(xa)+c2(xa)2+c3(xa)3+\sum_{n=0}^{\infty} c_n(x-a)^n = c_0 + c_1(x-a) + c_2(x-a)^2 + c_3(x-a)^3 + \dots     where xx is a variable, cnc_n are constants (coefficients), and aa is the center.

  • Radius and Interval of Convergence:     * Theorem 2.1.1: Exactly one of the following is true:         1. Converges only at x=ax = a (R=0R = 0).         2. Absolutely convergent for all xx (R=R = \infty).         3. \exists R > 0 such that series converges if |x-a| < R and diverges if |x-a| > R.     * Abel’s Theorem (2.2.3): Relates the function limit to the series sum at endpoints of the interval of convergence.

  • Differentiation and Integration (2.1.4): A power series P(x)P(x) with R > 0 is differentiable and integrable on (aR,a+R)(a-R, a+R) term by term. The radius RR remains unchanged.

  • Uniqueness Theorem (2.2.1): If f(x)f(x) is represented by a power series, the coefficients are cn=f(n)(a)n!c_n = \frac{f^{(n)}(a)}{n!}.

  • Taylor Series: The power series representation f(x)=n=0f(n)(a)n!(xa)nf(x) = \sum_{n=0}^{\infty} \frac{f^{(n)}(a)}{n!}(x-a)^n.     * Maclaurin Series: A Taylor series centered at a=0a = 0.

  • Common Series Representations:     * ex=n=0xnn!e^x = \sum_{n=0}^{\infty} \frac{x^n}{n!} for all xx.     * sin(x)=n=0(1)nx2n+1(2n+1)!\sin(x) = \sum_{n=0}^{\infty} (-1)^n \frac{x^{2n+1}}{(2n+1)!}.     * cos(x)=n=0(1)nx2n(2n)!\cos(x) = \sum_{n=0}^{\infty} (-1)^n \frac{x^{2n}}{(2n)!}.     * 11x=n=0xn\frac{1}{1-x} = \sum_{n=0}^{\infty} x^n for |x| < 1.     * ln(1+x)=n=1(1)n1xnn\ln(1+x) = \sum_{n=1}^{\infty} (-1)^{n-1} \frac{x^n}{n} for -1 < x \le 1.

  • Binomial Series (2.4.1): For any real mm, (1+x)m=n=0(mn)xn(1+x)^m = \sum_{n=0}^{\infty} \binom{m}{n} x^n where (mn)=m(m1)(mn+1)n!\binom{m}{n} = \frac{m(m-1)\dots(m-n+1)}{n!}. Converges for |x| < 1.

Chapter 3: Fourier Series

  • Periodic Functions: f(x+P)=f(x)f(x + P) = f(x). The smallest PP is the fundamental period.

  • Inner Product (3.1.4): (f,g)=abf(x)g(x)dx(f, g) = \int_a^b f(x)g(x) dx. Two functions are orthogonal if their inner product is zero.

  • Fourier Series (3.2.1): For a 2π2\pi-periodic function ff, the series is:     f(x)a02+n=1(ancos(nx)+bnsin(nx))f(x) \sim \frac{a_0}{2} + \sum_{n=1}^{\infty} (a_n \cos(nx) + b_n \sin(nx))     * Euler Formulas:         * a0=1πaa+2πf(x)dxa_0 = \frac{1}{\pi} \int_a^{a+2\pi} f(x) dx         * an=1πaa+2πf(x)cos(nx)dxa_n = \frac{1}{\pi} \int_a^{a+2\pi} f(x) \cos(nx) dx         * bn=1πaa+2πf(x)sin(nx)dxb_n = \frac{1}{\pi} \int_a^{a+2\pi} f(x) \sin(nx) dx

  • Arbitrary Period 2l:     f(x)a02+n=1(ancosnπxl+bnsinnπxl)f(x) \sim \frac{a_0}{2} + \sum_{n=1}^{\infty} (a_n \cos\frac{n\pi x}{l} + b_n \sin\frac{n\pi x}{l})

  • Special Cases:     * Even Functions: Only cosine terms exist (bn=0b_n = 0). an=2l0lf(x)cosnπxldxa_n = \frac{2}{l} \int_0^l f(x) \cos\frac{n\pi x}{l} dx.     * Odd Functions: Only sine terms exist (an=0a_n = 0). bn=2l0lf(x)sinnπxldxb_n = \frac{2}{l} \int_0^l f(x) \sin\frac{n\pi x}{l} dx.

  • Dirichlet Convergence Theorem (3.3.1): If ff and ff' are piecewise continuous and ff is periodic, the series converges to f(x)f(x) at continuity points and to the average of limits f(c+)+f(c)2\frac{f(c^+) + f(c^-)}{2} at discontinuities.

  • Parseval's Identity (3.7): 1lll[f(x)]2dx=a022+n=1(an2+bn2)\frac{1}{l} \int_{-l}^l [f(x)]^2 dx = \frac{a_0^2}{2} + \sum_{n=1}^{\infty} (a_n^2 + b_n^2).

  • Fourier Transform: f(w)=12πf(t)eiwtdtf(w) = \frac{1}{\sqrt{2\pi}} \int_{-\infty}^{\infty} f(t) e^{-iwt} dt.

Chapter 5: Limits and Continuity in Multiple Variables

  • Definition 5.1.1: A function of two variables assigns a unique number f(x,y)f(x, y) to each pair (x,y)(x, y) in domain DD.

  • Limit Definition (5.3.2): lim(x,y)(a,b)f(x,y)=L\lim_{(x,y) \to (a,b)} f(x, y) = L if \forall \varepsilon > 0, \exists \delta > 0 s.t. 0 < \sqrt{(x-a)^2 + (y-b)^2} < \delta \implies |f(x, y) - L| < \varepsilon.

  • Path Dependency: If f(x,y)f(x, y) approaches different values along different paths to (a,b)(a, b), the limit does not exist.

  • Continuity (5.4.2): ff is continuous at (a,b)(a, b) if lim(x,y)(a,b)f(x,y)=f(a,b)\lim_{(x,y) \to (a,b)} f(x, y) = f(a, b).

  • Squeeze Theorem (5.3.1): If fghf \le g \le h and limf=limh=L\lim f = \lim h = L, then limg=L\lim g = L.

Chapter 6: Partial Derivatives and Applications

  • Definition 6.1.1:     * With respect to xx: fx(x,y)=limh0f(x+h,y)f(x,y)hf_x(x, y) = \lim_{h \to 0} \frac{f(x+h, y) - f(x, y)}{h}.     * With respect to yy: fy(x,y)=limh0f(x,y+h)f(x,y)hf_y(x, y) = \lim_{h \to 0} \frac{f(x, y+h) - f(x, y)}{h}.

  • Clairaut's Theorem (6.2.1): If fxyf_{xy} and fyxf_{yx} are continuous, then fxy=fyxf_{xy} = f_{yx}.

  • Chain Rule:     * One independent variable: dzdt=zxdxdt+zydydt\frac{dz}{dt} = \frac{\partial z}{\partial x} \frac{dx}{dt} + \frac{\partial z}{\partial y} \frac{dy}{dt}.

  • Implicit Differentiation (6.5.1): If f(x,y,z)=0f(x, y, z) = 0, then zx=fxfz\frac{\partial z}{\partial x} = -\frac{f_x}{f_z} and zy=fyfz\frac{\partial z}{\partial y} = -\frac{f_y}{f_z}.

  • Directional Derivative (6.6.1): In direction of unit vector u=(a,b)\mathbf{u} = (a, b), Duf=fxa+fyb=fuD_{\mathbf{u}}f = f_x a + f_y b = \nabla f \cdot \mathbf{u}.

  • Gradient Vector: f=(fx,fy)\nabla f = (f_x, f_y).     * ff increases most rapidly in the direction of f\nabla f.     * Maximum rate of change is f||\nabla f||.

  • Tangent Plane (6.7.1): For z=f(x,y)z = f(x, y), the equation is zz0=fx(x0,y0)(xx0)+fy(x0,y0)(yy0)z - z_0 = f_x(x_0, y_0)(x - x_0) + f_y(x_0, y_0)(y - y_0).

  • Optimization:     * Second Partials Test: D=fxxfyy(fxy)2D = f_{xx}f_{yy} - (f_{xy})^2.         * D > 0 and f_{xx} > 0: Relative minimum.         * D > 0 and f_{xx} < 0: Relative maximum.         * D < 0: Saddle point.         * D=0D = 0: Inconclusive.     * Lagrange Multipliers: To maximize/minimize ff subject to g=kg = k, solve f=λg\nabla f = \lambda \nabla g.

Chapter 7: Multiple Integrals

  • Fubini’s Theorem (7.1.1): Allows evaluation of double integrals as iterated integrals over rectangles: Rf(x,y)dA=abcdf(x,y)dydx=cdabf(x,y)dxdy\iint_R f(x, y) dA = \int_a^b \int_c^d f(x, y) dy dx = \int_c^d \int_a^b f(x, y) dx dy.

  • Polar Coordinates Integration: Rf(x,y)dA=αβabf(rcosθ,rsinθ)rdrdθ\iint_R f(x, y) dA = \int_{\alpha}^{\beta} \int_a^b f(r \cos \theta, r \sin \theta) r dr d\theta.

  • Surface Area (7.1.7): SA=R(fx)2+(fy)2+1dASA = \iint_R \sqrt{(f_x)^2 + (f_y)^2 + 1} dA.

  • Triple Integrals:     * Cylindrical: Uses (r,θ,z)(r, \theta, z), volume element dV=rdzdrdθdV = r dz dr d\theta.     * Spherical: Uses (ρ,θ,ϕ)(\rho, \theta, \phi), volume element dV=ρ2sinϕdρdθdϕdV = \rho^2 \sin \phi d\rho d\theta d\phi.

  • Change of Variables (7.3.1): Rf(x,y)dxdy=Sf(x(u,v),y(u,v))J(u,v)dudv\iint_R f(x, y) dx dy = \iint_S f(x(u, v), y(u, v)) |J(u, v)| du dv where J(u,v)=(x,y)(u,v)J(u, v) = \frac{\partial(x,y)}{\partial(u,v)} is the Jacobian.