Active Calculus · 2: Computing Derivatives

2.8: Using Derivatives to Evaluate Limits

Motivating Questions
  • How can derivatives be used to help us evaluate indeterminate limits of the form 00?\frac{0}{0}\text{?}
  • What does it mean to say that lim⁡x→∞f(x)=L\lim_{x \to \infty} f(x) = L and lim⁡x→af(x)=∞?\lim_{x \to a} f(x) = \infty\text{?}
  • How can derivatives assist us in evaluating indeterminate limits of the form ∞∞?\frac{\infty}{\infty}\text{?}

Because differential calculus is based on the definition of the derivative, and the definition of the derivative involves a limit, there is a sense in which all of calculus rests on limits. In addition, the limit involved in the definition of the derivative always generates the indeterminate form 00.\frac{0}{0}\text{.} If ff is a differentiable function, then in the definition

f′(x)=lim⁡h→0f(x+h)−f(x)h, f'(x) = \lim_{h \to 0} \frac{f(x+h)-f(x)}{h}\text{,}

not only does h→0h \to 0 in the denominator, but also (f(x+h)−f(x))→0(f(x+h)-f(x)) \to 0 in the numerator, since ff is continuous. Remember, saying that a limit has an indeterminate form only means that we don't yet know its value and have more work to do: indeed, limits of the form 00\frac{0}{0} can take on any value, as is evidenced by evaluating f′(x)f'(x) for varying values of xx for a function such as f′(x)=x2.f'(x) = x^2\text{.}

We have learned many techniques for evaluating the limits that result from the derivative definition, including a large number of shortcut rules. In this section, we turn the situation upside-down: instead of using limits to evaluate derivatives, we explore how to use derivatives to evaluate certain limits.

Preview Activity 2.8.12.8.1

Let hh be the function given by h(x)=x5+x−2x2−1.h(x) = \frac{x^5 + x - 2}{x^2 - 1}\text{.}

  1. What is the domain of h?h\text{?}
  2. Explain why lim⁡x→1x5+x−2x2−1\displaystyle\lim_{x \to 1} \frac{x^5 + x - 2}{x^2 - 1} results in an indeterminate form.
  3. Next we will investigate the behavior of both the numerator and denominator of hh near the point where x=1.x = 1\text{.} Let f(x)=x5+x−2f(x) = x^5 + x - 2 and g(x)=x2−1.g(x) = x^2 - 1\text{.} Find the local linearizations of ff and gg at a=1,a = 1\text{,} and call these functions Lf(x)L_f(x) and Lg(x),L_g(x)\text{,} respectively.
  4. Explain why h(x)≈Lf(x)Lg(x)h(x) \approx \frac{L_f(x)}{L_g(x)} for xx near a=1.a = 1\text{.}
  5. Using your work from (c) and (d), evaluate
    lim⁡x→1Lf(x)Lg(x). \lim_{x \to 1} \frac{L_f(x)}{L_g(x)}\text{.}

    What do you think your result tells us about lim⁡x→1h(x)?\lim_{x \to 1} h(x)\text{?}

  6. Investigate the function h(x)h(x) graphically and numerically near x=1.x = 1\text{.} What do you think is the value of lim⁡x→1h(x)?\lim_{x \to 1} h(x)\text{?}

2.8.12.8.1 Using derivatives to evaluate indeterminate limits of the form 00.\dfrac{0}{0}\text{.}

2_8_LHR.svg

Figure 2.8.12.8.1. At left, the graphs of ff and gg near the value a,a\text{,} along with their tangent line approximations LfL_f and LgL_g at x=a.x = a\text{.} At right, zooming in on the point aa and the four graphs.

The idea demonstrated in Preview Activity 2.8.12.8.1 — that we can evaluate an indeterminate limit of the form 00\frac{0}{0} by replacing each of the numerator and denominator with their local linearizations at the point of interest — can be generalized in a way that enables us to evaluate a wide range of limits. We have a function h(x)h(x) that can be written as a quotient h(x)=f(x)g(x),h(x) = \frac{f(x)}{g(x)}\text{,} where ff and gg are both differentiable at x=ax=a and for which f(a)=g(a)=0.f(a) = g(a) = 0\text{.} We would like to evaluate the indeterminate limit given by lim⁡x→ah(x).\lim_{x \to a} h(x)\text{.} Figure 2.8.12.8.1 illustrates the situation. We see that both ff and gg have an xx-intercept at x=a.x = a\text{.} Their respective tangent line approximations LfL_f and LgL_g at x=ax = a are also shown in the figure. We can take advantage of the fact that a function and its tangent line approximation become indistinguishable as x→a.x \to a\text{.}

First, let's recall that Lf(x)=f′(a)(x−a)+f(a)L_f(x) = f'(a)(x-a) + f(a) and Lg(x)=g′(a)(x−a)+g(a).L_g(x) = g'(a)(x-a) +g(a)\text{.} Because xx is getting arbitrarily close to aa when we take the limit, we can replace ff with LfL_f and replace gg with Lg,L_g\text{,} and thus we observe that

lim⁡x→af(x)g(x)=(lim⁡x→aLf(x)Lg(x)=(lim⁡x→af′(a)(x−a)+f(a)g′(a)(x−a)+g(a).\begin{align*} \lim_{x \to a} \frac{f(x)}{g(x)} =\mathstrut & \lim_{x \to a} \frac{L_f(x)}{L_g(x)}\\[4pt] =\mathstrut & \lim_{x \to a} \frac{f'(a)(x-a) + f(a)}{g'(a)(x-a) + g(a)}\text{.} \end{align*}

Next, we remember that both f(a)=0f(a) = 0 and g(a)=0,g(a) = 0\text{,} which is precisely what makes the original limit indeterminate. Substituting these values for f(a)f(a) and g(a)g(a) in the limit above, we now have

lim⁡x→af(x)g(x)=(lim⁡x→af′(a)(x−a)g′(a)(x−a)=(lim⁡x→af′(a)g′(a),\begin{align*} \lim_{x \to a} \frac{f(x)}{g(x)} =\mathstrut & \lim_{x \to a} \frac{f'(a)(x-a)}{g'(a)(x-a)}\\[4pt] =\mathstrut & \lim_{x \to a} \frac{f'(a)}{g'(a)}\text{,} \end{align*}

where the latter equality holds because x−ax−a=1\frac{x-a}{x-a} = 1 when xx is approaching (but not equal to) a.a\text{.} Finally, we note that f′(a)g′(a)\frac{f'(a)}{g'(a)} is constant with respect to x,x\text{,} and thus

lim⁡x→af(x)g(x)=f′(a)g′(a). \lim_{x \to a} \frac{f(x)}{g(x)} = \frac{f'(a)}{g'(a)}\text{.}

This result holds as long as g′(a)g'(a) is not equal to zero. The formal name of the result is L'Hôpital's Rule.

L'Hôpital's Rule

Let ff and gg be differentiable at x=a,x=a\text{,} and suppose that f(a)=g(a)=0f(a) = g(a) = 0 and that g′(a)≠0.g'(a) \neq 0\text{.} Then lim⁡x→af(x)g(x)=f′(a)g′(a).\lim_{x \to a} \frac{f(x)}{g(x)} = \frac{f'(a)}{g'(a)}\text{.}

In practice, we typically work with a slightly more general version of L'Hôpital's Rule, which states that (under the identical assumptions as the boxed rule above and the extra assumption that g′g' is continuous at x=ax=a)

lim⁡x→af(x)g(x)=lim⁡x→af′(x)g′(x), \lim_{x \to a} \frac{f(x)}{g(x)} = \lim_{x \to a} \frac{f'(x)}{g'(x)}\text{,}

provided the righthand limit exists. This form reflects the basic idea of L'Hôpital's Rule: if f(x)g(x)\frac{f(x)}{g(x)} produces an indeterminate limit of form 00\frac{0}{0} as x→a,x \to a\text{,} that limit is equivalent to the limit of the quotient of the two functions' derivatives, f′(x)g′(x).\frac{f'(x)}{g'(x)}\text{.}

For example, if we consider the limit from Preview Activity 2.8.12.8.1 ,

lim⁡x→1x5+x−2x2−1, \lim_{x \to 1} \frac{x^5 + x - 2}{x^2 - 1}\text{,}

by L'Hôpital's Rule we have that

lim⁡x→1x5+x−2x2−1=lim⁡x→15x4+12x=62=3. \lim_{x \to 1} \frac{x^5 + x - 2}{x^2 - 1} = \lim_{x \to 1} \frac{5x^4 + 1}{2x} = \frac{6}{2} = 3. \\[4pt]

By replacing the numerator and denominator with their respective derivatives, we often replace an indeterminate limit with one whose value we can easily determine.

Activity 2.8.12.8.1

Evaluate each of the following limits. If you use L'Hôpital's Rule, indicate where it was used, and be certain its hypotheses are met before you apply it.

  1. lim⁡x→0ln⁡(1+x)x\displaystyle \lim_{x \to 0} \frac{\ln(1 + x)}{x}
  2. lim⁡x→πcos⁡(x)x\displaystyle \lim_{x \to \pi} \frac{\cos(x)}{x}
  3. lim⁡x→12ln⁡(x)1−ex−1\displaystyle \lim_{x \to 1} \frac{2 \ln(x)}{1-e^{x-1}}
  4. lim⁡x→0sin⁡(x)−xcos⁡(2x)−1\displaystyle \lim_{x \to 0} \frac{\sin(x) - x}{\cos(2x)-1}

While L'Hôpital's Rule can be applied in an entirely algebraic way, it is important to remember that the justification of the rule is graphical: the main idea is that the slopes of the tangent lines to ff and gg at x=ax = a determine the value of the limit of f(x)g(x)\frac{f(x)}{g(x)} as x→a.x \to a\text{.}

2_8_LHR2.svg

Figure 2.8.22.8.2. Two functions ff and gg that satisfy L'Hôpital's Rule.

We see this in Figure 2.8.22.8.2, where we can see from the grid that f′(a)=2f'(a) = 2 and g′(a)=−1,g'(a) = -1\text{,} hence by L'Hôpital's Rule,

lim⁡x→af(x)g(x)=f′(a)g′(a)=2−1=−2. \lim_{x \to a}\frac{f(x)}{g(x)} = \frac{f'(a)}{g'(a)} = \frac{2}{-1} = -2\text{.}

It's not the fact that ff and gg both approach zero that matters most, but rather the rate at which each approaches zero that determines the value of the limit. This is a good way to remember what L'Hôpital's Rule says: if f(a)=g(a)=0,f(a) = g(a) = 0\text{,} the the limit of f(x)g(x)\frac{f(x)}{g(x)} as x→ax \to a is given by the ratio of the slopes of ff and gg at x=a.x = a\text{.}

Activity 2.8.22.8.2

In this activity, we reason graphically from the following figure to evaluate limits of ratios of functions about which some information is known.

2_8_Act2.svg

Figure 2.8.32.8.3. Three graphs referenced in the questions of Activity 2.8.32.8.3.
  1. Use the left-hand graph to determine the values of f(2),f(2)\text{,} f′(2),f'(2)\text{,} g(2),g(2)\text{,} and g′(2).g'(2)\text{.} Then, evaluate lim⁡x→2f(x)g(x).\lim\limits_{x \to 2} \frac{f(x)}{g(x)}\text{.}
  2. Use the middle graph to find p(2),p(2)\text{,} p′(2),p'(2)\text{,} q(2),q(2)\text{,} and q′(2).q'(2)\text{.} Then, determine the value of lim⁡x→2p(x)q(x).\lim\limits_{x \to 2} \frac{p(x)}{q(x)}\text{.}
  3. Assume that rr and ss are functions whose for which r′′(2)≠0r''(2) \ne 0 and s′′(2)≠0s''(2) \ne 0 Use the right-hand graph to compute r(2),r(2)\text{,} r′(2),r'(2)\text{,} s(2),s(2)\text{,} s′(2).s'(2)\text{.} Explain why you cannot determine the exact value of lim⁡x→2r(x)s(x)\lim\limits_{x \to 2} \frac{r(x)}{s(x)} without further information being provided, but that you can determine the sign of lim⁡x→2r(x)s(x).\lim\limits_{x \to 2} \frac{r(x)}{s(x)}\text{.} In addition, state what the sign of the limit will be, with justification.

2.8.22.8.2 Limits involving ∞\infty

The concept of infinity, denoted ∞,\infty\text{,} arises naturally in calculus, as it does in much of mathematics. It is important to note from the outset that ∞\infty is a concept, but not a number itself. Indeed, the notion of ∞\infty naturally invokes the idea of limits. Consider, for example, the function f(x)=1x,f(x) = \frac{1}{x}\text{,} whose graph is pictured in Figure 2.8.42.8.4.

We note that x=0x = 0 is not in the domain of f,f\text{,} so we may naturally wonder what happens as x→0.x \to 0\text{.} As x→0+,x \to 0^+\text{,} we observe that f(x)f(x) increases without bound. That is, we can make the value of f(x)f(x) as large as we like by taking xx closer and closer (but not equal) to 0, while keeping x>0.x \gt 0\text{.} This is a good way to think about what infinity represents: a quantity is tending to infinity if there is no single number that the quantity is always less than.

2_8_Infty.svg

Figure 2.8.12.8.1. The graph of f(x)=1x.f(x) = \frac{1}{x}\text{.}

Recall that the statement lim⁡x→af(x)=L,\lim_{x \to a} f(x) = L\text{,} means that we can make f(x)f(x) as close to LL as we'd like by taking xx sufficiently close (but not equal) to a.a\text{.} We now expand this notation and language to include the possibility that either LL or aa can be ∞.\infty\text{.} For instance, for f(x)=1x,f(x) = \frac{1}{x}\text{,} we now write

lim⁡x→0+1x=∞, \lim_{x \to 0^+} \frac{1}{x} = \infty\text{,}

by which we mean that we can make 1x\frac{1}{x} as large as we like by taking xx sufficiently close (but not equal) to 0. In a similar way, we write

lim⁡x→∞1x=0, \lim_{x \to \infty} \frac{1}{x} = 0\text{,}

since we can make 1x\frac{1}{x} as close to 0 as we'd like by taking xx sufficiently large (i.e., by letting xx increase without bound).

In general, the notation lim⁡x→af(x)=∞\lim_{x \to a} f(x) = \infty means that we can make f(x)f(x) as large as we like by taking xx sufficiently close (but not equal) to a,a\text{,} and the notation lim⁡x→∞f(x)=L\lim_{x \to \infty} f(x) = L means that we can make f(x)f(x) as close to LL as we like by taking xx sufficiently large. This notation also applies to left- and right-hand limits, and to limits involving −∞.-\infty\text{.} For example, returning to Figure 2.8.42.8.4 and f(x)=1x,f(x) = \frac{1}{x}\text{,} we can say that

lim⁡x→0−1x=−∞  and  lim⁡x→−∞1x=0. \lim_{x \to 0^-} \frac{1}{x} = -\infty \ \ \text{and} \ \ \lim_{x \to -\infty} \frac{1}{x} = 0\text{.}

Finally, we write

lim⁡x→∞f(x)=∞ \lim_{x \to \infty} f(x) = \infty

if we can make the value of f(x)f(x) as large as we'd like by taking xx sufficiently large. For example,

lim⁡x→∞x2=∞. \lim_{x \to \infty} x^2 = \infty\text{.}

Limits involving infinity identify vertical and horizontal asymptotes of a function. If lim⁡x→af(x)=∞,\lim_{x \to a} f(x) = \infty\text{,} then x=ax = a is a vertical asymptote of f,f\text{,} while if lim⁡x→∞f(x)=L,\lim_{x \to \infty} f(x) = L\text{,} then y=Ly = L is a horizontal asymptote of f.f\text{.} Similar statements can be made using −∞,-\infty\text{,} and with left- and right-hand limits as x→a−x \to a^- or x→a+.x \to a^+\text{.}

In precalculus classes, it is common to study the end behavior of certain families of functions, by which we mean the behavior of a function as x→∞x \to \infty and as x→−∞.x \to -\infty\text{.} Here we briefly examine some familiar functions and note the values of several limits involving ∞.\infty\text{.}

2_8_InftyLib.svg

Figure 2.8.52.8.5. Graphs of some familiar functions whose end behavior as x→±∞x \to \pm \infty is known. In the middle graph, f(x)=x3−16xf(x) = x^3 - 16x and g(x)=x4−16x2−8.g(x) = x^4 - 16x^2 - 8\text{.}

For the natural exponential function ex,e^x\text{,} we note that lim⁡x→∞ex=∞\lim_{x \to \infty} e^x = \infty and lim⁡x→−∞ex=0.\lim_{x \to -\infty} e^x = 0\text{.} For the exponential decay function e−x,e^{-x}\text{,} these limits are reversed, with lim⁡x→∞e−x=0\lim_{x \to \infty} e^{-x} = 0 and lim⁡x→−∞e−x=∞.\lim_{x \to -\infty} e^{-x} = \infty\text{.} Turning to the natural logarithm function, we have lim⁡x→0+ln⁡(x)=−∞\lim_{x \to 0^+} \ln(x) = -\infty and lim⁡x→∞ln⁡(x)=∞.\lim_{x \to \infty} \ln(x) = \infty\text{.} While both exe^x and ln⁡(x)\ln(x) grow without bound as x→∞,x \to \infty\text{,} the exponential function does so much more quickly than the logarithm function does. We'll soon use limits to quantify what we mean by “quickly.”

For polynomial functions of the form

p(x)=anxn+an−1xn−1+⋯a1x+a0, p(x) = a_n x^n + a_{n-1}x^{n-1} + \cdots a_1 x + a_0\text{,}

the end behavior depends on the sign of ana_n and whether the highest power nn is even or odd. If nn is even and ana_n is positive, then lim⁡x→∞p(x)=∞\lim_{x \to \infty} p(x) = \infty and lim⁡x→−∞p(x)=∞,\lim_{x \to -\infty} p(x) = \infty\text{,} as in the plot of gg in Figure 2.8.52.8.5. If instead ana_n is negative, then lim⁡x→∞p(x)=−∞\lim_{x \to \infty} p(x) = -\infty and lim⁡x→−∞p(x)=−∞.\lim_{x \to -\infty} p(x) = -\infty\text{.} In the situation where nn is odd, then either lim⁡x→∞p(x)=∞\lim_{x \to \infty} p(x) = \infty and lim⁡x→−∞p(x)=−∞\lim_{x \to -\infty} p(x) = -\infty (which occurs when ana_n is positive, as in the graph of ff in Figure 2.8.52.8.5), or lim⁡x→∞p(x)=−∞\lim_{x \to \infty} p(x) = -\infty and lim⁡x→−∞p(x)=∞\lim_{x \to -\infty} p(x) = \infty (when ana_n is negative).

A function can fail to have a limit as x→∞.x \to \infty\text{.} For example, consider the plot of the sine function at right in Figure 2.8.52.8.5. Because the function continues oscillating between −1-1 and 11 as x→∞,x \to \infty\text{,} we say that lim⁡x→∞sin⁡(x)\lim_{x \to \infty} \sin(x) does not exist.

Finally, it is straightforward to analyze the behavior of any rational function as x→∞.x \to \infty\text{.}

Example 2.8.12.8.1

Determine the limit of the function

q(x)=3x2−4x+57x2+9x−10 q(x) = \frac{3x^2 - 4x + 5}{7x^2 + 9x - 10}

as x→∞.x \to \infty\text{.}

Note that both (3x2−4x+5)→∞(3x^2 - 4x + 5) \to \infty as x→∞x \to \infty and (7x2+9x−10)→∞(7x^2 + 9x - 10) \to \infty as x→∞.x \to \infty\text{.} Here we say that lim⁡x→∞q(x)\lim_{x \to \infty} q(x) has indeterminate form ∞∞.\frac{\infty}{\infty}\text{.} We can determine the value of this limit through a standard algebraic approach. Multiplying the numerator and denominator each by 1x2,\frac{1}{x^2}\text{,} we find that

lim⁡x→∞q(x)=(lim⁡x→∞3x2−4x+57x2+9x−10⋅1x21x2=(lim⁡x→∞3−41x+51x27+91x−101x2=37\begin{align*} \lim_{x \to \infty} q(x) =\mathstrut & \lim_{x \to \infty} \frac{3x^2 - 4x + 5}{7x^2 + 9x - 10} \cdot \frac{\frac{1}{x^2}}{\frac{1}{x^2}}\\[4pt] =\mathstrut & \lim_{x \to \infty} \frac{3 - 4\frac{1}{x} + 5\frac{1}{x^2}}{7 + 9\frac{1}{x} - 10\frac{1}{x^2}} = \frac{3}{7} \end{align*}

since 1x2→0\frac{1}{x^2} \to 0 and 1x→0\frac{1}{x} \to 0 as x→∞.x \to \infty\text{.} This shows that the rational function qq has a horizontal asymptote at y=37.y = \frac{3}{7}\text{.} A similar approach can be used to determine the limit of any rational function as x→∞.x \to \infty\text{.}

But how should we handle a limit such as

lim⁡x→∞x2ex? \lim_{x \to \infty} \frac{x^2}{e^x}?

Here, both x2→∞x^2 \to \infty and ex→∞,e^x \to \infty\text{,} but there is not an obvious algebraic approach that enables us to find the limit's value. Fortunately, it turns out that L'Hôpital's Rule extends to cases involving infinity.

L'Hôpital's Rule (∞\infty)

If ff and gg are differentiable and both approach zero or both approach ±∞\pm \infty as x→ax \to a (where aa is allowed to be ∞\infty) , then

lim⁡x→af(x)g(x)=lim⁡x→af′(x)g′(x), \lim_{x \to a} \frac{f(x)}{g(x)} = \lim_{x \to a} \frac{f'(x)}{g'(x)}\text{,}

provided the righthand limit exists.

(To be technically correct, we need to add the additional hypothesis that g′(x)≠0g'(x) \ne 0 on an open interval that contains aa or in every neighborhood of infinity if aa is ∞;\infty\text{;} this is almost always met in practice.)

To evaluate lim⁡x→∞x2ex,\lim_{x \to \infty} \frac{x^2}{e^x}\text{,} we can apply L'Hôpital's Rule, since both x2→∞x^2 \to \infty and ex→∞.e^x \to \infty\text{.} Doing so, it follows that

lim⁡x→∞x2ex=lim⁡x→∞2xex. \lim_{x \to \infty} \frac{x^2}{e^x} = \lim_{x \to \infty} \frac{2x}{e^x}\text{.}

This updated limit is still indeterminate and of the form ∞∞,\frac{\infty}{\infty}\text{,} but it is simpler since 2x2x has replaced x2.x^2\text{.} Hence, we can apply L'Hôpital's Rule again, and find that

lim⁡x→∞x2ex=lim⁡x→∞2xex=lim⁡x→∞2ex. \lim_{x \to \infty} \frac{x^2}{e^x} = \lim_{x \to \infty} \frac{2x}{e^x} = \lim_{x \to \infty} \frac{2}{e^x}\text{.}

Now, since 22 is constant and ex→∞e^x \to \infty as x→∞,x \to \infty\text{,} it follows that 2ex→0\frac{2}{e^x} \to 0 as x→∞,x \to \infty\text{,} which shows that

lim⁡x→∞x2ex=0. \lim_{x \to \infty} \frac{x^2}{e^x} = 0\text{.}
Activity 2.8.32.8.3

Evaluate each of the following limits. If you use L'Hôpital's Rule, indicate where it was used, and be certain its hypotheses are met before you apply it.

  1. lim⁡x→∞xln⁡(x)\displaystyle \lim_{x \to \infty} \frac{x}{\ln(x)}
  2. lim⁡x→∞ex+x2ex+x2\displaystyle \lim_{x \to \infty} \frac{e^{x} + x}{2e^{x} + x^2}
  3. lim⁡x→0+ln⁡(x)1x\displaystyle \lim_{x \to 0^+} \frac{\ln(x)}{\frac{1}{x}}
  4. lim⁡x→π2−tan⁡(x)x−π2\displaystyle \lim_{x \to \frac{\pi}{2}^-} \frac{\tan(x)}{x-\frac{\pi}{2}}
  5. lim⁡x→∞xe−x\displaystyle \lim_{x \to \infty} xe^{-x}

To evaluate the limit of a quotient of two functions f(x)g(x)\frac{f(x)}{g(x)} that results in an indeterminate form of ∞∞,\frac{\infty}{\infty}\text{,} in essence we are asking which function is growing faster without bound. We say that the function gg dominates the function ff as x→∞x \to \infty provided that

lim⁡x→∞f(x)g(x)=0, \lim_{x \to \infty} \frac{f(x)}{g(x)} = 0\text{,}

whereas ff dominates gg provided that lim⁡x→∞f(x)g(x)=∞.\lim_{x \to \infty} \frac{f(x)}{g(x)} = \infty\text{.} Finally, if the value of lim⁡x→∞f(x)g(x)\lim_{x \to \infty} \frac{f(x)}{g(x)} is finite and nonzero, we say that ff and gg grow at the same rate. For example, we saw that lim⁡x→∞x2ex=0,\lim_{x \to \infty} \frac{x^2}{e^x} = 0\text{,} so exe^x dominates x2,x^2\text{,} while lim⁡x→∞3x2−4x+57x2+9x−10=37,\lim_{x \to \infty} \frac{3x^2 - 4x + 5}{7x^2 + 9x - 10} = \frac{3}{7}\text{,} so f(x)=3x2−4x+5f(x) = 3x^2 - 4x + 5 and g(x)=7x2+9x−10g(x) = 7x^2 + 9x - 10 grow at the same rate.

2.82.8 Summary

  • Derivatives can be used to help us evaluate indeterminate limits of the form 00\frac{0}{0} through L'Hôpital's Rule, by replacing the functions in the numerator and denominator with their tangent line approximations. In particular, if f(a)=g(a)=0f(a) = g(a) = 0 and ff and gg are differentiable at a,a\text{,} L'Hôpital's Rule tells us that
    lim⁡x→af(x)g(x)=lim⁡x→af′(x)g′(x). \lim_{x \to a}\frac{f(x)}{g(x)} = \lim_{x \to a}\frac{f'(x)}{g'(x)}\text{.}
  • When we write x→∞,x \to \infty\text{,} this means that xx is increasing without bound. Thus, lim⁡x→∞f(x)=L\lim_{x \to \infty} f(x) = L means that we can make f(x)f(x) as close to LL as we like by choosing xx to be sufficiently large. Similarly, lim⁡x→af(x)=∞,\lim_{x \to a} f(x) = \infty\text{,} means that we can make f(x)f(x) as large as we like by choosing xx sufficiently close to a.a\text{.}
  • A version of L'Hôpital's Rule also helps us evaluate indeterminate limits of the form ∞∞.\frac{\infty}{\infty}\text{.} If ff and gg are differentiable and both approach zero or both approach ±∞\pm \infty as x→ax \to a (where aa is allowed to be ∞\infty), then
    lim⁡x→af(x)g(x)=lim⁡x→af′(x)g′(x). \lim_{x \to a} \frac{f(x)}{g(x)} = \lim_{x \to a} \frac{f'(x)}{g'(x)}\text{.}

Credit and licence

This page titled 2.8: Using Derivatives to Evaluate Limits was last modified on Thu, 28 Sep 2023 16:41:25 GMT and is shared under a CC BY-SA 4.0 license and was authored, remixed, and/or curated by Matthew Boelkins, David Austin, and Steven Schlicker ( ScholarWorks @Grand Valley State University ) via source content that was edited to the style and standards of the LibreTexts platform.

Source: https://math.libretexts.org/Bookshelves/Calculus/Active_Calculus_(Boelkins_et_al.)/02%3A_Computing_Derivatives/2.08%3A_Using_Derivatives_to_Evaluate_Limits

Licence: CC BY-SA 4.0 (creativecommons.org/licenses/by-sa/4.0/). You may share and adapt it under the same licence, with this credit. WorldClass adapted the formatting only: the text is the authors', with interactive parts and links to other sites left out.

Build status · Flash Infinity AI™ is a trademark of AI-Flash Inc.. WorldClass is not affiliated with, approved or accredited by any exam board, curriculum provider or university unless a page says so.