MATH 140 Calculus 1 • McGill University, Montreal

Corrected exercises: infinite limits, limits at infinity and asymptotes (MATH 140)

This is the corrected exercise set for infinite limits, limits at infinity and asymptotes in MATH 140, Calculus 1, at McGill University: the infinite limits of section 2.2 of Stewart and all of section 2.6. It comes before the derivative, so every limit here is settled by algebra, never by L'Hospital's rule, and every number is exact and chosen to be done by hand. Each solution names the step it takes, because a limit given without its sign study or its division earns almost nothing.

The thread running through the whole set: infinity is not a number you substitute. Near a vertical asymptote, “nonzero over zero” becomes an answer only once the sign of the denominator is written on EACH side; at infinity, the dominant term decides, and its sign depends on the direction, since x2=∣x∣\sqrt{x^2} = |x| and the dominant exponential is not the same at both ends. A form ∞−∞\infty - \infty or ∞∞\frac{\infty}{\infty} is a comparison to carry out, never a value.

The traps named in the solutions: writing 60=∞\frac{6}{0} = \infty without a side, declaring an asymptote where the factor cancels, forgetting the minus sign of x2\sqrt{x^2} as x→−∞x \to -\infty, answering 00 to ∞−∞\infty - \infty and 11 to ∞∞\frac{\infty}{\infty}, approximating inside a difference, dividing by exe^x at −∞-\infty, believing a graph never crosses its horizontal asymptote or has only one, taking a sign change for an asymptote, and reading a limit at infinity as a value that is eventually reached.

10 corrected exercises • 100 points • 150 minutes

Revision sheet for this chapter → Every MATH 140 chapter →

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Course recap

  • • lim⁡x→a±N(x)D(x)\lim_{x\to a^\pm} \frac{N(x)}{D(x)} with N→L≠0N \to L \ne 0 and D→0D \to 0: infinite, with the sign of LD\frac{L}{D} on each side. x=ax = a is a vertical asymptote if ONE one-sided limit is infinite.
  • • If N(a)=D(a)=0N(a) = D(a) = 0: factor first; a cancelled factor leaves a hole, not an asymptote.
  • • Rational function at ±∞\pm\infty: divide by the highest power of the denominator. Degree of NN below: 00; equal: ratio of leading coefficients; one more: oblique asymptote by long division.
  • • x2=∣x∣\sqrt{x^2} = |x|: for x<0x < 0, x2+…=−x1+…\sqrt{x^2 + \dots} = -x\sqrt{1 + \dots}. A difference A−B\sqrt A - B of form ∞−∞\infty - \infty: multiply by the conjugate.
  • • ex→0e^x \to 0 at −∞-\infty, ln⁡x→−∞\ln x \to -\infty at 0+0^+, arctan⁡x→±π2\arctan x \to \pm\frac{\pi}{2} at ±∞\pm\infty. Up to two horizontal asymptotes, one per direction.
  • • y=mx+by = mx + b is an asymptote when f(x)−(mx+b)→0f(x) - (mx + b) \to 0; the sign of that gap gives the side of the curve.

Part A: the basics (/50)

Exercise 1: Infinite limits: the sign on each side decides

We write lim⁡x→a+f(x)=∞\lim_{x\to a^+} f(x) = \infty when f(x)f(x) becomes as large as we like for all xx close enough to aa on the right, and similarly with −∞-\infty and with a−a^-. The line x=ax = a is a vertical asymptote of the graph as soon as ONE of the four one-sided limits lim⁡x→a±f(x)\lim_{x\to a^\pm} f(x) is ∞\infty or −∞-\infty.

A quotient whose numerator tends to a nonzero number LL and whose denominator tends to 00 is NOT yet an answer: its size goes to infinity, but its sign is decided by the sign of the denominator on each side of aa, and that sign must be written. The figure shows f(x)=x+3(x+2)(x−1)2f(x) = \frac{x+3}{(x+2)(x-1)^2}.

-6-5-4-3-2-112345-6-4-2246x = -2x = 1y = f(x)
  • a) Read on the figure lim⁡x→−2−f(x)\lim_{x\to -2^-} f(x), lim⁡x→−2+f(x)\lim_{x\to -2^+} f(x), lim⁡x→1f(x)\lim_{x\to 1} f(x) and lim⁡x→±∞f(x)\lim_{x\to \pm\infty} f(x). Then confirm the three limits at −2-2 and at 11 from the formula, by a study of signs.
  • b) Find lim⁡x→3−2xx−3\lim_{x\to 3^-} \frac{2x}{x-3} and lim⁡x→3+2xx−3\lim_{x\to 3^+} \frac{2x}{x-3}. What can you say about lim⁡x→32xx−3\lim_{x\to 3} \frac{2x}{x-3}?
  • c) Find lim⁡x→−1x−5(x+1)2\lim_{x\to -1} \frac{x-5}{(x+1)^2}.
  • d) Let h(x)=x2−4x2−x−2h(x) = \frac{x^2-4}{x^2-x-2}. The denominator vanishes at x=2x = 2 and at x=−1x = -1. For each of these two values, decide whether the graph of hh has a vertical asymptote there, and give the one-sided limits.
  • e) Find lim⁡x→2+ln⁡(x−2)\lim_{x\to 2^+} \ln(x-2), lim⁡x→(π/2)−tan⁡x\lim_{x\to (\pi/2)^-} \tan x, lim⁡x→(π/2)+tan⁡x\lim_{x\to (\pi/2)^+} \tan x, lim⁡x→0−e1/x\lim_{x\to 0^-} e^{1/x} and lim⁡x→0+e1/x\lim_{x\to 0^+} e^{1/x}. Which vertical asymptotes do these limits give?

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  • a) −∞-\infty, +∞+\infty, +∞+\infty (both sides of 11), and 00 at both ends; vertical asymptotes x=−2x = -2 and x=1x = 1.
  • b) −∞-\infty and +∞+\infty; lim⁡x→32xx−3\lim_{x\to 3} \frac{2x}{x-3} does not exist, not even as an infinite limit.
  • c) −∞-\infty
  • d) x=2x = 2: no asymptote, lim⁡x→2h(x)=43\lim_{x\to 2} h(x) = \frac{4}{3} (a hole); x=−1x = -1: asymptote, −∞-\infty on the left and +∞+\infty on the right.
  • e) −∞-\infty; +∞+\infty and −∞-\infty; 00 and +∞+\infty. Asymptotes x=2x = 2 (for ln⁡(x−2)\ln(x-2)), x=π2x = \frac{\pi}{2} (for tan⁡\tan), x=0x = 0 (for e1/xe^{1/x}, from the right only).

a) On the figure, the curve plunges down along x=−2x = -2 on the left and shoots up on the right; along x=1x = 1 it climbs on BOTH sides; and it flattens onto the xx-axis at both ends. So lim⁡x→−2−f(x)=−∞\lim_{x\to -2^-} f(x) = -\infty, lim⁡x→−2+f(x)=+∞\lim_{x\to -2^+} f(x) = +\infty, lim⁡x→1f(x)=+∞\lim_{x\to 1} f(x) = +\infty and lim⁡x→±∞f(x)=0\lim_{x\to\pm\infty} f(x) = 0. From the formula, near x=−2x = -2: the numerator x+3→1>0x + 3 \to 1 > 0 and (x−1)2→9>0(x-1)^2 \to 9 > 0, so the sign is the sign of x+2x + 2, which tends to 00 through negative values on the left (0−0^-) and through positive values on the right (0+0^+). Hence 19⋅0−\frac{1}{9 \cdot 0^-} gives −∞-\infty and 19⋅0+\frac{1}{9 \cdot 0^+} gives +∞+\infty. Near x=1x = 1: x+3→4x + 3 \to 4, x+2→3x + 2 \to 3, and (x−1)2→0+(x-1)^2 \to 0^+ from BOTH sides, because a square is never negative: the limit is +∞+\infty on each side, so lim⁡x→1f(x)=+∞\lim_{x\to 1} f(x) = +\infty. The two lines x=−2x = -2 and x=1x = 1 are vertical asymptotes. The factor to watch is the one that tends to 00, and the power on it decides: odd power, the sign flips across the asymptote; even power, it does not.

b) As x→3x \to 3, the numerator 2x→6>02x \to 6 > 0. For x<3x < 3, x−3<0x - 3 < 0, so the quotient is (positive)/(small negative): lim⁡x→3−2xx−3=−∞\lim_{x\to 3^-} \frac{2x}{x-3} = -\infty. For x>3x > 3, x−3>0x - 3 > 0: lim⁡x→3+2xx−3=+∞\lim_{x\to 3^+} \frac{2x}{x-3} = +\infty. The two one-sided limits are different, so lim⁡x→32xx−3\lim_{x\to 3} \frac{2x}{x-3} does not exist, and we may not even write =∞= \infty: that notation is reserved for a function that goes to +∞+\infty on both sides. Writing 60=∞\frac{6}{0} = \infty and stopping there is the most common way to lose this mark: the sign study IS the answer.

c) The numerator tends to −1−5=−6<0-1 - 5 = -6 < 0. The denominator (x+1)2(x+1)^2 tends to 00 and is positive on both sides of −1-1, so it tends to 0+0^+. Then x−5(x+1)2\frac{x-5}{(x+1)^2} is (about −6-6)/(small positive) on both sides: lim⁡x→−1x−5(x+1)2=−∞\lim_{x\to -1} \frac{x-5}{(x+1)^2} = -\infty. A negative numerator over 0+0^+ gives −∞-\infty: the sign of the NUMERATOR matters as much as that of the denominator, and a student who only looks at the square answers +∞+\infty.

d) Factor before deciding: x2−4=(x−2)(x+2)x^2 - 4 = (x-2)(x+2) and x2−x−2=(x−2)(x+1)x^2 - x - 2 = (x-2)(x+1). For x≠2x \ne 2, h(x)=x+2x+1h(x) = \frac{x+2}{x+1}. At x=2x = 2, both numerator and denominator of the original formula vanish: this is a form 00\frac{0}{0}, not a vertical asymptote. After simplification, lim⁡x→2h(x)=2+22+1=43\lim_{x\to 2} h(x) = \frac{2+2}{2+1} = \frac{4}{3}: the graph has a HOLE at (2,43)\left(2, \frac{4}{3}\right). At x=−1x = -1, the simplified numerator x+2→1≠0x + 2 \to 1 \ne 0 while x+1→0x + 1 \to 0: on the left x+1→0−x + 1 \to 0^- and h(x)→−∞h(x) \to -\infty; on the right x+1→0+x + 1 \to 0^+ and h(x)→+∞h(x) \to +\infty. The line x=−1x = -1 is a vertical asymptote. The rule: a zero of the denominator gives a vertical asymptote only when the numerator does NOT tend to 00 there; when both tend to 00, factor first.

e) As x→2+x \to 2^+, x−2→0+x - 2 \to 0^+ and ln⁡u→−∞\ln u \to -\infty as u→0+u \to 0^+, so lim⁡x→2+ln⁡(x−2)=−∞\lim_{x\to 2^+} \ln(x-2) = -\infty (and the limit from the left makes no sense, ln⁡(x−2)\ln(x-2) is not defined there). Next, tan⁡x=sin⁡xcos⁡x\tan x = \frac{\sin x}{\cos x} with sin⁡x→1\sin x \to 1 as x→π2x \to \frac{\pi}{2}; cos⁡x>0\cos x > 0 just left of π2\frac{\pi}{2} and <0< 0 just right, so tan⁡x→+∞\tan x \to +\infty on the left and −∞-\infty on the right. Finally, as x→0−x \to 0^-, 1x→−∞\frac{1}{x} \to -\infty, and eu→0e^u \to 0 as u→−∞u \to -\infty, so e1/x→0e^{1/x} \to 0; as x→0+x \to 0^+, 1x→+∞\frac{1}{x} \to +\infty and e1/x→+∞e^{1/x} \to +\infty. The vertical asymptotes are x=2x = 2, x=π2x = \frac{\pi}{2} (and every π2+kπ\frac{\pi}{2} + k\pi), and x=0x = 0 for e1/xe^{1/x}, although that last one is infinite from ONE side only. One infinite one-sided limit is enough for an asymptote.

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Exercise 2: Rational functions at infinity: divide by the dominant power

We write lim⁡x→∞f(x)=L\lim_{x\to\infty} f(x) = L when f(x)f(x) is as close to LL as we like for all xx large enough; the line y=Ly = L is then a horizontal asymptote. The basic facts: for r>0r > 0, 1xr→0\frac{1}{x^r} \to 0 as x→∞x \to \infty, and also as x→−∞x \to -\infty when xrx^r is defined.

For a rational function, divide the numerator and the denominator by the highest power of xx in the DENOMINATOR, then let every cxk\frac{c}{x^k} go to 00. The figure shows f(x)=3x2−5x+12x2+7f(x) = \frac{3x^2 - 5x + 1}{2x^2 + 7} and the line y=32y = \frac{3}{2}.

-12-10-8-6-4-224681012-0.50.511.522.5y = 3/2a crossingy = f(x)
  • a) Find lim⁡x→∞f(x)\lim_{x\to\infty} f(x) and lim⁡x→−∞f(x)\lim_{x\to -\infty} f(x). The figure shows the curve crossing the line y=32y = \frac{3}{2}: find exactly where, and say whether this contradicts the asymptote.
  • b) Find lim⁡x→∞4x−1x3+2\lim_{x\to\infty} \frac{4x - 1}{x^3 + 2} and lim⁡x→−∞5x3−x1−2x3\lim_{x\to -\infty} \frac{5x^3 - x}{1 - 2x^3}.
  • c) Find lim⁡x→∞2x3−x5−x2\lim_{x\to\infty} \frac{2x^3 - x}{5 - x^2} and lim⁡x→−∞2x3−x5−x2\lim_{x\to -\infty} \frac{2x^3 - x}{5 - x^2}.
  • d) Find lim⁡x→∞(2x−1)2(x+3)x3−4\lim_{x\to\infty} \frac{(2x-1)^2(x+3)}{x^3 - 4} without expanding the whole numerator.
  • e) Find lim⁡x→∞(x3−100x2)\lim_{x\to\infty} (x^3 - 100x^2) and lim⁡x→−∞(x3−100x2)\lim_{x\to -\infty} (x^3 - 100x^2). One of the two is a form ∞−∞\infty - \infty and the other is not: which?

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  • a) 32\frac{3}{2} at both ends; the curve crosses y=32y = \frac{3}{2} at x=−1910x = -\frac{19}{10}, which is allowed.
  • b) 00 and −52-\frac{5}{2}
  • c) −∞-\infty and +∞+\infty: no horizontal asymptote.
  • d) 44
  • e) +∞+\infty (the form ∞−∞\infty - \infty, settled by factoring x3x^3) and −∞-\infty (not indeterminate: −∞−∞-\infty - \infty).

a) Divide by x2x^2, the highest power of the denominator: f(x)=3−5x+1x22+7x2f(x) = \frac{3 - \frac{5}{x} + \frac{1}{x^2}}{2 + \frac{7}{x^2}}. As x→±∞x \to \pm\infty, every fraction cxk\frac{c}{x^k} tends to 00, so f(x)→32f(x) \to \frac{3}{2} at both ends, and y=32y = \frac{3}{2} is a horizontal asymptote. The crossing: f(x)=32f(x) = \frac{3}{2} means 2(3x2−5x+1)=3(2x2+7)2(3x^2 - 5x + 1) = 3(2x^2 + 7), that is 6x2−10x+2=6x2+216x^2 - 10x + 2 = 6x^2 + 21, so −10x=19-10x = 19 and x=−1910x = -\frac{19}{10}. No contradiction: an asymptote describes what the graph does as x→±∞x \to \pm\infty, and says nothing about finite xx. Here, for x<−1910x < -\frac{19}{10} the curve is above the line and comes down onto it from above as x→−∞x \to -\infty, exactly as the figure shows.

b) First limit: the highest power of the denominator is x3x^3: 4x2−1x31+2x3→0−01+0=0\frac{\frac{4}{x^2} - \frac{1}{x^3}}{1 + \frac{2}{x^3}} \to \frac{0 - 0}{1 + 0} = 0. Degree of the numerator below degree of the denominator always gives 00. Second limit: divide by x3x^3: 5−1x21x3−2→5−2=−52\frac{5 - \frac{1}{x^2}}{\frac{1}{x^3} - 2} \to \frac{5}{-2} = -\frac{5}{2}, and this is the same as x→+∞x \to +\infty: when the degrees are equal, the limit is the ratio of the leading coefficients, sign included. Writing 52\frac{5}{2} because the −2x3-2x^3 was read as 2x32x^3 costs the mark: keep each coefficient with its sign.

c) Divide by x2x^2: 2x3−x5−x2=2x−1x5x2−1\frac{2x^3 - x}{5 - x^2} = \frac{2x - \frac{1}{x}}{\frac{5}{x^2} - 1}. The denominator tends to −1-1 at both ends. As x→+∞x \to +\infty, the numerator 2x−1x→+∞2x - \frac{1}{x} \to +\infty, so the quotient tends to −∞-\infty. As x→−∞x \to -\infty, the numerator tends to −∞-\infty, and dividing by a number close to −1-1 gives +∞+\infty. No horizontal asymptote: the numerator's degree is larger. The shortcut, and the check, is to keep the leading terms: 2x3−x2=−2x\frac{2x^3}{-x^2} = -2x, which tends to −∞-\infty at +∞+\infty and to +∞+\infty at −∞-\infty. Answering ∞\infty for both ends is the classic mistake: the sign changes with the direction because the dominant term −2x-2x is ODD.

d) Only the leading term of each factor matters: (2x−1)2(x+3)=x3(2−1x)2(1+3x)(2x - 1)^2(x + 3) = x^3\left(2 - \frac{1}{x}\right)^2\left(1 + \frac{3}{x}\right) and x3−4=x3(1−4x3)x^3 - 4 = x^3\left(1 - \frac{4}{x^3}\right). Cancel x3x^3: (2−1x)2(1+3x)1−4x3→22⋅11=4\frac{\left(2 - \frac{1}{x}\right)^2\left(1 + \frac{3}{x}\right)}{1 - \frac{4}{x^3}} \to \frac{2^2 \cdot 1}{1} = 4. Factoring xx out of each bracket is quicker and safer than expanding, and it shows at a glance that the numerator has degree 33 with leading coefficient 22⋅1=42^2 \cdot 1 = 4. The trap is to read the leading coefficient of (2x−1)2(2x-1)^2 as 22 instead of 44.

e) As x→+∞x \to +\infty, x3→+∞x^3 \to +\infty and −100x2→−∞-100x^2 \to -\infty: this is the form ∞−∞\infty - \infty, which decides nothing by itself. Factor out the dominant power: x3−100x2=x3(1−100x)x^3 - 100x^2 = x^3\left(1 - \frac{100}{x}\right), a product of a factor tending to +∞+\infty and a factor tending to 11, so the limit is +∞+\infty. The first values are misleading: at x=50x = 50 the polynomial equals 125000−250000<0125000 - 250000 < 0, and it only becomes positive for x>100x > 100. As x→−∞x \to -\infty, x3→−∞x^3 \to -\infty AND −100x2→−∞-100x^2 \to -\infty: two terms going to −∞-\infty add up to −∞-\infty, and there is nothing to decide. A form ∞−∞\infty - \infty appears only when the two terms pull in opposite directions.

Exercise 3: Square roots at infinity: the square root of x squared is |x|

For every real number xx, x2=∣x∣\sqrt{x^2} = |x|, which equals xx when x>0x > 0 and −x-x when x<0x < 0. So when a square root is divided by xx, the step x2+…x=x2+…x2\frac{\sqrt{x^2 + \dots}}{x} = \sqrt{\frac{x^2 + \dots}{x^2}} is correct as x→+∞x \to +\infty and FALSE as x→−∞x \to -\infty, where a minus sign appears.

A difference of two terms that both tend to ∞\infty, one of them a square root, is settled by the conjugate: A−B=A−B2A+B\sqrt A - B = \frac{A - B^2}{\sqrt A + B}. The figure shows f(x)=6x−14x2+1f(x) = \frac{6x - 1}{\sqrt{4x^2 + 1}}.

-8-7-6-5-4-3-2-112345678-4-3-2-11234y = 3y = -3y = f(x)
  • a) Find lim⁡x→∞f(x)\lim_{x\to\infty} f(x).
  • b) Find lim⁡x→−∞f(x)\lim_{x\to -\infty} f(x), and give all the horizontal asymptotes of the graph of ff.
  • c) Find lim⁡x→∞(x2+6x−x)\lim_{x\to\infty} \left(\sqrt{x^2 + 6x} - x\right).
  • d) Find lim⁡x→−∞(x2+6x−x)\lim_{x\to -\infty} \left(\sqrt{x^2 + 6x} - x\right) and lim⁡x→−∞(x2+6x+x)\lim_{x\to -\infty} \left(\sqrt{x^2 + 6x} + x\right).
  • e) A student writes: for large xx, 4x2+x≈4x2=2x\sqrt{4x^2 + x} \approx \sqrt{4x^2} = 2x, so lim⁡x→∞(4x2+x−2x)=0\lim_{x\to\infty} \left(\sqrt{4x^2 + x} - 2x\right) = 0. Find the correct limit and say where the argument fails.

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  • a) 33
  • b) −3-3; two horizontal asymptotes, y=3y = 3 (as x→∞x \to \infty) and y=−3y = -3 (as x→−∞x \to -\infty).
  • c) 33
  • d) +∞+\infty (not indeterminate) and −3-3
  • e) 14\frac{1}{4}: the approximation throws away exactly the term that decides a form ∞−∞\infty - \infty.

a) Divide the numerator and the denominator by xx. For x>0x > 0, x=x2x = \sqrt{x^2}, so 4x2+1x=4x2+1x2=4+1x2\frac{\sqrt{4x^2 + 1}}{x} = \sqrt{\frac{4x^2 + 1}{x^2}} = \sqrt{4 + \frac{1}{x^2}}. Then f(x)=6−1x4+1x2→64=3f(x) = \frac{6 - \frac{1}{x}}{\sqrt{4 + \frac{1}{x^2}}} \to \frac{6}{\sqrt 4} = 3. The limit 4+1x2→2\sqrt{4 + \frac{1}{x^2}} \to 2 uses the continuity of the square root at 44.

b) For x<0x < 0, x2=∣x∣=−x\sqrt{x^2} = |x| = -x, so x=−x2x = -\sqrt{x^2} and 4x2+1x=−4+1x2\frac{\sqrt{4x^2 + 1}}{x} = -\sqrt{4 + \frac{1}{x^2}}. Hence f(x)=6−1x−4+1x2→−62=−3f(x) = \frac{6 - \frac{1}{x}}{-\sqrt{4 + \frac{1}{x^2}}} \to -\frac{6}{2} = -3. The graph has TWO horizontal asymptotes, y=3y = 3 on the right and y=−3y = -3 on the left, which is what the figure shows. Sanity check before any algebra: for xx very negative, the numerator 6x−16x - 1 is negative and the root is positive, so f(x)<0f(x) < 0, and an answer of +3+3 is impossible. Forgetting the minus sign is the trap of this chapter, and it costs the whole limit.

c) This is the form ∞−∞\infty - \infty. Multiply and divide by the conjugate: x2+6x−x=(x2+6x)−x2x2+6x+x=6xx2+6x+x\sqrt{x^2 + 6x} - x = \frac{(x^2 + 6x) - x^2}{\sqrt{x^2 + 6x} + x} = \frac{6x}{\sqrt{x^2 + 6x} + x}. Divide by x>0x > 0: 61+6x+1→61+1=3\frac{6}{\sqrt{1 + \frac{6}{x}} + 1} \to \frac{6}{1 + 1} = 3. Check with x=100x = 100: 10600≈102.96\sqrt{10600} \approx 102.96 (since 1032=10609103^2 = 10609), and 102.96−100≈2.96102.96 - 100 \approx 2.96, close to 33.

d) As x→−∞x \to -\infty, x2+6x→+∞\sqrt{x^2 + 6x} \to +\infty (the function is defined for x≤−6x \le -6) and −x→+∞-x \to +\infty: the sum of two terms going to +∞+\infty goes to +∞+\infty. There is no indeterminate form, and the conjugate would only complicate things. For the second limit, x2+6x→+∞\sqrt{x^2 + 6x} \to +\infty and x→−∞x \to -\infty: now it IS a form ∞−∞\infty - \infty. Conjugate: x2+6x+x=(x2+6x)−x2x2+6x−x=6xx2+6x−x\sqrt{x^2 + 6x} + x = \frac{(x^2 + 6x) - x^2}{\sqrt{x^2 + 6x} - x} = \frac{6x}{\sqrt{x^2 + 6x} - x}. Divide by x<0x < 0, using x2+6xx=−1+6x\frac{\sqrt{x^2 + 6x}}{x} = -\sqrt{1 + \frac{6}{x}}: 6−1+6x−1→6−2=−3\frac{6}{-\sqrt{1 + \frac{6}{x}} - 1} \to \frac{6}{-2} = -3. Always decide first whether the form is indeterminate, then whether xx is positive or negative before bringing it under the root.

e) 4x2+x−2x=(4x2+x)−4x24x2+x+2x=x4x2+x+2x=14+1x+2→12+2=14\sqrt{4x^2 + x} - 2x = \frac{(4x^2 + x) - 4x^2}{\sqrt{4x^2 + x} + 2x} = \frac{x}{\sqrt{4x^2 + x} + 2x} = \frac{1}{\sqrt{4 + \frac{1}{x}} + 2} \to \frac{1}{2 + 2} = \frac{1}{4}. The student's approximation is true as a RATIO, 4x2+x2x→1\frac{\sqrt{4x^2 + x}}{2x} \to 1, but a difference of two huge numbers is decided by what the approximation threw away: here 4x2+x\sqrt{4x^2 + x} exceeds 2x2x by about 14\frac{1}{4}, a gap that does not shrink. Replacing a term by an equivalent one is legitimate in a product or a quotient, never in a difference.

Exercise 4: Exponentials, logarithms and arctangent at the ends of the axis

Four facts carry this exercise, all read on the graphs of the functions: ex→∞e^x \to \infty as x→∞x \to \infty and ex→0e^x \to 0 as x→−∞x \to -\infty (so e−xe^{-x} does the opposite); ln⁡x→∞\ln x \to \infty as x→∞x \to \infty and ln⁡x→−∞\ln x \to -\infty as x→0+x \to 0^+; arctan⁡x→π2\arctan x \to \frac{\pi}{2} as x→∞x \to \infty and arctan⁡x→−π2\arctan x \to -\frac{\pi}{2} as x→−∞x \to -\infty. For a composition, find the limit of the inside first, then apply the outside function to where the inside goes.

The figure shows g(x)=2ex+3ex−1g(x) = \frac{2e^x + 3}{e^x - 1}, defined for x≠0x \ne 0.

-5-4-3-2-11234-8-6-4-22468y = 2y = -3y = g(x)
  • a) Find lim⁡x→∞g(x)\lim_{x\to\infty} g(x) and lim⁡x→−∞g(x)\lim_{x\to -\infty} g(x).
  • b) Find lim⁡x→0−g(x)\lim_{x\to 0^-} g(x) and lim⁡x→0+g(x)\lim_{x\to 0^+} g(x). List all the asymptotes of the graph of gg.
  • c) Find lim⁡x→∞arctan⁡(x2−x)\lim_{x\to\infty} \arctan(x^2 - x), lim⁡x→−∞arctan⁡(x3+x)\lim_{x\to -\infty} \arctan(x^3 + x), and the two one-sided limits of arctan⁡(1x)\arctan\left(\frac{1}{x}\right) at 00. Is x=0x = 0 a vertical asymptote of arctan⁡(1x)\arctan\left(\frac{1}{x}\right)?
  • d) Find lim⁡x→∞[ln⁡(2x+1)−ln⁡(x+3)]\lim_{x\to\infty} \left[\ln(2x + 1) - \ln(x + 3)\right] and lim⁡x→(−1/2)+ln⁡(2x+1)\lim_{x\to (-1/2)^+} \ln(2x + 1).
  • e) Find lim⁡x→∞e3x−e−xe3x+ex\lim_{x\to\infty} \frac{e^{3x} - e^{-x}}{e^{3x} + e^x} and lim⁡x→−∞e3x−e−xe3x+ex\lim_{x\to -\infty} \frac{e^{3x} - e^{-x}}{e^{3x} + e^x}.

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  • a) 22 and −3-3
  • b) −∞-\infty and +∞+\infty; asymptotes y=2y = 2 (right), y=−3y = -3 (left) and x=0x = 0.
  • c) π2\frac{\pi}{2}, −π2-\frac{\pi}{2}; −π2-\frac{\pi}{2} from the left and π2\frac{\pi}{2} from the right; no vertical asymptote (a jump, the function stays bounded).
  • d) ln⁡2\ln 2 and −∞-\infty
  • e) 11 and −∞-\infty

a) As x→∞x \to \infty, exe^x dominates: divide by it. g(x)=2+3e−x1−e−x→2+01−0=2g(x) = \frac{2 + 3e^{-x}}{1 - e^{-x}} \to \frac{2 + 0}{1 - 0} = 2. As x→−∞x \to -\infty, ex→0e^x \to 0 and nothing needs dividing: g(x)→0+30−1=−3g(x) \to \frac{0 + 3}{0 - 1} = -3. Two different horizontal asymptotes, y=2y = 2 on the right and y=−3y = -3 on the left, as on the figure. Dividing by exe^x at −∞-\infty would be dividing by a number that tends to 00: the dominant term is not the same at both ends, and exe^x only dominates as x→+∞x \to +\infty.

b) As x→0x \to 0, the numerator tends to 2+3=5>02 + 3 = 5 > 0 and the denominator ex−1e^x - 1 tends to 00. Its sign: ex>1e^x > 1 for x>0x > 0 and ex<1e^x < 1 for x<0x < 0, so ex−1→0+e^x - 1 \to 0^+ on the right and 0−0^- on the left. Hence lim⁡x→0−g(x)=−∞\lim_{x\to 0^-} g(x) = -\infty and lim⁡x→0+g(x)=+∞\lim_{x\to 0^+} g(x) = +\infty. The asymptotes: y=2y = 2 as x→∞x \to \infty, y=−3y = -3 as x→−∞x \to -\infty, and x=0x = 0, the yy-axis itself. The sign of ex−1e^x - 1 comes from the fact that exe^x is increasing with e0=1e^0 = 1: say it, it is the whole justification.

c) x2−x=x(x−1)→∞x^2 - x = x(x - 1) \to \infty as x→∞x \to \infty (product of two factors tending to ∞\infty), and arctan⁡u→π2\arctan u \to \frac{\pi}{2} as u→∞u \to \infty, so the first limit is π2\frac{\pi}{2}. x3+x=x(x2+1)→−∞x^3 + x = x(x^2 + 1) \to -\infty as x→−∞x \to -\infty, so the second is −π2-\frac{\pi}{2}. As x→0−x \to 0^-, 1x→−∞\frac{1}{x} \to -\infty and arctan⁡(1x)→−π2\arctan\left(\frac{1}{x}\right) \to -\frac{\pi}{2}; as x→0+x \to 0^+, 1x→+∞\frac{1}{x} \to +\infty and arctan⁡(1x)→π2\arctan\left(\frac{1}{x}\right) \to \frac{\pi}{2}. The one-sided limits are finite and different: a jump of height π\pi, and NOT a vertical asymptote, since ∣arctan⁡(1x)∣<π2\left|\arctan\left(\frac{1}{x}\right)\right| < \frac{\pi}{2} for all x≠0x \ne 0. A denominator that tends to 00 inside a bounded function produces no asymptote.

d) Each logarithm tends to ∞\infty: the form is ∞−∞\infty - \infty. Combine by the law of logarithms, valid since 2x+1>02x + 1 > 0 and x+3>0x + 3 > 0 for large xx: ln⁡(2x+1)−ln⁡(x+3)=ln⁡(2x+1x+3)\ln(2x + 1) - \ln(x + 3) = \ln\left(\frac{2x + 1}{x + 3}\right). The inside tends to 22 (ratio of the leading coefficients), and ln⁡\ln is continuous at 22, so the limit is ln⁡2\ln 2. Answering 00 because both logarithms grow alike is the trap. As x→(−12)+x \to \left(-\frac{1}{2}\right)^+, 2x+1→0+2x + 1 \to 0^+ and ln⁡u→−∞\ln u \to -\infty as u→0+u \to 0^+: the limit is −∞-\infty, and x=−12x = -\frac{1}{2} is a vertical asymptote of ln⁡(2x+1)\ln(2x + 1).

e) As x→∞x \to \infty, the dominant exponential is e3xe^{3x}: 1−e−4x1+e−2x→1−01+0=1\frac{1 - e^{-4x}}{1 + e^{-2x}} \to \frac{1 - 0}{1 + 0} = 1. As x→−∞x \to -\infty the ranking reverses: e−x→∞e^{-x} \to \infty while e3xe^{3x} and exe^x tend to 00, and in the denominator exe^x is the larger of the two (since e3x=ex⋅e2xe^{3x} = e^x \cdot e^{2x} with e2x→0e^{2x} \to 0). Divide by exe^x: e2x−e−2xe2x+1\frac{e^{2x} - e^{-2x}}{e^{2x} + 1}. The numerator tends to 0−∞=−∞0 - \infty = -\infty and the denominator to 11, so the limit is −∞-\infty. The largest exponent wins at +∞+\infty, the most negative one wins at −∞-\infty: always rank the exponentials again when the direction changes.

Exercise 5: Oblique asymptotes: long division, and the sign of what is left

The line y=mx+by = mx + b with m≠0m \ne 0 is an oblique (slant) asymptote when lim⁡x→∞[f(x)−(mx+b)]=0\lim_{x\to\infty} \left[f(x) - (mx + b)\right] = 0, or the same as x→−∞x \to -\infty. For a rational function whose numerator has degree exactly ONE more than the denominator, long division gives f(x)=mx+b+R(x)D(x)f(x) = mx + b + \frac{R(x)}{D(x)} with a remainder of lower degree than DD, so the fraction tends to 00 at both ends.

The sign of R(x)D(x)\frac{R(x)}{D(x)} says on which side of the asymptote the curve lies. The figure shows f(x)=x2+x+2x−1f(x) = \frac{x^2 + x + 2}{x - 1} and the dashed line y=x+2y = x + 2.

-6-5-4-3-2-112345678-8-6-4-2246810121416x = 1dashed: y = x + 2y = f(x)
  • a) Divide x2+x+2x^2 + x + 2 by x−1x - 1, and deduce the oblique asymptote of ff. Find also its vertical asymptote with the two one-sided limits.
  • b) Study the sign of f(x)−(x+2)f(x) - (x + 2). On which side of the asymptote is the curve, for x>1x > 1 and for x<1x < 1? Compare with the figure.
  • c) Let g(x)=x3−1x2+1g(x) = \frac{x^3 - 1}{x^2 + 1}. Find its oblique asymptote, and show that the graph of gg crosses it. Where?
  • d) Without dividing completely, say which of x3+2x−1\frac{x^3 + 2}{x - 1} and 3x2+1x2−4\frac{3x^2 + 1}{x^2 - 4} has an oblique asymptote, and describe the end behaviour of each.
  • e) Let k(x)=x2+4xk(x) = \sqrt{x^2 + 4x}. Show that y=x+2y = x + 2 is an oblique asymptote as x→∞x \to \infty and that y=−x−2y = -x - 2 is one as x→−∞x \to -\infty.

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  • a) f(x)=x+2+4x−1f(x) = x + 2 + \frac{4}{x-1}; oblique asymptote y=x+2y = x + 2; vertical asymptote x=1x = 1, with −∞-\infty on the left and +∞+\infty on the right.
  • b) f(x)−(x+2)=4x−1f(x) - (x+2) = \frac{4}{x-1}: above the line for x>1x > 1, below for x<1x < 1.
  • c) g(x)=x−x+1x2+1g(x) = x - \frac{x+1}{x^2+1}: asymptote y=xy = x, crossed at x=−1x = -1, at the point (−1,−1)(-1, -1).
  • d) x3+2x−1\frac{x^3+2}{x-1}: no oblique asymptote, it behaves like x2x^2 (+∞+\infty at both ends); 3x2+1x2−4\frac{3x^2+1}{x^2-4}: horizontal asymptote y=3y = 3, no oblique one.
  • e) k(x)−(x+2)=−4x2+4x+x+2→0k(x) - (x+2) = \frac{-4}{\sqrt{x^2+4x} + x + 2} \to 0 at ∞\infty; k(x)−(−x−2)=−4x2+4x−x−2→0k(x) - (-x-2) = \frac{-4}{\sqrt{x^2+4x} - x - 2} \to 0 at −∞-\infty.

a) Long division: x2÷x=xx^2 \div x = x, and x2+x+2−x(x−1)=2x+2x^2 + x + 2 - x(x - 1) = 2x + 2; then 2x÷x=22x \div x = 2, and 2x+2−2(x−1)=42x + 2 - 2(x - 1) = 4. So x2+x+2=(x−1)(x+2)+4x^2 + x + 2 = (x - 1)(x + 2) + 4 and f(x)=x+2+4x−1f(x) = x + 2 + \frac{4}{x - 1}. Check at x=3x = 3: f(3)=142=7f(3) = \frac{14}{2} = 7 and 3+2+42=73 + 2 + \frac{4}{2} = 7. As x→±∞x \to \pm\infty, 4x−1→0\frac{4}{x - 1} \to 0, so f(x)−(x+2)→0f(x) - (x + 2) \to 0 and y=x+2y = x + 2 is an oblique asymptote at both ends. At x=1x = 1 the numerator is 4≠04 \ne 0: with x−1→0−x - 1 \to 0^- on the left, f(x)→−∞f(x) \to -\infty; with 0+0^+ on the right, f(x)→+∞f(x) \to +\infty. The vertical asymptote is x=1x = 1. The quotient of the division is the asymptote; the remainder is only what tends to 00.

b) f(x)−(x+2)=4x−1f(x) - (x + 2) = \frac{4}{x - 1}, positive for x>1x > 1 and negative for x<1x < 1. So the curve lies ABOVE its asymptote on the right branch and BELOW on the left branch, and it approaches the line from above as x→∞x \to \infty and from below as x→−∞x \to -\infty. The figure agrees: the right branch comes down onto the dashed line from above, the left branch climbs to it from underneath. This sign study is the part examiners reward, because it is what makes a sketch correct near the asymptote.

c) Divide x3−1x^3 - 1 by x2+1x^2 + 1: x3÷x2=xx^3 \div x^2 = x, and x3−1−x(x2+1)=−x−1x^3 - 1 - x(x^2 + 1) = -x - 1. So g(x)=x−x+1x2+1g(x) = x - \frac{x + 1}{x^2 + 1}, and since x+1x2+1→0\frac{x + 1}{x^2 + 1} \to 0 at both ends (degree 11 over degree 22), the line y=xy = x is an oblique asymptote. The gap g(x)−x=−x+1x2+1g(x) - x = -\frac{x + 1}{x^2 + 1} vanishes when x=−1x = -1: g(−1)=−22=−1g(-1) = \frac{-2}{2} = -1, a point of the line y=xy = x. The curve crosses its asymptote at (−1,−1)(-1, -1): below the line for x>−1x > -1, above it for x<−1x < -1. Like a horizontal asymptote, an oblique one only describes the ends of the graph.

d) x3+2x−1\frac{x^3 + 2}{x - 1}: the degree difference is 22, so the quotient of the division has degree 22: x3+2=(x−1)(x2+x+1)+3x^3 + 2 = (x - 1)(x^2 + x + 1) + 3, and the function behaves like the parabola x2+x+1x^2 + x + 1, tending to +∞+\infty at both ends. No line approaches it, so no oblique asymptote. 3x2+1x2−4\frac{3x^2 + 1}{x^2 - 4}: equal degrees, so it tends to 31=3\frac{3}{1} = 3 at both ends, a horizontal asymptote y=3y = 3, and a function cannot have both a horizontal and an oblique asymptote in the same direction. The rule to remember: oblique asymptote for a rational function exactly when the degree of the numerator is ONE more than that of the denominator.

e) kk is defined for x2+4x≥0x^2 + 4x \ge 0, that is x≤−4x \le -4 or x≥0x \ge 0. As x→∞x \to \infty: k(x)−(x+2)=(x2+4x)−(x+2)2x2+4x+x+2=−4x2+4x+x+2k(x) - (x + 2) = \frac{(x^2 + 4x) - (x + 2)^2}{\sqrt{x^2 + 4x} + x + 2} = \frac{-4}{\sqrt{x^2 + 4x} + x + 2}, whose denominator tends to ∞\infty, so the gap tends to 00: y=x+2y = x + 2 is an oblique asymptote. As x→−∞x \to -\infty: k(x)−(−x−2)=x2+4x+(x+2)=(x2+4x)−(x+2)2x2+4x−(x+2)=−4x2+4x−x−2k(x) - (-x - 2) = \sqrt{x^2 + 4x} + (x + 2) = \frac{(x^2 + 4x) - (x + 2)^2}{\sqrt{x^2 + 4x} - (x + 2)} = \frac{-4}{\sqrt{x^2 + 4x} - x - 2}; now x2+4x→∞\sqrt{x^2 + 4x} \to \infty AND −x−2→∞-x - 2 \to \infty, so the denominator tends to ∞\infty and the gap to 00. The slope is +1+1 on the right and −1-1 on the left, because x2=∣x∣\sqrt{x^2} = |x|: the graph of kk opens like a V, not like a line.

Part B: problems and reasoning (/50)

Exercise 6: Asymptotes as constraints: finding the parameters

An exam favourite turns the chapter around: the asymptotes are given, the formula has unknown constants, and each asymptote becomes an equation. The trap is always the same: a zero of the denominator gives a vertical asymptote only if the numerator does NOT vanish there too, so every candidate must be checked in the numerator before it is accepted.

No figure here: every answer must come from the formula, as on the final.

  • a) Find the constants aa and bb so that the graph of f(x)=ax+5bx−6f(x) = \frac{ax + 5}{bx - 6} has the vertical asymptote x=3x = 3 and the horizontal asymptote y=2y = 2. Check that x=3x = 3 really is an asymptote.
  • b) Let g(x)=x2+px+qx−1g(x) = \frac{x^2 + px + q}{x - 1}. Find pp so that y=x+4y = x + 4 is an oblique asymptote. For which value of qq does the graph of gg have NO vertical asymptote, and what does it look like then?
  • c) Find the constant kk such that lim⁡x→∞(x2+kx−x)=5\lim_{x\to\infty} \left(\sqrt{x^2 + kx} - x\right) = 5.
  • d) Find aa and bb so that h(x)=ax2+3x2+bx+4h(x) = \frac{ax^2 + 3}{x^2 + bx + 4} has exactly one vertical asymptote, the line x=2x = 2, and the horizontal asymptote y=−1y = -1. Then give the behaviour of hh on each side of x=2x = 2.

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  • a) b=2b = 2, a=4a = 4: f(x)=4x+52x−6f(x) = \frac{4x+5}{2x-6}, numerator 17≠017 \ne 0 at x=3x = 3.
  • b) p=3p = 3; no vertical asymptote exactly when q=−4q = -4: then g(x)=x+4g(x) = x + 4 for x≠1x \ne 1, a line with a hole at (1,5)(1, 5).
  • c) k=10k = 10
  • d) a=−1a = -1, b=−4b = -4: h(x)=3−x2(x−2)2h(x) = \frac{3 - x^2}{(x-2)^2}, which tends to −∞-\infty on both sides of 22.

a) As x→±∞x \to \pm\infty, f(x)→abf(x) \to \frac{a}{b} (divide by xx), provided b≠0b \ne 0; so ab=2\frac{a}{b} = 2. A vertical asymptote at x=3x = 3 needs the denominator to vanish there: 3b−6=03b - 6 = 0, so b=2b = 2, then a=4a = 4. The check the question asks for: at x=3x = 3 the numerator is 4⋅3+5=17≠04 \cdot 3 + 5 = 17 \ne 0, so f(x)=4x+52x−6f(x) = \frac{4x + 5}{2x - 6} is (about 1717)/(something tending to 00) and tends to ±∞\pm\infty: lim⁡x→3−f(x)=−∞\lim_{x\to 3^-} f(x) = -\infty and lim⁡x→3+f(x)=+∞\lim_{x\to 3^+} f(x) = +\infty. Without that check, the answer is incomplete: had the numerator vanished at 33, the graph would have had a hole instead.

b) Divide: x2+px+q=(x−1)(x+p+1)+(1+p+q)x^2 + px + q = (x - 1)(x + p + 1) + (1 + p + q), which can be checked by expanding: (x−1)(x+p+1)=x2+px−p−1(x - 1)(x + p + 1) = x^2 + px - p - 1. So g(x)=x+p+1+1+p+qx−1g(x) = x + p + 1 + \frac{1 + p + q}{x - 1}, and the oblique asymptote is y=x+p+1y = x + p + 1. It equals y=x+4y = x + 4 exactly when p=3p = 3. Then g(x)=x+4+4+qx−1g(x) = x + 4 + \frac{4 + q}{x - 1}. If q≠−4q \ne -4, the numerator 1+3+q=4+q1 + 3 + q = 4 + q does not vanish at x=1x = 1, and x=1x = 1 is a vertical asymptote. If q=−4q = -4, the remainder is 00: x2+3x−4=(x−1)(x+4)x^2 + 3x - 4 = (x - 1)(x + 4), so g(x)=x+4g(x) = x + 4 for every x≠1x \ne 1. The graph is the line y=x+4y = x + 4 with a hole at (1,5)(1, 5), and there is no vertical asymptote. The value of qq that kills the asymptote is the one that makes the numerator vanish at 11: 1+3+q=01 + 3 + q = 0.

c) Conjugate, as in Exercise 3: x2+kx−x=kxx2+kx+x=k1+kx+1\sqrt{x^2 + kx} - x = \frac{kx}{\sqrt{x^2 + kx} + x} = \frac{k}{\sqrt{1 + \frac{k}{x}} + 1} for x>0x > 0, which tends to k2\frac{k}{2}. So the limit equals 55 exactly when k=10k = 10. Check: with k=10k = 10 and x=1000x = 1000, 1010000≈1004.99\sqrt{1010000} \approx 1004.99, since 10052=10100251005^2 = 1010025; the difference is about 4.994.99. The graph of x2+10x\sqrt{x^2 + 10x} therefore has the oblique asymptote y=x+5y = x + 5 as x→∞x \to \infty: a limit with a parameter is often an asymptote in disguise.

d) Horizontal asymptote: the degrees are equal, so h(x)→a1=ah(x) \to \frac{a}{1} = a at both ends, and a=−1a = -1. Vertical asymptote: the denominator must vanish at 22, so 4+2b+4=04 + 2b + 4 = 0 and b=−4b = -4; then x2−4x+4=(x−2)2x^2 - 4x + 4 = (x - 2)^2, whose only zero is 22. There is no other choice of bb: a quadratic x2+bx+4x^2 + bx + 4 with the root 22 has the product of its roots equal to 44, so its other root is 22 as well. Check the numerator at 22: −4+3=−1≠0-4 + 3 = -1 \ne 0, so x=2x = 2 really is a vertical asymptote, and it is the only one. On both sides, (x−2)2→0+(x - 2)^2 \to 0^+ and the numerator tends to −1-1: h(x)→−∞h(x) \to -\infty on the left AND on the right. The double root is what makes both branches go down.

Exercise 7: From a sign chart to the behaviour at every asymptote

Let f(x)=(x+1)(x−3)(x−1)2(x+2)f(x) = \frac{(x+1)(x-3)}{(x-1)^2(x+2)}. The figure is its sign chart: one row per factor, the sign of ff on the last row, a 00 where a factor vanishes and a double bar where ff is not defined.

The sign chart is the tool of this exercise: the size of ff near an asymptote comes from the factor that tends to 00, and its SIGN comes from the chart. No derivative is needed, and none is allowed: the question is only how the graph behaves at its asymptotes and where it meets the axes.

x-2-113x + 2−++++0x + 1−−+++0x − 3−−−−+0(x − 1)²+++++0f(x)−+−−+00
  • a) Explain why the row of (x−1)2(x-1)^2 has no minus sign, why the last row has a double bar at −2-2 and at 11, and check the sign of ff on the interval (1,3)(1, 3) from the factor rows.
  • b) Give the four one-sided limits of ff at −2-2 and at 11.
  • c) Find lim⁡x→∞f(x)\lim_{x\to\infty} f(x) and lim⁡x→−∞f(x)\lim_{x\to -\infty} f(x), and say from which side the graph approaches its horizontal asymptote at each end.
  • d) Find the intercepts with the axes, then sketch the graph near its three asymptotes, using only these intercepts and the results of b) and c).
  • e) A student writes: “ff has a vertical asymptote at x=1x = 1 because ff changes sign there, and none at x=3x = 3 because it only changes sign.” Correct the reasoning.

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  • a) A square is never negative; at −2-2 and 11 the denominator vanishes; on (1,3)(1, 3): (+)(−)(+)(+)<0\frac{(+)(-)}{(+)(+)} < 0.
  • b) lim⁡x→−2−f=−∞\lim_{x\to -2^-} f = -\infty, lim⁡x→−2+f=+∞\lim_{x\to -2^+} f = +\infty, lim⁡x→1±f=−∞\lim_{x\to 1^\pm} f = -\infty.
  • c) 00 at both ends: from above (f>0f > 0) as x→∞x \to \infty, from below (f<0f < 0) as x→−∞x \to -\infty.
  • d) xx-intercepts −1-1 and 33, yy-intercept −32-\frac{3}{2}; sketch in the solution figure.
  • e) ff does NOT change sign at 11 and is −∞-\infty on both sides; the asymptote comes from the denominator tending to 00, not from a sign change. At 33 the sign changes because f(3)=0f(3) = 0.

a) (x−1)2(x-1)^2 is a square, so it is positive for x≠1x \ne 1 and zero at 11: its row reads ++ everywhere, with a 00 at 11. The last row carries a double bar where ff is not defined, that is where the DENOMINATOR (x−1)2(x+2)(x-1)^2(x+2) vanishes: x=−2x = -2 and x=1x = 1. The zeros of ff are those of the numerator, −1-1 and 33. On (1,3)(1, 3): x+2>0x + 2 > 0, x+1>0x + 1 > 0, x−3<0x - 3 < 0 and (x−1)2>0(x-1)^2 > 0, so f(x)=(+)(−)(+)(+)<0f(x) = \frac{(+)(-)}{(+)(+)} < 0, as the chart says. Reading a chart is one step; being able to rebuild any cell from the factors is what the examiner checks.

b) At x=−2x = -2 the numerator tends to (−1)(−5)=5≠0(-1)(-5) = 5 \ne 0 and the denominator to 00, so ∣f(x)∣→∞|f(x)| \to \infty; the chart gives the sign: f<0f < 0 just left of −2-2 and f>0f > 0 just right. Hence lim⁡x→−2−f(x)=−∞\lim_{x\to -2^-} f(x) = -\infty and lim⁡x→−2+f(x)=+∞\lim_{x\to -2^+} f(x) = +\infty. At x=1x = 1 the numerator tends to (2)(−2)=−4≠0(2)(-2) = -4 \ne 0 and the denominator to 00, and f<0f < 0 on both sides: lim⁡x→1−f(x)=lim⁡x→1+f(x)=−∞\lim_{x\to 1^-} f(x) = \lim_{x\to 1^+} f(x) = -\infty, so lim⁡x→1f(x)=−∞\lim_{x\to 1} f(x) = -\infty. The two lines x=−2x = -2 and x=1x = 1 are vertical asymptotes. The chart replaces four separate studies of 0+0^+ and 0−0^- with one table, and the square factor explains why 11 behaves differently from −2-2.

c) The numerator has degree 22 and the denominator degree 33: dividing by x3x^3, f(x)=(1x+1x2)(1−3x)(1−1x)2(1+2x)→0⋅11⋅1=0f(x) = \frac{\left(\frac{1}{x} + \frac{1}{x^2}\right)\left(1 - \frac{3}{x}\right)}{\left(1 - \frac{1}{x}\right)^2\left(1 + \frac{2}{x}\right)} \to \frac{0 \cdot 1}{1 \cdot 1} = 0 at both ends, so y=0y = 0 is the horizontal asymptote. From which side: the last column of the chart says f>0f > 0 for x>3x > 3, so the graph comes down onto the axis from above as x→∞x \to \infty; the first column says f<0f < 0 for x<−2x < -2, so it rises to the axis from below as x→−∞x \to -\infty. The leading terms confirm it: f(x)f(x) behaves like x2x3=1x\frac{x^2}{x^3} = \frac{1}{x}, positive on the right and negative on the left.

d) The xx-intercepts are the zeros of the numerator that are in the domain, x=−1x = -1 and x=3x = 3; the yy-intercept is f(0)=(1)(−3)(1)(2)=−32f(0) = \frac{(1)(-3)}{(1)(2)} = -\frac{3}{2}. The sketch: on (−∞,−2)(-\infty, -2), the curve leaves the xx-axis from below and plunges to −∞-\infty along x=−2x = -2; on (−2,1)(-2, 1) it comes down from +∞+\infty, crosses the axis at −1-1, passes through (0,−32)\left(0, -\frac{3}{2}\right) and falls to −∞-\infty along x=1x = 1; on (1,∞)(1, \infty) it rises from −∞-\infty, crosses the axis at 33 and settles on the axis from above. The solution figure shows exactly these pieces, and nothing more is asked: where the curve turns belongs to the chapter on curve sketching.

e) Both halves of the claim are wrong. At x=1x = 1, ff does NOT change sign: it is negative on both sides, and it still has a vertical asymptote, because the denominator tends to 00 while the numerator tends to −4≠0-4 \ne 0. At x=3x = 3, ff changes sign because the numerator vanishes, f(3)=0f(3) = 0: a sign change through a zero of ff is an intercept, not an asymptote. A sign change can happen at a zero or at an asymptote, and an asymptote can happen with or without a sign change: the only question to ask is whether the denominator tends to 00 while the numerator does not.

-6-5-4-3-2-1123456-6-4-2246x = -2x = 1y = 0 from abovey = 0 from below

Exercise 8: Five statements to correct

Each statement below was written by a student on a MATH 140 assignment, and each is false. Say what is wrong, give a counterexample, and write the correct statement.

  • a) If the denominator of a rational function ff is zero at x=ax = a, then x=ax = a is a vertical asymptote of the graph of ff.
  • b) The graph of a function can never cross its horizontal asymptote.
  • c) A function has at most one horizontal asymptote.
  • d) ∞−∞=0\infty - \infty = 0 and ∞∞=1\frac{\infty}{\infty} = 1.
  • e) lim⁡x→01x3=∞\lim_{x\to 0} \frac{1}{x^3} = \infty, so this limit exists.

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  • a) False: x2−4x−2→4\frac{x^2 - 4}{x - 2} \to 4 at 22 (a hole). True if the numerator does not tend to 00 at aa.
  • b) False: sin⁡xx→0\frac{\sin x}{x} \to 0 and equals 00 at every x=kπx = k\pi.
  • c) False: arctan⁡x\arctan x has y=π2y = \frac{\pi}{2} and y=−π2y = -\frac{\pi}{2}. At most TWO, one per direction.
  • d) False: (x+1)−x→1(x + 1) - x \to 1, x2−x→∞x^2 - x \to \infty; 2xx→2\frac{2x}{x} \to 2. These are indeterminate forms.
  • e) False twice: −∞-\infty from the left, +∞+\infty from the right; and an infinite limit is a limit that does not exist.

a) FALSE. f(x)=x2−4x−2f(x) = \frac{x^2 - 4}{x - 2} has a denominator that vanishes at 22, but f(x)=x+2f(x) = x + 2 for x≠2x \ne 2, so lim⁡x→2f(x)=4\lim_{x\to 2} f(x) = 4: the graph is a line with a hole at (2,4)(2, 4), and nothing goes to infinity. Correct statement: if the denominator tends to 00 at aa while the numerator tends to a NONZERO number, then x=ax = a is a vertical asymptote. When both tend to 00, the form is 00\frac{0}{0}: factor and simplify before deciding.

b) FALSE. For x>0x > 0, ∣sin⁡xx∣≤1x\left|\frac{\sin x}{x}\right| \le \frac{1}{x}, which tends to 00, so sin⁡xx→0\frac{\sin x}{x} \to 0 as x→∞x \to \infty and y=0y = 0 is a horizontal asymptote; yet sin⁡xx=0\frac{\sin x}{x} = 0 at x=π,2π,3π,…x = \pi, 2\pi, 3\pi, \dots, so the graph crosses its asymptote infinitely often. A rational example: 3x2−5x+12x2+7\frac{3x^2 - 5x + 1}{2x^2 + 7} crosses y=32y = \frac{3}{2} at x=−1910x = -\frac{19}{10} (Exercise 2). Correct statement: a horizontal asymptote describes the graph as x→∞x \to \infty or x→−∞x \to -\infty only; it can be crossed any number of times at finite xx.

c) FALSE. arctan⁡x→π2\arctan x \to \frac{\pi}{2} as x→∞x \to \infty and arctan⁡x→−π2\arctan x \to -\frac{\pi}{2} as x→−∞x \to -\infty: two horizontal asymptotes. So does 6x−14x2+1\frac{6x - 1}{\sqrt{4x^2 + 1}}, with y=3y = 3 and y=−3y = -3 (Exercise 3), and 2ex+3ex−1\frac{2e^x + 3}{e^x - 1}, with y=2y = 2 and y=−3y = -3 (Exercise 4). Correct statement: a function has at most TWO horizontal asymptotes, one as x→∞x \to \infty and one as x→−∞x \to -\infty, and the two limits must be computed separately. For a rational function they coincide, which is where the false belief comes from.

d) FALSE. ∞\infty is not a number, and these are forms, not values. (x+1)−x=1→1(x + 1) - x = 1 \to 1, while x2−x→∞x^2 - x \to \infty and x−x2→−∞x - x^2 \to -\infty: three limits of the form ∞−∞\infty - \infty, three different answers. Likewise 2xx→2\frac{2x}{x} \to 2, x2x→∞\frac{x^2}{x} \to \infty and xx2→0\frac{x}{x^2} \to 0 are all of the form ∞∞\frac{\infty}{\infty}. Correct statement: ∞−∞\infty - \infty and ∞∞\frac{\infty}{\infty} are indeterminate forms; transform the expression (factor the dominant term, divide by it, or use a conjugate) before taking the limit.

e) FALSE, twice. First, x3x^3 has the sign of xx: lim⁡x→0−1x3=−∞\lim_{x\to 0^-} \frac{1}{x^3} = -\infty and lim⁡x→0+1x3=+∞\lim_{x\to 0^+} \frac{1}{x^3} = +\infty, so lim⁡x→01x3\lim_{x\to 0} \frac{1}{x^3} is not even infinite; only 1x2\frac{1}{x^2} or 1x4\frac{1}{x^4} would go to +∞+\infty on both sides. Second, writing lim⁡x→01x2=∞\lim_{x\to 0} \frac{1}{x^2} = \infty does not mean the limit exists: it is a precise way of saying HOW it fails to exist, the values growing without bound. Correct statement: lim⁡x→0+1x3=∞\lim_{x\to 0^+} \frac{1}{x^3} = \infty and lim⁡x→0−1x3=−∞\lim_{x\to 0^-} \frac{1}{x^3} = -\infty; the two-sided limit does not exist, and x=0x = 0 is a vertical asymptote.

Exercise 9: The brine tank: a concentration that never reaches its limit

A storage tank holds 600600 L of pure water. Brine containing 4040 g of salt per litre is pumped in at 2020 L/min; the mixture is stirred, so its concentration is the same everywhere, and nothing flows out. The tank can hold 10 00010\,000 L.

The questions ask what happens to the concentration of salt in the tank in the long run, and how long “the long run” really is. No calculator: every answer is exact.

  • a) Show that after tt minutes the concentration of salt in the tank is C(t)=40t30+tC(t) = \frac{40t}{30 + t} grams per litre.
  • b) Find lim⁡t→∞C(t)\lim_{t\to\infty} C(t) and interpret it. Show that C(t)<40C(t) < 40 for every t≥0t \ge 0.
  • c) When does the concentration reach 3030 g/L? 3636 g/L? Compare the two waiting times.
  • d) When does the tank become full, and what is the concentration then? What does the limit of b) tell you about this tank, and what does it not?
  • e) The same pump now fills a tank that starts with 600600 L of brine at 1010 g/L, or at 5050 g/L. Find the concentration in each case and its limit, and say from which side each approaches it.

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  • a) Salt 800t800t g, volume 600+20t600 + 20t L, so C(t)=800t600+20t=40t30+tC(t) = \frac{800t}{600 + 20t} = \frac{40t}{30 + t} g/L.
  • b) lim⁡t→∞C(t)=40\lim_{t\to\infty} C(t) = 40 g/L, the concentration of the incoming brine; 40−C(t)=120030+t>040 - C(t) = \frac{1200}{30 + t} > 0.
  • c) t=90t = 90 min for 3030 g/L, t=270t = 270 min for 3636 g/L: the next 66 g/L take twice as long as the first 3030.
  • d) Full at t=470t = 470 min, with C(470)=37.6C(470) = 37.6 g/L; the limit 4040 is a bound and a trend, never a value reached.
  • e) 300+40t30+t→40\frac{300 + 40t}{30 + t} \to 40 from below; 1500+40t30+t→40\frac{1500 + 40t}{30 + t} \to 40 from above.

a) Every minute the pump brings 2020 L of brine, each litre carrying 4040 g of salt, so 800800 g of salt per minute; the tank starts with no salt, so after tt minutes it contains 800t800t grams. Nothing flows out, so the volume is 600+20t600 + 20t litres. The concentration is the amount of salt divided by the volume: C(t)=800t600+20tC(t) = \frac{800t}{600 + 20t}, and dividing the numerator and the denominator by 2020 gives C(t)=40t30+tC(t) = \frac{40t}{30 + t} g/L. Check at t=0t = 0: C(0)=0C(0) = 0, pure water.

b) Divide by tt: C(t)=4030t+1→400+1=40C(t) = \frac{40}{\frac{30}{t} + 1} \to \frac{40}{0 + 1} = 40 as t→∞t \to \infty. The line C=40C = 40 is a horizontal asymptote of the graph of CC, and 4040 g/L is precisely the concentration of the brine being pumped in: after a very long time, the tank holds almost nothing but incoming brine, and the 600600 L of water it started with are diluted into insignificance. Never reached: 40−C(t)=40(30+t)−40t30+t=120030+t>040 - C(t) = \frac{40(30 + t) - 40t}{30 + t} = \frac{1200}{30 + t} > 0 for every t≥0t \ge 0. The concentration gets as close to 4040 as we like, but always from below, and the gap shrinks only like 1t\frac{1}{t}.

c) C(t)=30C(t) = 30 means 40t=30(30+t)40t = 30(30 + t), so 10t=90010t = 900 and t=90t = 90 min. C(t)=36C(t) = 36 means 40t=36(30+t)40t = 36(30 + t), so 4t=10804t = 1080 and t=270t = 270 min. The first 3030 g/L take 9090 minutes; the next 66 g/L take 180180 more minutes, twice as long. Near a horizontal asymptote, each further step toward the limit costs more time than the last: with the gap equal to 120030+t\frac{1200}{30 + t}, halving the gap means roughly doubling 30+t30 + t.

d) The volume 600+20t600 + 20t reaches 10 00010\,000 L when 20t=940020t = 9400, that is at t=470t = 470 min. Then C(470)=40⋅470500=18800500=37.6C(470) = \frac{40 \cdot 470}{500} = \frac{18800}{500} = 37.6 g/L. So in this tank the concentration never gets beyond 37.637.6 g/L: the tank is full long before the limit could matter. What the limit does tell you: 4040 g/L is a ceiling the concentration can never exceed, and the direction in which the model is heading. What it does not tell you: that the value 4040 is ever reached, or even approached closely, within the life of the model. A limit at infinity is a property of the formula; whether tt can really go to infinity is a question about the tank.

e) Starting with 600600 L at 1010 g/L, the tank holds 60006000 g of salt at t=0t = 0, so the salt is 6000+800t6000 + 800t and C1(t)=6000+800t600+20t=300+40t30+tC_1(t) = \frac{6000 + 800t}{600 + 20t} = \frac{300 + 40t}{30 + t}. Starting at 5050 g/L, the initial salt is 30 00030\,000 g and C2(t)=1500+40t30+tC_2(t) = \frac{1500 + 40t}{30 + t}. Both tend to 401=40\frac{40}{1} = 40: the limit depends only on the incoming brine and forgets the initial state. The sides: C1(t)−40=300−120030+t=−90030+t<0C_1(t) - 40 = \frac{300 - 1200}{30 + t} = -\frac{900}{30 + t} < 0, so C1C_1 approaches 4040 from below; C2(t)−40=1500−120030+t=30030+t>0C_2(t) - 40 = \frac{1500 - 1200}{30 + t} = \frac{300}{30 + t} > 0, so C2C_2 comes down to 4040 from above, the stronger initial brine being diluted by the weaker one. The solution figure shows the three tanks, and the three curves closing in on the same line.

601201802403003604204801020304050start at 50 g/Lstart with pure waterstart at 10 g/Lt (min)C (g/L)

Exercise 10: Terminal velocity: two skydivers and a parachute

Two skydivers jump from rest. Air resistance grows with speed until it balances the weight, so each speed approaches a TERMINAL VELOCITY: the limit of the speed as t→∞t \to \infty. Jumper A, in a position where drag is roughly proportional to the speed, falls at vA(t)=50(1−e−t/5)v_A(t) = 50\left(1 - e^{-t/5}\right) m/s. Jumper B, for whom drag grows like the square of the speed, falls at vB(t)=60⋅et/3−1et/3+1v_B(t) = 60 \cdot \frac{e^{t/3} - 1}{e^{t/3} + 1} m/s, with tt in seconds.

No calculator: give exact answers, then estimate them with ln⁡2≈0.69\ln 2 \approx 0.69, ln⁡3≈1.10\ln 3 \approx 1.10, ln⁡5≈1.61\ln 5 \approx 1.61 and e>2.7e > 2.7 if needed. The figure shows the two speeds.

5101520253010203040506070v = 60v = 50jumper Bjumper At (s)v (m/s)
  • a) Find the terminal velocity of each jumper, as a limit.
  • b) Prove that neither jumper ever reaches their terminal velocity.
  • c) How long does each jumper take to reach 80%80\% of their own terminal velocity?
  • d) Jumper A opens a parachute when falling at 4545 m/s. With the clock reset to s=0s = 0 at that moment, the speed becomes w(s)=5+40e−2sw(s) = 5 + 40e^{-2s} m/s. Find the new terminal velocity and from which side it is approached, and the time needed to slow down to 1010 m/s.
  • e) Show that 2020 s after the jump, jumper A is within 11 m/s of the terminal velocity, even though it is never reached.

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  • a) 5050 m/s for A, 6060 m/s for B.
  • b) 50−vA(t)=50e−t/5>050 - v_A(t) = 50e^{-t/5} > 0 and 60−vB(t)=120et/3+1>060 - v_B(t) = \frac{120}{e^{t/3} + 1} > 0.
  • c) A: t=5ln⁡5≈8.05t = 5\ln 5 \approx 8.05 s; B: t=3ln⁡9=6ln⁡3≈6.6t = 3\ln 9 = 6\ln 3 \approx 6.6 s.
  • d) 55 m/s, approached from above; s=32ln⁡2≈1.04s = \frac{3}{2}\ln 2 \approx 1.04 s.
  • e) 50−vA(20)=50e−4<150 - v_A(20) = 50e^{-4} < 1 because e4>2.74=53.1441>50e^4 > 2.7^4 = 53.1441 > 50.

a) As t→∞t \to \infty, −t5→−∞-\frac{t}{5} \to -\infty and eu→0e^u \to 0 as u→−∞u \to -\infty, so e−t/5→0e^{-t/5} \to 0 and vA(t)→50(1−0)=50v_A(t) \to 50(1 - 0) = 50 m/s. For B, both et/3−1e^{t/3} - 1 and et/3+1e^{t/3} + 1 tend to ∞\infty: the form ∞∞\frac{\infty}{\infty}. Divide by the dominant term et/3e^{t/3}: vB(t)=60⋅1−e−t/31+e−t/3→60⋅11=60v_B(t) = 60 \cdot \frac{1 - e^{-t/3}}{1 + e^{-t/3}} \to 60 \cdot \frac{1}{1} = 60 m/s. On the figure these are the two horizontal asymptotes v=50v = 50 and v=60v = 60. Answering “∞∞=1\frac{\infty}{\infty} = 1, so 6060” gets the right number for a wrong reason and loses the method mark.

b) 50−vA(t)=50e−t/550 - v_A(t) = 50e^{-t/5}, and an exponential is always positive, so vA(t)<50v_A(t) < 50 for every tt. For B: 60−vB(t)=60⋅(et/3+1)−(et/3−1)et/3+1=120et/3+1>060 - v_B(t) = 60 \cdot \frac{(e^{t/3} + 1) - (e^{t/3} - 1)}{e^{t/3} + 1} = \frac{120}{e^{t/3} + 1} > 0, so vB(t)<60v_B(t) < 60 for every tt. Both speeds approach their limit from below and never reach it: the terminal velocity is a horizontal asymptote, not a value of the function. Physically, the drag equals the weight only in the limit, so the acceleration is never exactly zero.

c) Jumper A: vA(t)=40v_A(t) = 40 means 1−e−t/5=451 - e^{-t/5} = \frac{4}{5}, so e−t/5=15e^{-t/5} = \frac{1}{5}, −t5=−ln⁡5-\frac{t}{5} = -\ln 5 and t=5ln⁡5≈5×1.61=8.05t = 5\ln 5 \approx 5 \times 1.61 = 8.05 s. Jumper B: vB(t)=48v_B(t) = 48 means u−1u+1=45\frac{u - 1}{u + 1} = \frac{4}{5} with u=et/3u = e^{t/3}, so 5u−5=4u+45u - 5 = 4u + 4 and u=9u = 9; then t3=ln⁡9=2ln⁡3\frac{t}{3} = \ln 9 = 2\ln 3 and t=6ln⁡3≈6.6t = 6\ln 3 \approx 6.6 s. Jumper B reaches 80%80\% of a HIGHER terminal velocity sooner. The substitution u=et/3u = e^{t/3} turns the equation into a linear one: solve for uu first, take the logarithm last.

d) As s→∞s \to \infty, e−2s→0e^{-2s} \to 0, so w(s)→5w(s) \to 5 m/s: the new terminal velocity, about ten times smaller. Since w(s)−5=40e−2s>0w(s) - 5 = 40e^{-2s} > 0, the speed comes DOWN to 55 m/s from above: the jumper is slowed by the parachute and approaches the asymptote from the other side. Slowing to 1010 m/s: 40e−2s=540e^{-2s} = 5, so e−2s=18e^{-2s} = \frac{1}{8}, 2s=ln⁡8=3ln⁡22s = \ln 8 = 3\ln 2 and s=32ln⁡2≈1.5×0.69≈1.04s = \frac{3}{2}\ln 2 \approx 1.5 \times 0.69 \approx 1.04 s. The side of approach is read on the sign of w(s)−5w(s) - 5, exactly as the side of an oblique asymptote is read on the sign of the remainder.

e) At t=20t = 20 s the gap is 50−vA(20)=50e−450 - v_A(20) = 50e^{-4}. It is less than 11 exactly when e4>50e^4 > 50. Since e>2.7e > 2.7, e4>2.74e^4 > 2.7^4, and by hand 2.72=7.292.7^2 = 7.29 and 7.292=53.14417.29^2 = 53.1441, so e4>53.1441>50e^4 > 53.1441 > 50. Hence 50−vA(20)<150 - v_A(20) < 1: after 2020 s jumper A falls at more than 4949 m/s, within 11 m/s of the terminal velocity, and yet vA(t)<50v_A(t) < 50 forever by b). This is the practical meaning of a limit at infinity: not that the value is reached, but that the gap becomes as small as any tolerance we fix, from some time on.

© Ahmed Squalli Houssaini. Exercise set published at www.letuteurscientifique.ca/en/exercices/math140-limits-infinity-asymptotes. Free for personal and classroom use; republishing it elsewhere requires written permission (legal notice).

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