PAGE 1

Related Rates: Rectangle Area

The length of a rectangle is increasing at a constant rate of 8 cm/s and its width is decreasing at a constant rate of 3 cm/s. How fast, in cm²/s, is the area of the rectangle increasing at the moment when the length is 20 cm and the width is 10 cm?

do NOT plug in until taking derivative
  • A. 140
  • B. 130
  • C. 40
  • D. 24
  • E. 20
A simple rectangle diagram with the horizontal side labeled x and the vertical side labeled y.
  • x: length
  • y: width
given:
\[ \frac{dx}{dt} = 8 \]
\[ \frac{dy}{dt} = -3 \]
find:
\[ \frac{dA}{dt} \text{ when } x=20, y=10 \]

\[ A = xy \]

both \( x \) and \( y \) are functions of \( t \) (time)

\[ \frac{d}{dt} A = \frac{d}{dt} (xy) = x \frac{dy}{dt} + y \frac{dx}{dt} \]

now we can plug in numbers

\[ = x(-3) + y(8) \]

\[ = -3x + 8y \]

at the moment when \( x=20, y=10 \)

\[ \frac{dA}{dt} = -60 + 80 = \boxed{20} \]

increasing at 20 cm²/s

PAGE 2

Linear Approximation

Use a linear approximation to estimate the value of \( e^{-0.01} \)

  • A. 1.001
  • B. 1.01
  • C. 0.9
  • D. 0.99
  • E. 0.999

linear approx: \[ L = f(a) + f'(a)(x-a) \]

identify \( f(x) \): \( e^x \)

a: a convenient number where we know \( f(a) \) easily and close to where we want to be

here, we use \( a=0 \) since we know \( e^0 = 1 \) and \( 0 \) is close to \( -0.01 \)

\[ L = f(a) + f'(a)(x-a) \]

  • \( f(a) = e^0 = 1 \)
  • \( f'(x) = e^x \)
  • \( f'(a) = e^0 = 1 \)

\[ L = 1 + (1)(x-0) = 1 + x \approx e^x \]

\[ e^{-0.01} \approx 1 + (-0.01) = 0.99 \]

PAGE 3

Absolute Extrema on a Closed Interval

Note: Always work with a given closed interval.

Find the absolute maximum and minimum values of the function \( f(x) = \cos x + \sin x \) on the interval \( [0, \pi] \).

A. max: \( \sqrt{2} \); min: \( -1 \)

B. max: \( \frac{\pi}{4} \); min: \( \pi \)

C. max: 2; min: -2

D. max: 1; min: -1

E. max: \( \pi \); min: 0

Procedure:

  1. Find critical pts \( \rightarrow f' = 0 \) or \( f' \text{ DNE} \)
  2. Then compare \( f(x) \) at critical pts and at the end points of interval

We do NOT use first or second derivative test with absolute max/min.

Step-by-Step Solution

\( f'(x) = -\sin x + \cos x = 0 \)

Solve \( \cos x = \sin x \) on \( [0, \pi] \)

or \( \tan x = 1 \) on \( [0, \pi] \)

\( x = \pi/4 \) only crit. pt.

Compare \( f(x) = \cos x + \sin x \) at \( x = 0, \pi/4, \pi \):

\( f(0) = 1 \)

\( f(\pi/4) = \frac{\sqrt{2}}{2} + \frac{\sqrt{2}}{2} = \sqrt{2} \approx 1.4 \quad \text{ (max)} \)

\( f(\pi) = -1 \quad \text{ (min)} \)

PAGE 4

Evaluating Limits with L'Hospital's Rule

\( \lim_{x \to \pi} \frac{\cos x + \sin 2x + 1}{x^2 - \pi^2} = \frac{-1 + 0 + 1}{\pi^2 - \pi^2} \rightarrow \frac{0}{0} \)

A. \( \frac{1}{2\pi} \)

B. \( \frac{1}{\pi} \)

C. 1

D. \( -\frac{1}{\pi} \)

E. \( -\frac{1}{2\pi} \)

L'Hospital's Rule

  • When limit seems to go to \( \frac{0}{0} \) or \( \frac{\infty}{\infty} \)
  • Take the deriv. of top and bottom and then re-evaluate limit
  • Repeat until no longer \( \frac{0}{0} \) or \( \frac{\infty}{\infty} \)

Application

\( \stackrel{L}{=} \lim_{x \to \pi} \frac{-\sin x + 2\cos 2x}{2x} \)

Now try \( x = \pi \):

\( = \frac{-\sin(\pi) + 2\cos(2\pi)}{2\pi} = \frac{2}{2\pi} = \frac{1}{\pi} \)

Do NOT apply l'Hospital's Rule because not \( \frac{0}{0} \) or \( \frac{\infty}{\infty} \).

PAGE 5

Evaluating Indeterminate Limits

\[ \lim_{x \to 0} (1 + 2x)^{\cot x} = \]

As \( x \to 0 \), the expression takes the form \( 1^{\infty} \), which is an indeterminate form.

Strategy: Turn into \( \frac{0}{0} \) or \( \frac{\infty}{\infty} \) then use L'Hôpital's Rule.

Let \( y = (1 + 2x)^{\cot x} \). We want to find \( \lim_{x \to 0} y \).

Taking the natural logarithm of both sides:

\[ \ln y = \ln (1 + 2x)^{\cot x} \]\[ \ln y = (\cot x) \ln (1 + 2x) \]\[ \ln y = \frac{\ln (1 + 2x)}{\tan x} \]

Multiple Choice Options:

  • A. 0
  • B. 1
  • C. 2
  • D. \( e \)
  • E. \( e^2 \)

Note: as \( x \to 0 \), \( \frac{\ln (1 + 2x)}{\tan x} \to \frac{0}{0} \). So we can use L'Hôpital's Rule to find \( \lim_{x \to 0} \ln y \).

PAGE 6

Applying L'Hôpital's Rule

\[ \lim_{x \to 0} \ln y = \lim_{x \to 0} \frac{\ln (1 + 2x)}{\tan x} \]\[ \stackrel{L}{=} \lim_{x \to 0} \frac{\frac{2}{1 + 2x}}{\sec^2 x} \]

Recall: \( \sec x = \frac{1}{\cos x} \) and \( \cos(0) = 1 \)

If \( x = 0 \):

\[ = \frac{\frac{2}{1}}{1} = 2 \]

Final Result

Not done: \( \lim_{x \to 0} \ln y = 2 \) but we want \( \lim_{x \to 0} y \).

\[ y = e^{\ln y} = e^2 \]

The correct answer is E.

PAGE 7

Find the locations ( \(x\)  values) of the inflection points of \(f(x) = e^{-x^2}\). Note that its first and second derivatives are: \(f'(x) = -2xe^{-x^2}\), \(f''(x) = (4x^2 - 2)e^{-x^2}\).

  1. A. \(x = 1\) and \(x = -1\)
  2. B. \(x = 2\) and \(x = -2\)
  3. C. \(x = 0\)
  4. D. \(x = \sqrt{2}\) and \(x = -\sqrt{2}\)
  5. E. \(x = \frac{1}{\sqrt{2}}\) and \(x = -\frac{1}{\sqrt{2}}\)

inflection pts: \(f'' = 0\) or \(f''\) DNE

and \(f''\) changes sign

\[f'' = (4x^2 - 2)e^{-x^2} = 0\]

\[4x^2 - 2 = 0 \quad \text{or} \quad e^{-x^2} = 0\]

\(e^{-x^2} = 0\) never

\[x^2 = \frac{1}{2}\]

\[x = \frac{1}{\sqrt{2}}, -\frac{1}{\sqrt{2}}\]

Sign Analysis

Sign chart for f'' with roots at -\frac{1}{\sqrt{2}} and \frac{1}{\sqrt{2}}, showing concavity changes.

Sign change across both, so both are where inflection pts are.

\[f''(-2) > 0 \quad f''(0) = -2 \quad f''(2) > 0\]

PAGE 8

A six-sided box is to have four clear plastic sides, a wooden square top, and a wooden square bottom. The volume of the box must be \(24 \text{ ft}^3\). Plastic costs \(\$1\) per \(\text{ft}^2\) and wood costs \(\$3\) per \(\text{ft}^2\). Find the dimensions of the box which minimize cost.

  1. A. \(2 \text{ ft} \times 2 \text{ ft} \times 6 \text{ ft}\)
  2. B. \(\sqrt{6} \text{ ft} \times \sqrt{6} \text{ ft} \times 4 \text{ ft}\)
  3. C. \(\sqrt[3]{4} \text{ ft} \times \sqrt[3]{4} \text{ ft} \times 6\sqrt[3]{4} \text{ ft}\)
  4. D. \(\sqrt[3]{3} \text{ ft} \times \sqrt[3]{3} \text{ ft} \times 8\sqrt[3]{3} \text{ ft}\)
  5. E. \(2\sqrt[3]{2} \text{ ft} \times 2\sqrt[3]{2} \text{ ft} \times 3\sqrt[3]{2} \text{ ft}\)
Diagram of a rectangular prism with square base sides labeled x and height labeled y.

Optimization Setup

\(\text{volume} = x^2y = 24\) (constraint)

\(\text{cost} = (x^2)(3) + (x^2)(3) + (4)(xy)(1)\)

basetopfour sides

\[= 6x^2 + 4xy\]

Solving for Dimensions

Eliminate \(y\) using constraint:

\[x^2y = 24 \rightarrow y = \frac{24}{x^2}\]

\[C(x) = 6x^2 + 4x\left(\frac{24}{x^2}\right) = 6x^2 + \frac{96}{x}\]

\[C'(x) = 12x - \frac{96}{x^2} = 0 \rightarrow 12x = \frac{96}{x^2} \rightarrow x^3 = \frac{96}{12} = 8 \rightarrow x = 2\]

\[y = \frac{24}{x^2} = 6\]

Verification

Check \(x=2\) minimizes cost using 2nd deriv. test:

\[C'' = 12 + \frac{192}{x^3}\]

\[C''(2) > 0 \text{ so } x=2 \text{ min } C\]

PAGE 9

F17 E3 #4

\[f(x) = \frac{\ln x}{x^2} \text{ on } [\frac{1}{e}, e]\]

Find abs. max/min

Find critical numbers: \(f' = 0\) or \(f' \text{ DNE}\)

\[f'(x) = \frac{(x^2)(\frac{1}{x}) - (\ln x)(2x)}{(x^2)^2} = \frac{x - 2x \ln x}{x^4}\]
\[f' = 0 \rightarrow x - 2x \ln x = 0\]\[x(1 - 2 \ln x) = 0\]

\(x \neq 0\)

discard because not in \([\frac{1}{e}, e]\)

or \(1 - 2 \ln x = 0\)

\(\ln x = \frac{1}{2}\)

\(x = e^{1/2}\) keep

\[f' \text{ DNE} \rightarrow x^4 = 0 \rightarrow x \neq 0\]

\(f(\frac{1}{e}) = \frac{\ln \frac{1}{e}}{(\frac{1}{e})^2} = \frac{-1}{\frac{1}{e^2}} = -e^2\)

min

\(f(e^{1/2}) = \frac{\ln e^{1/2}}{(e^{1/2})^2} = \frac{1/2}{e} = \frac{1}{2e}\)

max

\(f(e) = \frac{\ln e}{e^2} = \frac{1}{e^2}\)

PAGE 10

F17 E3 #4

\[\sqrt{9.1}\]

Identify \(f(x)\):

\(f(x) = \sqrt{x} = x^{1/2}\)

Identify \(a\):

close to 9.1 and \(\sqrt{a}\) is known

so, \(a = 9\)

\(L = f(a) + f'(a)(x - a)\)

\(f(a) = \sqrt{9} = 3\)

\(f'(x) = \frac{1}{2}x^{-1/2} = \frac{1}{2\sqrt{x}}\)

\(f'(a) = f'(9) = \frac{1}{2\sqrt{9}} = \frac{1}{6}\)

\[L = 3 + \frac{1}{6}(x - 9) \approx \sqrt{x}\]
\[\sqrt{9.1} \approx 3 + \frac{1}{6}(0.1) = 3 + \frac{1}{60} = 3\frac{1}{60}\]