MATH 1560 Final Exam Study Guide

MATH:1560 Final Exam Overview and Point Distribution

  • The final exam for MATH:1560 is worth a total of 200200 points.

  • Exam 1 Content (30 points): Consists of 66 Multiple Choice Questions covering:     - Convergence Test     - Approximate area under curve     - Definite Integral geometrically     - Geometric Series     - Sequence Convergence     - Taylor polynomials

  • Exam 2 Content (30 points): Consists of 66 Multiple Choice Questions covering:     - Integration by parts     - Partial Fractions     - Trig Sub     - Area Between Curves     - Improper Integral     - Probability

  • Chapter 8 Content (60 points): Consists of 1212 Multiple Choice Questions covering:     - Work (2 questions)     - Parametrized curves     - Projections     - Cross Product     - Arc Length (Parametric or Polar)     - Partial Derivative     - Derivatives in Polar Coordinates     - Polar Coordinate Conversion     - Vector Valued Functions     - Surface Area     - Vertical or Horizontal Definite Integral

  • Free Response Section (80 points total): There are four free-response questions, each worth 2020 points:     - Power Series (2020 points)     - Arc Length (2020 points)     - Center of Mass (2020 points)     - Area in Polar Coordinates (2020 points)

Sequence and Series Convergence Analysis

  • Direct Comparison Test Application: If the condition 0≤an≤3n2+10 \le a_n \le \frac{3}{n^2 + 1} holds for all nn, the Direct Comparison Test is used to determine the convergence of ∑n=1∞an\sum_{n=1}^{\infty} a_n. Since ∑n=1∞3n2\sum_{n=1}^{\infty} \frac{3}{n^2} is a convergent p-series (p=2>1p = 2 > 1), and 3n2+1<3n2\frac{3}{n^2+1} < \frac{3}{n^2}, the series ∑n=1∞an\sum_{n=1}^{\infty} a_n must also converge.

  • Sequence Convergence Evaluation: For the sequence an=5n−28n+7a_n = \frac{5n - 2}{8n + 7}, convergence is determined by calculating the limit as n→∞n \rightarrow \infty:     - lim⁡n→∞5n−28n+7=58\lim_{n \to \infty} \frac{5n - 2}{8n + 7} = \frac{5}{8}     - The sequence converges to 58\frac{5}{8}.

  • Geometric Series Summation: For the series ∑n=0∞73n\sum_{n=0}^{\infty} \frac{7}{3^n}, it is a geometric series where the first term a=7a = 7 and the common ratio r=13r = \frac{1}{3}. Since ∣r∣<1|r| < 1, the series converges. The sum is calculated as:     - S = \frac{a}{1 - r} = \frac{7}{1 - \frac{1}{3}} = \frac{7}{\frac{2}{3}} = \frac{21}{2}

  • Divergence Test / Comparison: To determine the convergence of ∑n=1∞n+4n2+1\sum_{n=1}^{\infty} \frac{n + 4}{n^2 + 1}, one can use the Limit Comparison Test with the harmonic series bn=1nb_n = \frac{1}{n}. This series behaves like 1n\frac{1}{n} at infinity and thus diverges.

Power Series and Taylor Polynomials

  • Radius of Convergence Calculation: For the power series ∑n=1∞n0˘001x40˘002n\sum_{n=1}^{\infty} n \u0001\frac{x}{4}\u0002^n, the radius of convergence RR is found using the Ratio Test:     - L=lim⁡n→∞∣(n+1)xn+14n+1×4nnxn∣=∣x∣4L = \lim_{n \to \infty} \left| \frac{(n+1)x^{n+1}}{4^{n+1}} \times \frac{4^n}{nx^n} \right| = \frac{|x|}{4}     - Set L<1→∣x∣4<1→∣x∣<4L < 1 \rightarrow \frac{|x|}{4} < 1 \rightarrow |x| < 4. Thus, R=4R = 4.

  • Interval of Convergence Evaluation: For the series ∑n=1∞(x−2)nn5n\sum_{n=1}^{\infty} \frac{(x - 2)^n}{n 5^n}, the interval is found by the Ratio Test:     - L=lim⁡n→∞∣(x−2)n+1(n+1)5n+1×n5n(x−2)n∣=∣x−2∣5L = \lim_{n \to \infty} \left| \frac{(x-2)^{n+1}}{(n+1)5^{n+1}} \times \frac{n 5^n}{(x-2)^n} \right| = \frac{|x-2|}{5}     - Centralized at x=2x=2 with radius 55. Boundaries are at x=−3x = -3 and x=7x = 7.     - At x=7x = 7, the series is the harmonic series (diverges).     - At x=−3x = -3, the series is the alternating harmonic series (converges).     - Interval: [−3,7)[-3, 7).

  • Power Series Representations:     - For 1(1−x)2\frac{1}{(1-x)^2}, one can differentiate the known series 11−x=∑xn\frac{1}{1-x} = \sum x^n term-by-term.     - For ∫0x11+t2dt\int_0^x \frac{1}{1+t^2} dt, which is arctan⁡(x)\arctan(x), the representation is derived from the integration of the series for 11+t2=∑n=0∞(−1)nt2n\frac{1}{1+t^2} = \sum_{n=0}^{\infty} (-1)^n t^{2n}, resulting in ∑n=0∞(−1)nx2n+12n+1\sum_{n=0}^{\infty} \frac{(-1)^n x^{2n+1}}{2n+1}.

  • Maclaurin and Taylor Polynomials:     - For e−x2e^{-x^2}, the first four nonzero terms of the Maclaurin series are 1−x2+x42−x661 - x^2 + \frac{x^4}{2} - \frac{x^6}{6}.     - Degree 3 Taylor Polynomial (T3(x)T_3(x)) centered at 00 for a function where f(0)=3f(0) = 3, f′(0)=2f'(0) = 2, f′′(0)=−4f''(0) = -4, and f(3)(0)=12f^{(3)}(0) = 12:         - T3(x)=f(0)+f′(0)x+f′′(0)2!x2+f(3)(0)3!x3T_3(x) = f(0) + f'(0)x + \frac{f''(0)}{2!}x^2 + \frac{f^{(3)}(0)}{3!}x^3         - T3(x)=3+2x−2x2+2x3T_3(x) = 3 + 2x - 2x^2 + 2x^3

Riemann Sums and Work Integrals

  • Area Approximations:     - Left-endpoint Riemann sum for y=x2+1y = x^2 + 1 on [0,4][0, 4] with n=4n = 4 (Δx=1\Delta x = 1): 1×[f(0)+f(1)+f(2)+f(3)]=1×[1+2+5+10]=181 \times [f(0) + f(1) + f(2) + f(3)] = 1 \times [1 + 2 + 5 + 10] = 18.     - Midpoint approximation for ∫15xdx\int_1^5 \sqrt{x} dx with 44 rectangles (Δx=1\Delta x = 1): ∑i=14i+0.5\sum_{i=1}^4 \sqrt{i + 0.5}, specifically f(1.5)+f(2.5)+f(3.5)+f(4.5)f(1.5) + f(2.5) + f(3.5) + f(4.5).

  • Work Scenarios:     - Cable and Crate: A crate weighing 120120 lbs is lifted 4040 ft by a cable weighing 1.51.5 lb/ft. The work integral is W=∫040(120+1.5(40−y))dyW = \int_0^{40} (120 + 1.5(40 - y)) dy.     - Rocket Weigh: Weight decreases linearly from 500500 lbs at y=0y=0 to 420420 lbs at y=800y=800. The weight function is w(y)=500−110yw(y) = 500 - \frac{1}{10}y. The work integral is W=∫0800(500−0.1y)dyW = \int_0^{800} (500 - 0.1y) dy.     - Pumping Water: A cylindrical tank (radius 33, height 1010) full of water (62.462.4 lb/ft). The work to pump all water to the top: W=∫010π(3)2(62.4)(10−y)dyW = \int_0^{10} \pi(3)^2 (62.4)(10 - y) dy.

Vector Operations and Geometry

  • Projections and Products:     - Given u=⟨2,−1⟩\mathbf{u} = \langle 2, -1 \rangle and v=⟨3,4⟩\mathbf{v} = \langle 3, 4 \rangle, the projection of u\mathbf{u} onto v\mathbf{v} is proj<em>v(u)=u⋅v∣v∣2v\text{proj}<em>{\mathbf{v}}(\mathbf{u}) = \frac{\mathbf{u} \cdot \mathbf{v}}{|\mathbf{v}|^2} \mathbf{v}.         - u⋅v=(2)(3)+(−1)(4)=2\mathbf{u} \cdot \mathbf{v} = (2)(3) + (-1)(4) = 2         - ∣v∣2=32+42=25|\mathbf{v}|^2 = 3^2 + 4^2 = 25         - proj</em>v(u)=225⟨3,4⟩=⟨625,825⟩\text{proj}</em>{\mathbf{v}}(\mathbf{u}) = \frac{2}{25} \langle 3, 4 \rangle = \langle \frac{6}{25}, \frac{8}{25} \rangle     - Dot product of ⟨1,2,3⟩\langle 1, 2, 3 \rangle and ⟨−1,4,0⟩\langle -1, 4, 0 \rangle: (1)(−1)+(2)(4)+(3)(0)=7(1)(-1) + (2)(4) + (3)(0) = 7.     - Cross product of ⟨2,1,−1⟩×⟨1,3,2⟩\langle 2, 1, -1 \rangle \times \langle 1, 3, 2 \rangle results in ⟨5,−5,5⟩\langle 5, -5, 5 \rangle.

  • Lines and Planes:     - Angle between ⟨1,1,0⟩\langle 1, 1, 0 \rangle and ⟨1,0,1⟩\langle 1, 0, 1 \rangle is found using cos⁡(θ)=122=12\cos(\theta) = \frac{1}{\sqrt{2} \sqrt{2}} = \frac{1}{2}, so θ=π3\theta = \frac{\pi}{3}.     - Vector equation of a line through (1,−2,3)(1, -2, 3) parallel to ⟨2,5,−1⟩\langle 2, 5, -1 \rangle: r(t)=⟨1,−2,3⟩+t⟨2,5,−1⟩\mathbf{r}(t) = \langle 1, -2, 3 \rangle + t \langle 2, 5, -1 \rangle.     - Plane equation through (1,0,2)(1, 0, 2) with normal ⟨3,−1,4⟩\langle 3, -1, 4 \rangle: 3(x−1)−1(y−0)+4(z−2)=03(x - 1) - 1(y - 0) + 4(z - 2) = 0, which simplifies to 3x−y+4z=113x - y + 4z = 11.

Parametric and Polar Calculus

  • Parametric Derivatives: For curve x=t3+1x = t^3 + 1 and y=t2−4ty = t^2 - 4t, the derivative is dydx=dy/dtdx/dt=2t−43t2\frac{dy}{dx} = \frac{dy/dt}{dx/dt} = \frac{2t - 4}{3t^2}.

  • Arc Length of Parametric Curves: For x=t2,y=2t3x = t^2, y = 2t^3 for 0≤t≤10 \le t \le 1, the integral is L=∫01(2t)2+(6t2)2dt=∫014t2+36t4dtL = \int_0^1 \sqrt{(2t)^2 + (6t^2)^2} dt = \int_0^1 \sqrt{4t^2 + 36t^4} dt.

  • Polar Coordinates:     - Polar to Cartesian: r=4sin⁡(θ)r = 4 \sin(\theta) becomes r2=4rsin⁡(θ)→x2+y2=4yr^2 = 4r \sin(\theta) \rightarrow x^2 + y^2 = 4y.     - Slope of polar curve r=1+2cos⁡(θ)r = 1 + 2 \cos(\theta) at θ=π3\theta = \frac{\pi}{3}: Requires \frac{dy}{dx} = \frac{dr/d\theta \sin(\theta) + r \cos(\theta)}{dr/d\theta \cos(\theta) - r \sin(\theta)}.

  • Polar Area Integration:     - Area inside r=3−3cos⁡(θ)r = 3 - 3 \cos(\theta): A=∫02π12(3−3cos⁡(θ))2dθA = \int_0^{2\pi} \frac{1}{2} (3 - 3 \cos(\theta))^2 d\theta.     - Shared area between circles r=2r = 2 and r=2cos⁡(θ)r = 2 \cos(\theta), finding intersection points to establish integration limits.

Advanced Integration and Multivariable Calculus

  • Integration Methods:     - Integration by Parts (IBP): ∫xe2xdx\int x e^{2x} dx and ∫xcos⁡(4x)dx\int x \cos(4x) dx.     - Partial Fractions: ∫1x2−4dx\int \frac{1}{x^2 - 4} dx and ∫3x+5x2+x−2dx\int \frac{3x + 5}{x^2 + x - 2} dx.     - Trigonometric Substitution: For ∫x21−x2dx\int \frac{x^2}{\sqrt{1 - x^2}} dx, use x=sin⁡(θ)x = \sin(\theta), dx=cos⁡(θ)dθdx = \cos(\theta) d\theta, resulting in ∫sin⁡2(θ)cos⁡(θ)cos⁡(θ)dθ=∫sin⁡2(θ)dθ\int \frac{\sin^2(\theta)}{\cos(\theta)} \cos(\theta) d\theta = \int \sin^2(\theta) d\theta.

  • Improper Integrals:     - ∫1∞1x3/2dx\int_1^{\infty} \frac{1}{x^{3/2}} dx: Converges to 22.     - ∫011xdx\int_0^1 \frac{1}{\sqrt{x}} dx: Converges to 22.

  • Partial Derivatives:     - For f(x,y)=x3y2+excos⁡(y)f(x, y) = x^3 y^2 + e^x \cos(y), the partial derivative with respect to xx is fx=3x2y2+excos⁡(y)f_x = 3x^2 y^2 + e^x \cos(y).     - For f(x,y)=x2eysin⁡(y)f(x, y) = x^2 e^y \sin(y), finding fxyf_{xy} requires differentiating fx=2xeysin⁡(y)f_x = 2x e^y \sin(y) with respect to yy: fxy=2x(eysin⁡(y)+eycos⁡(y))f_{xy} = 2x (e^y \sin(y) + e^y \cos(y)).

Area, Surface Area, Mass, and Probability

  • Geometric Area:     - Between y=x2y = x^2 and y=2xy = 2x: Integate 2x−x22x - x^2 from 00 to 22.     - Between x=y3x = y^3 and y=xy = x: Integrate y1/3−yy^{1/3} - y or x−x3x - x^3 depending on intersection boundaries.

  • Surface Area of Rotation:     - For y=x+1y = \sqrt{x + 1} on [0,3][0, 3] around x-axis: S=∫032πx+11+0˘00112x+10˘0022dxS = \int_0^3 2\pi \sqrt{x+1} \sqrt{1 + \u0001\frac{1}{2\sqrt{x+1}}\u0002^2} dx.     - For y=ln⁡(x)y = \ln(x) on [1,e2][1, e^2] about x-axis (with respect to yy): Since x=eyx = e^y, the range is 0≤y≤20 \le y \le 2; S=∫022πy1+(ey)2dyS = \int_0^2 2\pi y \sqrt{1 + (e^y)^2} dy.

  • Mass and Moments:     - For region bounded by y=3xy = 3x and y=x2y = x^2 on [0,3][0, 3] with density ρ(x)=2x\rho(x) = 2x:         - Mass M=∫032x(3x−x2)dxM = \int_0^3 2x(3x - x^2) dx.         - Moment about y-axis My=∫03x(2x)(3x−x2)dxM_y = \int_0^3 x(2x)(3x - x^2) dx.         - Moment about x-axis Mx=∫0312(2x)((3x)2−(x2)2)dx=∫03x(9x2−x4)dxM_x = \int_0^3 \frac{1}{2} (2x) ((3x)^2 - (x^2)^2) dx = \int_0^3 x (9x^2 - x^4) dx .

  • Probability Distributions:     - Verification of PDF: For f(x)=6x(1−x)f(x) = 6x(1 - x) on [0,1][0, 1], checking ∫01f(x)dx=1\int_0^1 f(x) dx = 1 is necessary.     - Variance: For density f(x)=38x2f(x) = \frac{3}{8}x^2 on [0,2][0, 2], variance is calculated as V(X)=E[X2]−(E[X])2V(X) = E[X^2] - (E[X])^2.         - E[X]=∫02x⋅38x2dx=∫0238x3dx=[332x4]02=4832=1.5E[X] = \int_0^2 x \cdot \frac{3}{8}x^2 dx = \int_0^2 \frac{3}{8}x^3 dx = \left[ \frac{3}{32}x^4 \right]_0^2 = \frac{48}{32} = 1.5.         - E[X2]=∫02x2⋅38x2dx=∫0238x4dx=[340x5]02=9640=2.4E[X^2] = \int_0^2 x^2 \cdot \frac{3}{8}x^2 dx = \int_0^2 \frac{3}{8}x^4 dx = \left[ \frac{3}{40}x^5 \right]_0^2 = \frac{96}{40} = 2.4.         - Variance V(x)=2.4−(1.5)2=2.4−2.25=0.15V(x) = 2.4 - (1.5)^2 = 2.4 - 2.25 = 0.15.