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Work Required to Pump Water from a Cylindrical Tank

A cylindrical tank of height 4 feet and radius 1 foot is filled with water. How much work is required to pump all but 1 foot of water out of the tank. (Density = \(62.5 \text{ lbs.}/\text{ft}^3\))

Note: Density in lbs./ft³ is force, no gravity to multiply. kg is a mass so mult. by \(g = 9.8\).

Cylindrical tank diagram with height 4, radius 1, and a water slice at height y with thickness dy.
  • A \(9\pi(62.5) \text{ ft-lbs.}\)
  • B \(3\pi(62.5) \text{ ft-lbs.}\)
  • C \(\frac{9\pi}{2}(62.5) \text{ ft-lbs.}\)
  • D \(18\pi(62.5) \text{ ft-lbs.}\)
  • E \(6\pi(62.5) \text{ ft-lbs.}\)

Solution Steps

work = force \(\cdot\) distance

Work to move one slice of water then integrate over water to move:

\(\text{work of slice} = (\text{weight}) (\text{distance to go})\)

\(= (62.5)(\pi)(1)^2(dy) \cdot (4-y)\)

\(= 62.5\pi (4-y)dy\)

\[ \int_{1}^{4} 62.5\pi (4-y)dy \]\[ = 62.5\pi \left( 4y - \frac{1}{2}y^2 \right) \Big|_1^4 \]\[ = 62.5\pi \left[ (16-8) - (4 - \frac{1}{2}) \right] = 62.5\pi \left( 8 - \frac{7}{2} \right) \]\[ = 62.5\pi \left( \frac{9}{2} \right) \]
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Integration by Parts Evaluation

Evaluate \[ \int_{0}^{1} xe^{3x} dx \]

  • A. \(\frac{2e^3}{9}\)
  • B \(\frac{1}{9} + \frac{2e^3}{9}\)
  • C. 1
  • D. \(\frac{1}{9}\)
  • E. \(\frac{e^3}{9} - 1\)

Method: Integration by Parts

By parts: \(uv - \int v du\)

Order to pick \(u\): LIATE

  • L: Logarithmic
  • I: Inverse trig
  • A: Algebraic (here, \(x\))
  • T: Trig
  • E: Exponential (here, \(e^{3x}\))

Here, \(x\) is Algebraic and \(e^{3x}\) is Exponential, so:

\(u = x\)

\(du = dx\)

\(dv = e^{3x} dx\)

\(v = \frac{1}{3}e^{3x}\)

\[ uv \Big|_0^1 - \int_{0}^{1} v du = \frac{1}{3}xe^{3x} \Big|_0^1 - \int_{0}^{1} \frac{1}{3}e^{3x} dx \]\[ = \frac{1}{3}xe^{3x} \Big|_0^1 - \frac{1}{9}e^{3x} \Big|_0^1 \]\[ = \frac{1}{3}e^3 - \frac{1}{9}e^3 + \frac{1}{9} = \frac{2}{9}e^3 + \frac{1}{9} \]
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Basic Trig Integrals

Basic trig integrals: \( \cos x, \sin x \rightarrow u = \cos x \) or \( u = \sin x \). Move powers around to make things fit.

\[ \int_{0}^{\pi/2} \sin^3 x dx = \]
A. 2/3
B. 4/3
C. 0
D. 1/4
E. 1/3

Solution Strategy

\[ \int_{0}^{\pi/2} \sin^2 x \cdot \sin x dx \]

Using identity: \( \sin^2 x = 1 - \cos^2 x \)

Substitution:

If \( u = \cos x \), then \( du = -\sin x dx \)

We have this part in the integral.

\[ = \int_{0}^{\pi/2} (1 - \cos^2 x) \sin x dx \]

\( u = \cos x \)

\( du = -\sin x dx \)

Definite Integral Calculation

\[ = \int_{1}^{0} -(1 - u^2) du = -u + \frac{1}{3}u^3 \Big|_1^0 = 0 - (-1 + \frac{1}{3}) = \frac{2}{3} \]

or back-substituting:

\[ -u + \frac{1}{3}u^3 \Big|_{x=0}^{x=\pi/2} = -\cos x + \frac{1}{3}\cos^3 x \Big|_0^{\pi/2} = \dots = \frac{2}{3} \]
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\[ \int_{0}^{\pi/4} \sec^4 x \tan x dx = \]
A. 1
B. 1/3
C. 4/3
D. 3/4
E. 2/9

Substitution Options

  • If \( u = \tan x \) then \( du = \sec^2 x dx \)
  • If \( u = \sec x \) then \( du = \sec x \tan x dx \)

Step-by-Step Solution

\[ \int_{0}^{\pi/4} \sec^4 x \tan x dx = \int_{0}^{\pi/4} \sec^2 x \cdot \tan x \cdot \sec^2 x dx \]

\( \sec^2 x = \tan^2 x + 1 \)

\( = u^2 + 1 \)

\( \tan x = u \)

\( \sec^2 x dx = du \)

if \( u = \tan x \)

Changing limits: when \( x = \pi/4, u = \tan(\pi/4) = 1 \). When \( x = 0, u = 0 \).

\[ = \int_{0}^{1} (u^2 + 1)(u) du = \int_{0}^{1} (u^3 + u) du \]
\[ = \frac{u^4}{4} + \frac{u^2}{2} \Big|_0^1 = \frac{1}{4} + \frac{1}{2} = \frac{3}{4} \]
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Definite Integral with Substitution

Evaluate the following definite integral using $u$-substitution:

\[ \int_{0}^{\pi/4} \sec^4 x \tan x \, dx \]

Substitution:

If \( u = \sec x \),

then \( du = \sec x \tan x \, dx \)

Rewrite the integral to isolate the \( du \) term:

\[ = \int_{0}^{\pi/4} \sec^3 x (\sec x \tan x) \, dx \]

Change the limits of integration and substitute \( u \):

\[ = \int_{1}^{\sqrt{2}} u^3 \, du = \dots \]
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Trigonometric Substitution

\[ \int \frac{dx}{\sqrt{9 - 4x^2}} = \]
  1. A. \( \sec^{-1} (\frac{3x}{2}) + C \)
  2. B. \( \frac{1}{2} \sin^{-1} (\frac{2x}{3}) + C \)
  3. C. \( \tan^{-1} (\frac{2x}{3}) + C \)
  4. D. \( \frac{1}{3} \sin^{-1} (\frac{3x}{2}) + C \)
  5. E. \( \sqrt{9 - 4x^2} + \tan^{-1} (\frac{2x}{3}) + C \)

Trigonometric Substitution Method

Trig subs: \( \sqrt{9 - 4x^2} \)

Triangle with sides: \( \sqrt{9 - 4x^2} \), \( 3 \), \( 2x \)

Hypotenuse: \( 3 \)

Adjacent: \( \sqrt{9 - 4x^2} \) (contains constant)

Right triangle with hypotenuse 3, opposite side 2x, adjacent side sqrt(9-4x^2), and angle theta.

\[ \sin \theta = \frac{2x}{3} \implies x = \frac{3}{2} \sin \theta \]

\[ dx = \frac{3}{2} \cos \theta \, d\theta \]

Substituting into the integral:

\[ \int \frac{dx}{\sqrt{9 - 4x^2}} = \int \frac{\frac{3}{2} \cos \theta \, d\theta}{\sqrt{9 - 4(\frac{9}{4} \sin^2 \theta)}} \]
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Integration by Trigonometric Substitution

\[ = \int \frac{\frac{3}{2} \cos \theta}{\sqrt{9(1 - \sin^2 \theta)}} d\theta = \int \frac{\frac{3}{2} \cos \theta}{3 \cos \theta} d\theta \]

Note: In the denominator, \( 1 - \sin^2 \theta \) simplifies to \( \cos^2 \theta \).

\[ = \int \frac{1}{2} d\theta = \frac{1}{2} \theta + C = \frac{1}{2} \sin^{-1} \left( \frac{2x}{3} \right) + C \]

Back Substitution

To return to the original variable \( x \):

\[ \text{back to } \sin \theta = \frac{2}{3} x \]\[ \theta = \sin^{-1} \left( \frac{2}{3} x \right) \]
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Integration by Partial Fractions

\[ \int \frac{x + 1}{x^3 - 2x^2 + x} dx = \]

A. \( \ln |x| + \ln |x - 1| + C \)

B. \( \ln |x| - \ln |x - 1| + C \)

C. \( \ln |x| - \frac{2}{x - 1} + C \)

D. \( \ln |x - 1| - \frac{2}{x - 1} + C \)

E. \( \ln |x| - \ln |x - 1| - \frac{2}{x - 1} + C \)

Partial Fraction Decomposition

\[ \frac{x + 1}{x(x^2 - 2x + 1)} = \frac{x + 1}{(x)(x - 1)(x - 1)} = \frac{A}{x} + \frac{B}{x - 1} + \frac{C}{(x - 1)^2} \]

The factors are linear (\( x \)) and repeated linear (\( (x - 1)^2 \)).

Solving for Coefficients

Multiply by \( (x)(x - 1)(x - 1) \):

\[ x + 1 = A(x - 1)^2 + B(x)(x - 1) + C(x) \]\[ = A(x^2 - 2x + 1) + B(x^2 - x) + Cx \]\[ 0x^2 + 1x + 1 = (A + B)x^2 + (-2A - B + C)x + A \]
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So,

\( A + B = 0 \)

\( -2A - B + C = 1 \)

\( A = 1 \)

\( B = -1 \)

Substituting these values into the second equation:

\[ -2(1) - (-1) + C = 1 \]\[ -2 + 1 + C = 1 \]\[ C = 2 \]

Integration by Partial Fractions

\[ \int \left( \frac{1}{x} - \frac{1}{x-1} + \frac{2}{(x-1)^2} \right) dx \]\[ = \int \frac{1}{x} dx - \int \frac{1}{x-1} dx + 2 \int \frac{1}{(x-1)^2} dx \]

Let \( u = x - 1 \)

\( du = dx \)

\[ = \int \frac{1}{x} dx - \int \frac{1}{x-1} dx + 2 \int \frac{1}{u^2} du \]\[ = \ln|x| - \ln|x-1| - \frac{2}{u} + C \]\[ = \ln|x| - \ln|x-1| - \frac{2}{x-1} + C \]
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Indicate convergence or divergence for each of the following improper integrals:

\( (I) \int_{2}^{\infty} \frac{1}{(x-1)^2} dx \)
conv.
\( (II) \int_{0}^{2} \frac{1}{(x-1)^2} dx \)
div.
\( (III) \int_{0}^{1} \frac{\ln x}{x} dx \)
div.

A. I converges, II and III diverge.

B. II converges, I and III diverge.

C. I and III converge, II diverges.

D. I and II converge, III diverges.

E. I, II and III diverge.

I. Evaluation of Integral I

\[ \lim_{a \to \infty} \int_{2}^{a} \frac{1}{(x-1)^2} dx = \lim_{a \to \infty} \left. -\frac{1}{(x-1)} \right|_{2}^{a} \]\[ = \lim_{a \to \infty} \left( -\frac{1}{a-1} \right) + \frac{1}{1} = 1 \]

Note: \( -\frac{1}{a-1} \to 0 \) as \( a \to \infty \).

II. Evaluation of Integral II

trouble at \( x = 1 \)

\[ \int_{0}^{1} \frac{1}{(x-1)^2} dx + \int_{1}^{2} \frac{1}{(x-1)^2} dx \]\[ = \lim_{a \to 1^-} \int_{0}^{a} \frac{1}{(x-1)^2} dx + \lim_{b \to 1^+} \int_{b}^{2} \frac{1}{(x-1)^2} dx \]
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Improper Integrals and Divergence

\[= \lim_{a \to 1^-} \left. -\frac{1}{x-1} \right|_0^a + \lim_{b \to 1^+} \left. -\frac{1}{x-1} \right|_b^2\]
\[= \lim_{a \to 1^-} \left( -\frac{1}{a-1} - 1 \right) + \lim_{b \to 1^+} \left( -1 + \frac{1}{b-1} \right)\]

As \( a \to 1^- \):

\[ \frac{1}{a-1} = \frac{1}{\text{small negative}} = -\infty \]

\[= \infty + \text{whatever}\]

One part diverges, so the whole thing diverges.

Example IV

\[ \int_0^1 \frac{\ln x}{x} dx = \lim_{a \to 0^+} \int_a^1 \frac{\ln x}{x} dx \]

Substitution:

\( u = \ln x \)

\( du = \frac{1}{x} dx \)

\[ = \lim_{a \to 0^+} \int_{\ln a}^0 u \, du = \lim_{a \to 0^+} \left. \frac{1}{2} u^2 \right|_{\ln a}^0 \]
\[ = \lim_{a \to 0^+} 0 - \frac{1}{2} (\ln a)^2 \]

Note: As \( a \to 0^+ \), \( \ln a \to -\infty \).