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.github/workflows/pretext-cli.yml

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.github/workflows/pretext-deploy.yml

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source/chap-3.xml

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<title>Using Derivatives</title>
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<xi:include href="./sec-3-1-rel-rates.xml" />
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<xi:include href="./sec-3-2-LHR.xml" />
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<!-- <xi:include href="./sec-3-3-tests.xml" /> -->
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<!-- <xi:include href="./sec-3-4-families.xml" /> -->
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<!-- <xi:include href="./sec-3-5-optimization.xml" /> -->
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<!-- <xi:include href="./sec-3-6-applied-opt.xml" /> -->
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<xi:include href="./sec-3-3-tests.xml" />
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<xi:include href="./sec-3-4-families.xml" />
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<xi:include href="./sec-3-5-optimization.xml" />
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</chapter>
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<section xmlns:xi="http://www.w3.org/2001/XInclude" xml:id="sec-3-4-families">
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<title>Using derivatives to describe families of functions</title>
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<objectives>
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<!-- <objectives>
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<ul>
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<li>
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<p>
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</p>
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</li>
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</ul>
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</objectives>
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<subsection><title>Introduction</title>
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<p>
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Mathematicians are often interested in making general observations to describe patterns that hold in a large number of related situations.
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Think about the Pythagorean Theorem:
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it doesn't tell us something about a single right triangle,
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but rather a fact about <em>every</em> right triangle.
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In the next part of our studies,
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we use calculus to make general observations about families of functions that depend on one or more parameters.
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People who use applied mathematics,
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such as engineers and economists,
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often encounter the same types of functions where only small changes to certain constants occur.
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These constants are called <em>parameters</em>.
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</p>
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<figure xml:id="F-3-2-SineFam">
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<caption>The graph of <m>f(t) = a \sin(b(t-c)) + d</m> based on parameters <m>a</m>, <m>b</m>, <m>c</m>, and <m>d</m>.</caption>
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<image width="65%" source="images/3_2_SineFam"/>
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</figure>
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<p>
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You are already familiar with certain families of functions.
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For example,
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<me>
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f(t) = a \sin(b(t-c)) + d
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</me>
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is a stretched and shifted version of the sine function with amplitude <m>a</m>,
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period <m>\frac{2\pi}{b}</m>,
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phase shift <m>c</m>, and vertical shift <m>d</m>.
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We know that <m>a</m> affects the size of the oscillation,
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<m>b</m> the rapidity of oscillation,
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and <m>c</m> where the oscillation starts,
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as shown in <xref ref="F-3-2-SineFam">Figure</xref>,
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while <m>d</m> affects the vertical positioning of the graph.
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</p>
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<p>
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As another example, every function of the form
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<m>y = mx + b</m> is a line with slope <m>m</m> and <m>y</m>-intercept <m>(0,b)</m>.
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The value of <m>m</m> affects the line's steepness,
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and the value of <m>b</m> situates the line vertically on the coordinate axes.
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These two parameters describe all possible non-vertical lines.
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</p>
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</objectives> -->
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<subsection xml:id="subsec-families-foundations">
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<title>Foundations</title>
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<p>
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For other less familiar families of functions,
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we can use calculus to discover where key behavior occurs:
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where members of the family are increasing or decreasing,
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concave up or concave down,
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where relative extremes occur, and more,
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all in terms of the parameters involved.
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To get started,
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we revisit a common collection of functions to see how calculus confirms things we already know.
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</p>
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<xi:include href="./previews/PA-3-4-WW.xml" />
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<xi:include href="./previews/PA-3-4.xml" />
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</subsection>
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<xi:include href="./proteus/proteus-3-2.xml" />
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<subsection>
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<title>Describing families of functions in terms of parameters</title>
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<p>
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Our goal is to describe the key characteristics of the overall behavior of each member of a family of functions in terms of its parameters.
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By finding the first and second derivatives and constructing sign charts
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(each of which may depend on one or more of the parameters),
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we can often make broad conclusions about how each member of the family will appear.
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</p>
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<example xml:id="Ex-3-2-1">
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<statement>
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<p>
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Consider the two-parameter family of functions given by <m>g(x) = axe^{-bx}</m>,
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where <m>a</m> and <m>b</m> are positive real numbers.
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Fully describe the behavior of a typical member of the family in terms of <m>a</m> and <m>b</m>,
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including the location of all critical numbers,
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where <m>g</m> is increasing, decreasing, concave up,
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and concave down, and the long term behavior of <m>g</m>.
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</p>
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</statement>
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<solution>
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<p>
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We begin by computing <m>g'(x)</m>.
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By the product rule,
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<me>
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g'(x) = ax \frac{d}{dx}\left[e^{-bx}\right] + e^{-bx} \frac{d}{dx}[ax]
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</me>.
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By applying the chain rule and constant multiple rule,
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we find that
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<me>
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g'(x) = axe^{-bx}(-b) + e^{-bx}(a)
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</me>.
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</p>
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<p>
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To find the critical numbers of <m>g</m>,
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we solve the equation <m>g'(x) = 0</m>.
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By factoring <m>g'(x)</m>, we find
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<me>
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0 = ae^{-bx}(-bx + 1)
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</me>.
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</p>
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<p>
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Since we are given that <m>a \ne 0</m> and we know that
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<m>e^{-bx} \ne 0</m> for all values of <m>x</m>,
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the only way this equation can hold is when <m>-bx + 1 = 0</m>.
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Solving for <m>x</m>, we find <m>x = \frac{1}{b}</m>,
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and this is therefore the only critical number of <m>g</m>.
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</p>
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<p>
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We construct the first derivative sign chart for <m>g</m> that is shown in <xref ref="F-3-2-signchartg">Figure</xref>.
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</p>
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<figure xml:id="F-3-2-signchartg">
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<caption>The first derivative sign chart for <m>g(x) = axe^{-bx}</m>.</caption>
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<image width="45%" source="images/3_2_signchartg"/>
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</figure>
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<p>
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Because the factor <m>ae^{-bx}</m> is always positive,
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the sign of <m>g'</m> depends on the linear factor <m>(1-bx)</m>,
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which is positive for
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<m>x \lt \frac{1}{b}</m> and negative for <m>x \gt \frac{1}{b}</m>.
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Hence we can conclude that <m>g</m> is always increasing for
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<m>x \lt \frac{1}{b}</m> and decreasing for <m>x \gt \frac{1}{b}</m>,
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and also that <m>g</m> has a global maximum at
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<m>(\frac{1}{b}, g(\frac{1}{b}))</m> and no local minimum.
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</p>
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<p>
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We turn next to analyzing the concavity of <m>g</m>.
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With <m>g'(x) = -abxe^{-bx} + ae^{-bx}</m>,
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we differentiate to find that
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<me>
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g''(x) = -abxe^{-bx}(-b) + e^{-bx}(-ab) + ae^{-bx}(-b)
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</me>.
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</p>
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<p>
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Combining like terms and factoring, we now have
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<me>
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g''(x) = ab^2xe^{-bx} - 2abe^{-bx} = abe^{-bx}(bx - 2)
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</me>.
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</p>
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<figure xml:id="F-3-2-signchartg2">
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<caption>The second derivative sign chart for <m>g(x) = axe^{-bx}</m>.</caption>
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<image width="45%" source="images/3_2_signchartg2"/>
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</figure>
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<p>
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We observe that <m>abe^{-bx}</m> is always positive,
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and thus the sign of <m>g''</m> depends on the sign of <m>(bx-2)</m>,
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which is zero when <m>x = \frac{2}{b}</m>.
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Since <m>b</m> is positive,
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the value of <m>(bx-2)</m> is negative for
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<m>x \lt \frac{2}{b}</m> and positive for <m>x \gt \frac{2}{b}</m>.
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The sign chart for <m>g''</m> is shown in <xref ref="F-3-2-signchartg2">Figure</xref>.
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Thus, <m>g</m> is concave down for all
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<m>x \lt \frac{2}{b}</m> and concave up for all <m>x \gt \frac{2}{b}</m>.
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</p>
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<p>
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Finally, we analyze the long term behavior of <m>g</m> by considering two limits.
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First, we note that
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<me>
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\lim_{x \to \infty} g(x) = \lim_{x \to \infty} axe^{-bx} = \lim_{x \to \infty} \frac{ax}{e^{bx}}
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</me>.
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</p>
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<p>
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This limit has indeterminate form <m>\frac{\infty}{\infty}</m>, so
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we apply L'Hôpital's Rule and find that <m>\lim_{x \to \infty} g(x) = 0</m>.
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In the other direction,
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<me>
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\lim_{x \to -\infty} g(x) = \lim_{x \to -\infty} axe^{-bx} = -\infty
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</me>,
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because <m>ax \to -\infty</m> and
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<m>e^{-bx} \to \infty</m> as <m>x \to -\infty</m>.
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Hence, as we move left on its graph,
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<m>g</m> decreases without bound,
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while as we move to the right, <m>g(x) \to 0</m>.
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</p>
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<p>
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All of this information now helps us produce the graph of a typical member of this family of functions without using a graphing utility
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(and without choosing particular values for <m>a</m> and <m>b</m>),
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as shown in <xref ref="F-3-2-SurgeFam">Figure</xref>.
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</p>
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<figure xml:id="F-3-2-SurgeFam">
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<caption>The graph of <m>g(x) = axe^{-bx}</m>.</caption>
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<image width="80%" source="images/3_2_SurgeFam"/>
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</figure>
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<p>
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Note that the value of <m>b</m> controls the horizontal location of the global maximum and the inflection point,
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as neither depends on <m>a</m>.
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The value of <m>a</m> affects the vertical stretch of the graph.
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For example,
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the global maximum occurs at the point <m>(\frac{1}{b}, g(\frac{1}{b})) = (\frac{1}{b}, \frac{a}{b}e^{-1})</m>,
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so the larger the value of <m>a</m>,
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the greater the value of the global maximum.
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</p>
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</solution>
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</example>
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<p>
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The work we've completed in <xref ref="Ex-3-2-1">Example</xref>
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can often be replicated for other families of functions that depend on parameters.
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Normally we are most interested in determining all critical numbers,
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a first derivative sign chart,
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a second derivative sign chart,
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and the limit of the function as <m>x \to \infty</m>.
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Throughout,
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we prefer to work with the parameters as arbitrary constants.
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In addition,
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we can experiment with some particular values of the parameters present to reduce the algebraic complexity of our work.
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The following activities offer several key examples where we see that the values of the parameters substantially affect the behavior of individual functions within a given family.
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</p>
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<xi:include href="./activities/act-3-4-1.xml"/>
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<xi:include href="./activities/act-3-4-2.xml"/>
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<xi:include href="./activities/act-3-4-3.xml"/>
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</subsection>
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<subsection>
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<title>Summary</title>
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<p>
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<ul>
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<li>
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<p>
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Given a family of functions that depends on one or more parameters,
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by investigating how critical numbers and locations where the second derivative is zero depend on the values of these parameters,
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we can often accurately describe the shape of the function in terms of the parameters.
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</p>
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</li>
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<li>
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<p>
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In particular,
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just as we can create first and second derivative sign charts for a single function,
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we can often do so for entire families of functions where critical numbers and possible inflection points depend on arbitrary constants.
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These sign charts then reveal where members of the family are increasing or decreasing,
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concave up or concave down,
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and help us to identify relative extremes and inflection points.
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</p>
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</li>
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</ul>
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Coming soon.
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</p>
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</subsection>
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<xi:include href="./exercises/ez-3-4.xml"/>
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<exercises xml:id="cp-families">
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<title>Calculus Practice</title>
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<introduction>
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<p>
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Coming soon.
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</p>
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</introduction>
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</exercises>
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</section>

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