2.4: The Limit Laws - Limits at Infinity (Lecture Notes)
- Page ID
- 121550
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\(\newcommand{\avec}{\mathbf a}\) \(\newcommand{\bvec}{\mathbf b}\) \(\newcommand{\cvec}{\mathbf c}\) \(\newcommand{\dvec}{\mathbf d}\) \(\newcommand{\dtil}{\widetilde{\mathbf d}}\) \(\newcommand{\evec}{\mathbf e}\) \(\newcommand{\fvec}{\mathbf f}\) \(\newcommand{\nvec}{\mathbf n}\) \(\newcommand{\pvec}{\mathbf p}\) \(\newcommand{\qvec}{\mathbf q}\) \(\newcommand{\svec}{\mathbf s}\) \(\newcommand{\tvec}{\mathbf t}\) \(\newcommand{\uvec}{\mathbf u}\) \(\newcommand{\vvec}{\mathbf v}\) \(\newcommand{\wvec}{\mathbf w}\) \(\newcommand{\xvec}{\mathbf x}\) \(\newcommand{\yvec}{\mathbf y}\) \(\newcommand{\zvec}{\mathbf z}\) \(\newcommand{\rvec}{\mathbf r}\) \(\newcommand{\mvec}{\mathbf m}\) \(\newcommand{\zerovec}{\mathbf 0}\) \(\newcommand{\onevec}{\mathbf 1}\) \(\newcommand{\real}{\mathbb R}\) \(\newcommand{\twovec}[2]{\left[\begin{array}{r}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\ctwovec}[2]{\left[\begin{array}{c}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\threevec}[3]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\cthreevec}[3]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\fourvec}[4]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\cfourvec}[4]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\fivevec}[5]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\cfivevec}[5]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\mattwo}[4]{\left[\begin{array}{rr}#1 \amp #2 \\ #3 \amp #4 \\ \end{array}\right]}\) \(\newcommand{\laspan}[1]{\text{Span}\{#1\}}\) \(\newcommand{\bcal}{\cal B}\) \(\newcommand{\ccal}{\cal C}\) \(\newcommand{\scal}{\cal S}\) \(\newcommand{\wcal}{\cal W}\) \(\newcommand{\ecal}{\cal E}\) \(\newcommand{\coords}[2]{\left\{#1\right\}_{#2}}\) \(\newcommand{\gray}[1]{\color{gray}{#1}}\) \(\newcommand{\lgray}[1]{\color{lightgray}{#1}}\) \(\newcommand{\rank}{\operatorname{rank}}\) \(\newcommand{\row}{\text{Row}}\) \(\newcommand{\col}{\text{Col}}\) \(\renewcommand{\row}{\text{Row}}\) \(\newcommand{\nul}{\text{Nul}}\) \(\newcommand{\var}{\text{Var}}\) \(\newcommand{\corr}{\text{corr}}\) \(\newcommand{\len}[1]{\left|#1\right|}\) \(\newcommand{\bbar}{\overline{\bvec}}\) \(\newcommand{\bhat}{\widehat{\bvec}}\) \(\newcommand{\bperp}{\bvec^\perp}\) \(\newcommand{\xhat}{\widehat{\xvec}}\) \(\newcommand{\vhat}{\widehat{\vvec}}\) \(\newcommand{\uhat}{\widehat{\uvec}}\) \(\newcommand{\what}{\widehat{\wvec}}\) \(\newcommand{\Sighat}{\widehat{\Sigma}}\) \(\newcommand{\lt}{<}\) \(\newcommand{\gt}{>}\) \(\newcommand{\amp}{&}\) \(\definecolor{fillinmathshade}{gray}{0.9}\)Finite Limits at Infinity and Horizontal Asymptotes
If the values of \(f(x)\) become arbitrarily close to the finite value \(L\) as \(x\) becomes sufficiently large, we say the function \(f\) has a finite limit at infinity and write
\[\lim_{x \to \infty}f(x)=L. \nonumber \]
If the values of \(f(x)\) becomes arbitrarily close to the finite value \(L\) for \(x<0\) as \(|x|\) becomes sufficiently large, we say that the function \(f\) has a finite limit at negative infinity and write
\[\lim_{x \to −\infty}f(x)=L. \nonumber \]
If the values \(f(x)\) are getting arbitrarily close to some finite value \(L\) as \(x \to \infty\) or \(x \to −\infty\), the graph of \(f\) approaches the line \(y=L\). In that case, the line \(y=L\) is a horizontal asymptote of \(f\).
Build a table of values to investigate the limit.
\[ \displaystyle \lim_{t \to -\infty}{ e^t \sin{(t)} } \nonumber \]
If \(\displaystyle \lim_{x \to \infty}f(x)=L\) or \(\displaystyle \lim_{x \to −\infty}f(x)=L\), we say the line \(y=L\) is a horizontal asymptote of \(f\).
Revisiting the Limit Laws
Let \(f(x)\) and \(g(x)\) be defined for all \(x \gt a\), where \(a\) is a real number. Assume that \(L\) and \(M\) are real numbers such that \(\displaystyle \lim_{x \to \infty}{f(x)} = L\) and \(\displaystyle \lim_{x \to \infty}{g(x)} = M\). Let \(c\) be a constant. Then, each of the following statements holds:
- Sum and Difference Laws for Limits:
\[\displaystyle \lim_{x \to \infty}{(f(x) \pm g(x))} = \lim_{x \to \infty}{f(x)} \pm \lim_{x \to \infty}{g(x)} = L \pm M \nonumber \]
- Constant Multiple Law for Limits:
\[\displaystyle \lim_{x \to \infty}{cf(x)} = c \cdot \lim_{x \to \infty}{f(x)} = c L \nonumber \]
- Product Law for Limits:
\[\displaystyle \lim_{x \to \infty}{(f(x) \cdot g(x))} = \lim_{x \to \infty}{f(x)} \cdot \lim_{x \to \infty}{g(x)} = L \cdot M \nonumber \]
- Quotient Law for Limits:
\[\displaystyle \lim_{x \to \infty}\frac{f(x)}{g(x)} = \frac{\displaystyle \lim_{x \to \infty}f(x)}{\displaystyle \lim_{x \to \infty}g(x)}=\frac{L}{M} \nonumber \]
for \(M \neq 0\).
- Power Law for Limits:
\[\displaystyle \lim_{x \to \infty}\big(f(x)\big)^n = \big(\lim_{x \to \infty}f(x)\big)^n = L^n \nonumber \]
for every positive integer \(n\).
- Root Law for Limits:
\[\displaystyle \lim_{x \to \infty}\sqrt[n]{f(x)} = \sqrt[n]{\lim_{x \to \infty} f(x)}=\sqrt[n]{L} \nonumber \]
for all \(L\) if \(n\) is odd and for \(L \geq 0\) if \(n\) is even.
Each of these Limit Laws can be adjusted for \(x \to -\infty\) as long as \(f(x)\) and \(g(x)\) are defined for all \(x \lt a\), where \(a\) is a real number.
\[ \displaystyle \lim_{x \to \infty}{x} = \infty, \nonumber \]
\[ \displaystyle \lim_{x \to -\infty}{x} = -\infty, \nonumber \]
and
\[ \displaystyle \lim_{x \to \pm \infty}{\frac{1}{x}} = 0. \nonumber \]
If \(p \gt 0\) is a rational number, then
\[ \displaystyle \lim_{x \to \infty}{\frac{1}{x^p}} = 0. \nonumber \]
If \(p \gt 0 \) is a rational number such that \(x^p\) is defined for all \(x\), then
\[ \displaystyle \lim_{x \to -\infty}{\frac{1}{x^p}} = 0. \nonumber \]
- Proof
- Let \(p\) be a rational number. The only constraint on using the Limit Laws is that the values of the limits must be finite. Therefore, \(a\) is allowed to be \(\pm \infty\). Thus,
\[ \begin{array}{rclcl} \displaystyle \lim_{x \to \infty}{\frac{1}{x^p}} & = & \displaystyle \lim_{x \to \infty}{\left(\frac{1}{x}\right)^p} & & \\ & = & \left(\displaystyle \lim_{x \to \infty}{\frac{1}{x}} \right)^p & & (\text{a mixture of the Power Law and Root Law for Limits}) \\ & = & 0^p & & (\text{by Lemma }\PageIndex{1}) \\ & = & 0 & & \\ \end{array} \nonumber \]
If we allow \(x \to -\infty\), then additional restrictions on \(p\) must be made. Specifically, since \(p\) is a rational number, it cannot be equivalent to a simplified fraction with an even denominator. Otherwise, the even denominator would imply an even-indexed root of \(x\), and this would result in imaginary numbers. Hence, as long as \(x^p\) is defined,
\[ \displaystyle \lim_{x \to -\infty}{\frac{1}{x^p}} = 0 \nonumber \]
by a similar derivation.
Evaluating Finite Limits at Infinity
Evaluate each of the following limits.
- \( \displaystyle \lim_{x \to \infty}{\frac{8.4 x^{15} - \pi x^9 + e}{4.2 x^{15} - x + 1.228}}\)
- \( \displaystyle \lim_{x \to -\infty}{\frac{\sqrt{11 + 2x + 4x^2}}{5 x - 8}}\)
- \( \displaystyle \lim_{x \to \infty}{\left(\sqrt{1 + x + 16x^2} - 4x\right)}\)
Determine the horizontal asymptote(s) for the function.
- \( f(x) = e^{-x} \)
- \( g(t) = \tanh{(t)} \)
- \( h(x) = 2 - 2^{1/x} \)
\[ \lim_{x \to \infty}{\tan^{−1}{(x)}} = \frac{\pi}{2}, \nonumber \]
\[ \lim_{x \to -\infty}{\tan^{−1}{(x)}} = −\frac{\pi}{2}, \nonumber\]
\[ \lim_{x \to \infty}{\tanh{(x)}} = 1, \nonumber\]
\[ \lim_{x \to -\infty}{\tanh{(x)}} = -1, \text{ and }\nonumber\]
\[ \lim_{x \to \infty}{b^{-x}} = 0, \text{ where }b \gt 1. \nonumber\]
Revisiting the Squeeze Theorem
Let \(f(x),g(x)\), and \(h(x)\) be defined for all \(x \gt a\), where \(a\) is a real number. If
\[f(x) \leq g(x) \leq h(x) \nonumber \]
for all \(x \gt a\) and
\[\lim_{x \to \infty}f(x)=L=\lim_{x \to \infty}h(x) \nonumber \]
where \(L\) is a real number, then \(\displaystyle \lim_{x \to \infty}g(x)=L.\)
Likewise, let \(f(x),g(x)\), and \(h(x)\) be defined for all \(x \lt a\), where \(a\) is a real number. If
\[f(x) \leq g(x) \leq h(x) \nonumber \]
for all \(x \lt a\) and
\[\lim_{x \to -\infty}f(x)=L=\lim_{x \to -\infty}h(x) \nonumber \]
where \(L\) is a real number, then \(\displaystyle \lim_{x \to -\infty}g(x)=L.\)
Evaluate the limit.
- \(\displaystyle \lim_{x \to \infty}{ e^{-3x} \sin{(x)} }\).
- \(\displaystyle \lim_{x \to \infty}{ e^{-3x} + \sin{(x)} }\).
- \(\displaystyle \lim_{x \to \infty}{\dfrac{\lfloor x \rfloor}{x}}\).
Infinite Limits at Infinity
We say a function \(f\) has an infinite limit at infinity and write
\[\lim_{x \to \infty}f(x)=\infty. \nonumber \]
if \(f(x)\) becomes arbitrarily large for \(x\) sufficiently large. We say a function has a negative infinite limit at infinity and write
\[\lim_{x \to \infty}f(x)=−\infty. \nonumber \]
if \(f(x)<0\) and \(|f(x)|\) becomes arbitrarily large for \(x\) sufficiently large. Similarly, we can define infinite limits as \(x \to −\infty.\)
- \( \displaystyle \lim_{x \to \infty} x = \infty \)
- \( \displaystyle \lim_{x \to -\infty} x = -\infty \)
- If \( p \gt 0 \), \( \displaystyle \lim_{x \to \infty} x^p = \infty \)
- If \( b > 1 \), \( \displaystyle \lim_{x \to \infty} b^x = \infty. \)
Evaluate the limit.
- \( \lim_{x \to -\infty}{ \dfrac{2x + x^2 - x^3 + x^8}{x^5 + 8x^4 - x} } \)
- \( \lim_{x \to \infty}{ e^x } \)
- \( \lim_{x \to -\infty}{ (a x^6 + b x^{11}) }, \) where \( a, b \gt 0 \).