MATH 203 Calculus I • Concordia University, Montreal

Corrected exercises: inverse trigonometric functions (MATH 203)

This is the corrected exercise set for the inverse trigonometric functions in MATH 203, Differential and Integral Calculus I, at Concordia University: section 1.6 of Thomas for sin⁡−1\sin^{-1} and cos⁡−1\cos^{-1}, and section 3.9 for all six functions and their derivatives. The chapter comes late in the term, just before related rates, and it reuses everything before it: the chain rule, implicit differentiation, the derivative as a slope. A scientific calculator is allowed, and every exact answer is also given to four decimals.

The thread running through the set: an inverse trigonometric function returns ONE angle, the one in its restricted range, and that range decides every answer. It is why sin⁡−1(sin⁡5π6)\sin^{-1}\left(\sin\frac{5\pi}{6}\right) is not 5π6\frac{5\pi}{6}, why the triangle of tan⁡−1(−2)\tan^{-1}(-2) has a positive cosine, why the derivative of sec⁡−1x\sec^{-1}x carries an ∣x∣|x|, and why an identity proved by a zero derivative has one constant PER INTERVAL. The algebraic gesture where the marks are really lost is named in every solution: bring 1+u21 + u^2 or 1−u21 - u^2 to one fraction before inverting or taking a root, and read the square root of a square as an absolute value, x2=∣x∣\sqrt{x^2} = |x|.

The traps named in the solutions: the degree mode, cos⁡−1\cos^{-1} answered with a negative angle, a domain written for xx instead of the inner function, 9−x2\sqrt{9 - x^2} taken for 3−x3 - x, (3x)2(3x)^2 written 3x23x^2, a chain factor dropped in tan⁡−11x\tan^{-1}\frac{1}{x}, sin⁡2x\sqrt{\sin^2 x} taken for sin⁡x\sin x, a constant read at a point of the wrong interval, a candidate created by squaring and kept, and a complex fraction left unsimplified.

10 corrected exercises • 100 points • 150 minutes

Revision sheet for this chapter → Every MATH 203 chapter →

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Course recap

  • • sin⁡−1x∈[−π2,π2]\sin^{-1}x \in \left[-\frac{\pi}{2}, \frac{\pi}{2}\right] for x∈[−1,1]x \in [-1, 1]; cos⁡−1x∈[0,π]\cos^{-1}x \in [0, \pi] for x∈[−1,1]x \in [-1, 1]; tan⁡−1x∈(−π2,π2)\tan^{-1}x \in \left(-\frac{\pi}{2}, \frac{\pi}{2}\right) for every xx; sec⁡−1x=cos⁡−11x\sec^{-1}x = \cos^{-1}\frac{1}{x} for ∣x∣≥1|x| \ge 1.
  • • sin⁡(sin⁡−1x)=x\sin(\sin^{-1}x) = x on [−1,1][-1, 1], but sin⁡−1(sin⁡x)=x\sin^{-1}(\sin x) = x only on [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]. cos⁡−1(−x)=π−cos⁡−1x\cos^{-1}(-x) = \pi - \cos^{-1}x and sin⁡−1x+cos⁡−1x=π2\sin^{-1}x + \cos^{-1}x = \frac{\pi}{2}.
  • • ddxsin⁡−1u=u′1−u2\frac{d}{dx}\sin^{-1}u = \frac{u'}{\sqrt{1 - u^2}}, ddxcos⁡−1u=−u′1−u2\frac{d}{dx}\cos^{-1}u = -\frac{u'}{\sqrt{1 - u^2}}, ddxtan⁡−1u=u′1+u2\frac{d}{dx}\tan^{-1}u = \frac{u'}{1 + u^2}, ddxsec⁡−1u=u′∣u∣u2−1\frac{d}{dx}\sec^{-1}u = \frac{u'}{|u|\sqrt{u^2 - 1}}.
  • • cot⁡−1x=π2−tan⁡−1x\cot^{-1}x = \frac{\pi}{2} - \tan^{-1}x and csc⁡−1x=π2−sec⁡−1x\csc^{-1}x = \frac{\pi}{2} - \sec^{-1}x: their derivatives are the opposites.
  • • x2=∣x∣\sqrt{x^2} = |x|. A complex fraction is simplified by multiplying its top and bottom by the common denominator of the small fractions.
  • • If F′(x)=0F'(x) = 0 at every point of an interval, FF is constant on that interval: read the constant at a point of THAT interval.

Part A: the basics (/50)

Exercise 1: Restricted ranges: the one angle an inverse function returns

Sine, cosine and tangent take each of their values infinitely often, so none of them has an inverse on its whole domain. Thomas (section 1.6) restricts each one to an interval where it is one-to-one and inverts the restriction. y=sin⁡−1x=arcsin⁡xy = \sin^{-1}x = \arcsin x is THE angle yy of [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right] with sin⁡y=x\sin y = x, defined for −1≤x≤1-1 \le x \le 1. y=cos⁡−1x=arccos⁡xy = \cos^{-1}x = \arccos x is the angle of [0,π][0, \pi] with cos⁡y=x\cos y = x. y=tan⁡−1x=arctan⁡xy = \tan^{-1}x = \arctan x is the angle of (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right) with tan⁡y=x\tan y = x, defined for every real xx. The −1-1 of sin⁡−1\sin^{-1} names an inverse function, it is NOT an exponent.

The figure shows y=sin⁡xy = \sin x for −2π≤x≤2π-2\pi \le x \le 2\pi, the restricted piece on [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right] in blue, and the dashed line y=12y = \frac{1}{2}. A scientific calculator is allowed, in RADIAN mode.

-7-6-5-4-3-2-11234567-1.5-1-0.50.511.5π/2−π/2y = 1/2y = sin x
  • a) Find exactly, in radians: arcsin⁡(−12)\arcsin\left(-\frac{1}{2}\right), arccos⁡(−32)\arccos\left(-\frac{\sqrt 3}{2}\right), arctan⁡3\arctan\sqrt 3, arccos⁡0\arccos 0 and arctan⁡(−1)\arctan(-1).
  • b) Using the figure, how many solutions does the equation sin⁡x=12\sin x = \frac{1}{2} have on [−2π,2π][-2\pi, 2\pi]? Give them all exactly, and say which one is arcsin⁡12\arcsin\frac{1}{2} and why.
  • c) Find the domain of f(x)=arcsin⁡(2x−3)f(x) = \arcsin(2x - 3), of g(x)=arccos⁡x−13g(x) = \arccos\frac{x - 1}{3} and of h(x)=arctan⁡4−xh(x) = \arctan\sqrt{4 - x}.
  • d) In radian mode, a calculator gives cos⁡−1(0.2)≈1.3694\cos^{-1}(0.2) \approx 1.3694. Using only this value, the identity arccos⁡(−x)=π−arccos⁡x\arccos(-x) = \pi - \arccos x and the identity arcsin⁡x+arccos⁡x=π2\arcsin x + \arccos x = \frac{\pi}{2} of Thomas 1.6, find arccos⁡(−0.2)\arccos(-0.2) and arcsin⁡(0.2)\arcsin(0.2) to four decimals. Explain the first identity with the unit circle.
  • e) A student whose calculator is in degree mode types tan⁡−1(1)\tan^{-1}(1) and reads 4545, then types sin⁡−1(2)\sin^{-1}(2) and reads an error message. Give arctan⁡1\arctan 1 in radians, exactly and to four decimals, and explain the error message.

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a)
b)
c)
Domain of ff ,
Domain of gg ,
Domain of hh ,
d)
e)
Show the solution

Answers

  • a) −π6-\frac{\pi}{6}, 5π6\frac{5\pi}{6}, π3\frac{\pi}{3}, π2\frac{\pi}{2}, −π4-\frac{\pi}{4}
  • b) Four solutions: −11π6-\frac{11\pi}{6}, −7π6-\frac{7\pi}{6}, π6\frac{\pi}{6}, 5π6\frac{5\pi}{6}; arcsin⁡12=π6\arcsin\frac{1}{2} = \frac{\pi}{6}, the only one on the blue piece
  • c) ff: [1,2][1, 2]; gg: [−2,4][-2, 4]; hh: (−∞,4](-\infty, 4]
  • d) arccos⁡(−0.2)≈1.7722\arccos(-0.2) \approx 1.7722, arcsin⁡(0.2)≈0.2014\arcsin(0.2) \approx 0.2014
  • e) arctan⁡1=π4≈0.7854\arctan 1 = \frac{\pi}{4} \approx 0.7854; sin⁡−1(2)\sin^{-1}(2) does not exist, since 22 is not the sine of any angle

a) Each answer is found by asking which angle OF THE RANGE has the given sine, cosine or tangent. sin⁡(−π6)=−12\sin\left(-\frac{\pi}{6}\right) = -\frac{1}{2} and −π6∈[−π2,π2]-\frac{\pi}{6} \in \left[-\frac{\pi}{2}, \frac{\pi}{2}\right], so arcsin⁡(−12)=−π6\arcsin\left(-\frac{1}{2}\right) = -\frac{\pi}{6}; the angle 7π6\frac{7\pi}{6} also has sine −12-\frac{1}{2}, but it is not in the range. cos⁡5π6=−32\cos\frac{5\pi}{6} = -\frac{\sqrt 3}{2} with 5π6∈[0,π]\frac{5\pi}{6} \in [0, \pi], so arccos⁡(−32)=5π6\arccos\left(-\frac{\sqrt 3}{2}\right) = \frac{5\pi}{6}: the answer −π6-\frac{\pi}{6}, which a student gets by copying the sine case, is outside [0,π][0, \pi] and its cosine is +32+\frac{\sqrt 3}{2}. tan⁡π3=3\tan\frac{\pi}{3} = \sqrt 3, so arctan⁡3=π3\arctan\sqrt 3 = \frac{\pi}{3}. cos⁡π2=0\cos\frac{\pi}{2} = 0, so arccos⁡0=π2\arccos 0 = \frac{\pi}{2}. tan⁡(−π4)=−1\tan\left(-\frac{\pi}{4}\right) = -1, so arctan⁡(−1)=−π4\arctan(-1) = -\frac{\pi}{4}, and not 3π4\frac{3\pi}{4}, which has the same tangent but lies outside (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right). The rule to memorize: a negative input sends arcsin⁡\arcsin and arctan⁡\arctan below zero, and sends arccos⁡\arccos into the second quadrant.

b) The dashed line y=12y = \frac{1}{2} crosses the grey curve four times on [−2π,2π][-2\pi, 2\pi]. On [0,2π][0, 2\pi], the solutions are π6\frac{\pi}{6} and π−π6=5π6\pi - \frac{\pi}{6} = \frac{5\pi}{6}, since sin⁡(π−x)=sin⁡x\sin(\pi - x) = \sin x. Subtracting one period 2π2\pi gives the two others: π6−2π=−11π6\frac{\pi}{6} - 2\pi = -\frac{11\pi}{6} and 5π6−2π=−7π6\frac{5\pi}{6} - 2\pi = -\frac{7\pi}{6}. Four solutions, and the calculator key sin⁡−1\sin^{-1} returns only ONE of them, π6≈0.5236\frac{\pi}{6} \approx 0.5236: the only one on the blue piece, because arcsin⁡\arcsin is by definition the inverse of the RESTRICTED sine. That is the whole chapter in one picture: an inverse trigonometric function answers the question 'which angle of my range', never 'which angles'.

c) Each inverse function imposes a condition on what is inside it, and the domain is found by solving an inequality: this is the algebra that costs marks. arcsin⁡u\arcsin u needs −1≤u≤1-1 \le u \le 1: −1≤2x−3≤1-1 \le 2x - 3 \le 1, add 33 to the three members, 2≤2x≤42 \le 2x \le 4, divide by 22: 1≤x≤21 \le x \le 2, so the domain of ff is [1,2][1, 2]. arccos⁡u\arccos u needs the same: −1≤x−13≤1-1 \le \frac{x - 1}{3} \le 1, multiply by 33, −3≤x−1≤3-3 \le x - 1 \le 3, so −2≤x≤4-2 \le x \le 4. arctan⁡\arctan accepts every real number, so the only condition on hh comes from the square root: 4−x≥04 - x \ge 0, that is x≤4x \le 4, and the domain is (−∞,4](-\infty, 4]. The classic slip is to answer [−1,1][-1, 1] for ff, the domain of arcsin⁡x\arcsin x itself: the condition is on the INSIDE 2x−32x - 3, not on xx.

d) On the unit circle, the angle α=arccos⁡x\alpha = \arccos x of [0,π][0, \pi] has the point (x,sin⁡α)(x, \sin\alpha); the angle π−α\pi - \alpha, also in [0,π][0, \pi], is its mirror image in the vertical axis, with first coordinate −x-x. So cos⁡(π−α)=−x\cos(\pi - \alpha) = -x, and since π−α\pi - \alpha is in the range, arccos⁡(−x)=π−arccos⁡x\arccos(-x) = \pi - \arccos x. With arccos⁡(0.2)≈1.369438\arccos(0.2) \approx 1.369438: arccos⁡(−0.2)=π−1.369438≈1.772154\arccos(-0.2) = \pi - 1.369438 \approx 1.772154, that is 1.77221.7722 to four decimals. Then arcsin⁡(0.2)=π2−arccos⁡(0.2)≈1.570796−1.369438=0.201358\arcsin(0.2) = \frac{\pi}{2} - \arccos(0.2) \approx 1.570796 - 1.369438 = 0.201358, that is 0.20140.2014. Both are checked directly on the calculator. The false symmetry arccos⁡(−x)=−arccos⁡x\arccos(-x) = -\arccos x gives a NEGATIVE answer, impossible for arccos⁡\arccos, whose values are in [0,π][0, \pi]: that alone refutes it.

e) In degree mode the calculator returns angles in degrees: 4545 means 45°45°, and 45°=π445° = \frac{\pi}{4} rad. In calculus every angle is in radians, because the derivative formulas of the chapter, such as ddxarctan⁡x=11+x2\frac{d}{dx}\arctan x = \frac{1}{1 + x^2}, are only true in radians. So arctan⁡1=π4≈0.7854\arctan 1 = \frac{\pi}{4} \approx 0.7854; a 4545 copied into a tangent line or a limit makes the whole answer wrong by a factor 180π\frac{180}{\pi}. The error message on sin⁡−1(2)\sin^{-1}(2) is correct: sin⁡−1\sin^{-1} is only defined on [−1,1][-1, 1], since no angle has a sine equal to 22. It is not the reciprocal 1sin⁡2≈1.0998\frac{1}{\sin 2} \approx 1.0998, which does exist: the reciprocal of the sine is csc⁡\csc. Check the mode before the first question of any test: sin⁡−1(1)\sin^{-1}(1) must display 1.57081.5708.

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Exercise 2: Compositions and the reference triangle: the range fixes the sign

sin⁡(arcsin⁡x)=x\sin(\arcsin x) = x for every xx of [−1,1][-1, 1]: the inverse acts first and the sine undoes it. The other order is the trap: arcsin⁡(sin⁡x)=x\arcsin(\sin x) = x ONLY when xx is already in [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right], because arcsin⁡\arcsin can only return an angle of its range. To evaluate a trigonometric function of an inverse trigonometric function, draw the right triangle of the angle, find the missing side by Pythagoras, then fix the SIGN with the range.

The figure shows the triangle of θ=arcsin⁡x3\theta = \arcsin\frac{x}{3} for 0<x<30 < x < 3: hypotenuse 33, side opposite θ\theta equal to xx, so that sin⁡θ=x3\sin\theta = \frac{x}{3}.

θ3x√(9 − x²)
  • a) Find exactly: arcsin⁡(sin⁡7π6)\arcsin\left(\sin\frac{7\pi}{6}\right), arccos⁡(cos⁡5π3)\arccos\left(\cos\frac{5\pi}{3}\right) and arctan⁡(tan⁡(−3π4))\arctan\left(\tan\left(-\frac{3\pi}{4}\right)\right).
  • b) Find exactly, then to four decimals: cos⁡(arctan⁡(−2))\cos(\arctan(-2)), sin⁡(arctan⁡(−2))\sin(\arctan(-2)) and tan⁡(arcsin⁡(−513))\tan\left(\arcsin\left(-\frac{5}{13}\right)\right).
  • c) Using the triangle of the figure, write cos⁡(arcsin⁡x3)\cos\left(\arcsin\frac{x}{3}\right) and tan⁡(arcsin⁡x3)\tan\left(\arcsin\frac{x}{3}\right) as algebraic expressions in xx, and say for which xx each one holds. With a triangle of your own, write sec⁡(arctan⁡2x)\sec(\arctan 2x) in the same way. Evaluate the second expression at x=1x = 1 and the third at x=1x = 1.
  • d) Thomas also defines sec⁡−1x=cos⁡−11x\sec^{-1}x = \cos^{-1}\frac{1}{x} for ∣x∣≥1|x| \ge 1, with values in [0,π][0, \pi] except π2\frac{\pi}{2}. Find sec⁡−12\sec^{-1}2, sec⁡−1(−2)\sec^{-1}(-2) and tan⁡(sec⁡−1(−2))\tan\left(\sec^{-1}(-2)\right). Show that tan⁡(sec⁡−1x)=x2−1\tan(\sec^{-1}x) = \sqrt{x^2 - 1} for x≥1x \ge 1 but −x2−1-\sqrt{x^2 - 1} for x≤−1x \le -1.
  • e) Solve for xx: arcsin⁡(2x)=π6\arcsin(2x) = \frac{\pi}{6}; arctan⁡(x−1)=−π3\arctan(x - 1) = -\frac{\pi}{3}; arccos⁡x=4π3\arccos x = \frac{4\pi}{3}.

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a)
b)
c)
d)
e)
Show the solution

Answers

  • a) −π6-\frac{\pi}{6}, π3\frac{\pi}{3}, π4\frac{\pi}{4}
  • b) 15≈0.4472\frac{1}{\sqrt 5} \approx 0.4472, −25≈−0.8944-\frac{2}{\sqrt 5} \approx -0.8944, −512≈−0.4167-\frac{5}{12} \approx -0.4167
  • c) 9−x23\frac{\sqrt{9 - x^2}}{3} on [−3,3][-3, 3]; x9−x2\frac{x}{\sqrt{9 - x^2}} on (−3,3)(-3, 3); 1+4x2\sqrt{1 + 4x^2} for every xx; values 122≈0.3536\frac{1}{2\sqrt 2} \approx 0.3536 and 5≈2.2361\sqrt 5 \approx 2.2361
  • d) π3\frac{\pi}{3}, 2π3\frac{2\pi}{3}, −3-\sqrt 3; the sign of tan⁡\tan follows the quadrant of the angle
  • e) x=14x = \frac{1}{4}; x=1−3x = 1 - \sqrt 3; no solution, 4π3\frac{4\pi}{3} is not in [0,π][0, \pi]

a) Compute the inner value first, then ask for the angle OF THE RANGE. sin⁡7π6=−12\sin\frac{7\pi}{6} = -\frac{1}{2}, and the angle of [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right] with sine −12-\frac{1}{2} is −π6-\frac{\pi}{6}. cos⁡5π3=12\cos\frac{5\pi}{3} = \frac{1}{2}, and the angle of [0,π][0, \pi] with cosine 12\frac{1}{2} is π3\frac{\pi}{3}. tan⁡(−3π4)=1\tan\left(-\frac{3\pi}{4}\right) = 1, since the tangent has period π\pi and −3π4+π=π4-\frac{3\pi}{4} + \pi = \frac{\pi}{4}; the angle of (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right) with tangent 11 is π4\frac{\pi}{4}. None of the three answers is the angle we started from: each of 7π6\frac{7\pi}{6}, 5π3\frac{5\pi}{3}, −3π4-\frac{3\pi}{4} lies outside the range of its inverse, and writing it back as the answer is the most frequent zero of the chapter.

b) Let θ=arctan⁡(−2)\theta = \arctan(-2). Then tan⁡θ=−2\tan\theta = -2 and θ∈(−π2,0)\theta \in \left(-\frac{\pi}{2}, 0\right), a fourth-quadrant angle: cosine POSITIVE, sine NEGATIVE. The triangle with opposite side 22 and adjacent side 11 has hypotenuse 1+4=5\sqrt{1 + 4} = \sqrt 5, so cos⁡θ=15=55≈0.4472\cos\theta = \frac{1}{\sqrt 5} = \frac{\sqrt 5}{5} \approx 0.4472 and sin⁡θ=−25≈−0.8944\sin\theta = -\frac{2}{\sqrt 5} \approx -0.8944. The triangle gives the SIZES, the range gives the SIGNS. Let φ=arcsin⁡(−513)\varphi = \arcsin\left(-\frac{5}{13}\right), also in (−π2,0)\left(-\frac{\pi}{2}, 0\right): the triangle 55, 1313 has third side 169−25=12\sqrt{169 - 25} = 12, cos⁡φ=+1213\cos\varphi = +\frac{12}{13} and tan⁡φ=−5/1312/13=−512≈−0.4167\tan\varphi = \frac{-5/13}{12/13} = -\frac{5}{12} \approx -0.4167. A student who takes cos⁡θ=−15\cos\theta = -\frac{1}{\sqrt 5} because the input was negative has moved the angle to the second quadrant, where arctan⁡\arctan never goes.

c) In the figure, the adjacent side is 32−x2=9−x2\sqrt{3^2 - x^2} = \sqrt{9 - x^2} by Pythagoras. It is NOT 3−x3 - x: a square root does not distribute over a difference, and 9−4=5≠1\sqrt{9 - 4} = \sqrt 5 \ne 1 settles it. So cos⁡(arcsin⁡x3)=9−x23\cos\left(\arcsin\frac{x}{3}\right) = \frac{\sqrt{9 - x^2}}{3}. The triangle only shows 0<x<30 < x < 3, but the formula holds on all of [−3,3][-3, 3]: θ\theta is in [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right], where the cosine is never negative, so the positive root is the right one. Then tan⁡(arcsin⁡x3)=x9−x2\tan\left(\arcsin\frac{x}{3}\right) = \frac{x}{\sqrt{9 - x^2}} for −3<x<3-3 < x < 3 (the sign now comes from xx, as it should). At x=1x = 1: 18=24≈0.3536\frac{1}{\sqrt 8} = \frac{\sqrt 2}{4} \approx 0.3536. For β=arctan⁡2x\beta = \arctan 2x: opposite side 2x2x, adjacent 11, hypotenuse 1+(2x)2=1+4x2\sqrt{1 + (2x)^2} = \sqrt{1 + 4x^2}, and since cos⁡β>0\cos\beta > 0 on the range, sec⁡β=1+4x2\sec\beta = \sqrt{1 + 4x^2} for every xx. Watch the square: (2x)2=4x2(2x)^2 = 4x^2, not 2x22x^2. At x=1x = 1: 5≈2.2361\sqrt 5 \approx 2.2361.

d) sec⁡−12=cos⁡−112=π3\sec^{-1}2 = \cos^{-1}\frac{1}{2} = \frac{\pi}{3} and sec⁡−1(−2)=cos⁡−1(−12)=2π3\sec^{-1}(-2) = \cos^{-1}\left(-\frac{1}{2}\right) = \frac{2\pi}{3}. The angle 2π3\frac{2\pi}{3} is in the second quadrant, so tan⁡2π3=−3≈−1.7321\tan\frac{2\pi}{3} = -\sqrt 3 \approx -1.7321. In general, let y=sec⁡−1xy = \sec^{-1}x, so sec⁡y=x\sec y = x and tan⁡2y=sec⁡2y−1=x2−1\tan^2 y = \sec^2 y - 1 = x^2 - 1, which gives tan⁡y=±x2−1\tan y = \pm\sqrt{x^2 - 1}, and the range decides. For x≥1x \ge 1, cos⁡y=1x>0\cos y = \frac{1}{x} > 0, so y∈[0,π2)y \in \left[0, \frac{\pi}{2}\right) and tan⁡y≥0\tan y \ge 0: tan⁡(sec⁡−1x)=x2−1\tan(\sec^{-1}x) = \sqrt{x^2 - 1}. For x≤−1x \le -1, cos⁡y<0\cos y < 0, so y∈(π2,π]y \in \left(\frac{\pi}{2}, \pi\right] and tan⁡y≤0\tan y \le 0: tan⁡(sec⁡−1x)=−x2−1\tan(\sec^{-1}x) = -\sqrt{x^2 - 1}. Check at x=−2x = -2: −3-\sqrt 3, as found directly. This sign is exactly the one that will put an absolute value in the derivative of sec⁡−1x\sec^{-1}x.

e) Apply the direct function to both sides, but only after checking that the right side is in the range. π6\frac{\pi}{6} is in [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right], so arcsin⁡(2x)=π6\arcsin(2x) = \frac{\pi}{6} gives 2x=sin⁡π6=122x = \sin\frac{\pi}{6} = \frac{1}{2} and x=14x = \frac{1}{4}; check: arcsin⁡12=π6\arcsin\frac{1}{2} = \frac{\pi}{6}. −π3-\frac{\pi}{3} is in (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right), so x−1=tan⁡(−π3)=−3x - 1 = \tan\left(-\frac{\pi}{3}\right) = -\sqrt 3 and x=1−3≈−0.7321x = 1 - \sqrt 3 \approx -0.7321. For the third, 4π3>π\frac{4\pi}{3} > \pi is NOT a value of arccos⁡\arccos: the equation has no solution. Taking the cosine of both sides blindly gives x=cos⁡4π3=−12x = \cos\frac{4\pi}{3} = -\frac{1}{2}, and the check refutes it at once: arccos⁡(−12)=2π3≠4π3\arccos\left(-\frac{1}{2}\right) = \frac{2\pi}{3} \ne \frac{4\pi}{3}.

Exercise 3: Derivatives of arcsin, arccos and arctan: the formula is one line, the algebra is the rest

Thomas (section 3.9) gives, for a differentiable inner function uu of xx: ddxsin⁡−1u=u′1−u2\frac{d}{dx}\sin^{-1}u = \frac{u'}{\sqrt{1 - u^2}} and ddxcos⁡−1u=−u′1−u2\frac{d}{dx}\cos^{-1}u = -\frac{u'}{\sqrt{1 - u^2}} for ∣u∣<1|u| < 1, and ddxtan⁡−1u=u′1+u2\frac{d}{dx}\tan^{-1}u = \frac{u'}{1 + u^2} for every uu.

Every one of these formulas contains 1−u21 - u^2 or 1+u21 + u^2. When uu is a power, a fraction or a root, that expression is where the marks are lost: square uu correctly, bring 1±u21 \pm u^2 to ONE fraction, then take the root or invert. Exact answers, then the decimal asked.

  • a) Differentiate f(x)=arccos⁡(x2)f(x) = \arccos(x^2), g(x)=arctan⁡(x2−1)g(x) = \arctan(x^2 - 1) and h(x)=arcsin⁡xh(x) = \arcsin\sqrt x, naming each inner function, simplify, and evaluate f′(12)f'\left(\frac{1}{2}\right), g′(1)g'(1) and h′(12)h'\left(\frac{1}{2}\right).
  • b) Differentiate y=arcsin⁡x1+x2y = \arcsin\frac{x}{\sqrt{1 + x^2}} and show that y′=11+x2y' = \frac{1}{1 + x^2}. Which familiar function has the same derivative and the same value at x=0x = 0? What do you conclude?
  • c) Differentiate k(x)=(1+x2)arctan⁡xk(x) = (1 + x^2)\arctan x and m(x)=arcsin⁡xxm(x) = \frac{\arcsin x}{x}, and evaluate k′(1)k'(1) and m′(12)m'\left(\frac{1}{2}\right).
  • d) Find the equation of the tangent line to y=arccos⁡x2y = \arccos\frac{x}{2} at x=1x = 1.
  • e) Show that y=arctan⁡xy = \arctan x satisfies (1+x2)y′′+2xy′=0(1 + x^2)y'' + 2xy' = 0, and give y′′(1)y''(1).

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  • a) f′=−2x1−x4f' = -\frac{2x}{\sqrt{1 - x^4}}, f′(12)=−415f'\left(\frac{1}{2}\right) = -\frac{4}{\sqrt{15}}; g′=2xx4−2x2+2g' = \frac{2x}{x^4 - 2x^2 + 2}, g′(1)=2g'(1) = 2; h′=12x1−xh' = \frac{1}{2\sqrt{x}\sqrt{1 - x}}, h′(12)=1h'\left(\frac{1}{2}\right) = 1
  • b) y′=11+x2y' = \frac{1}{1 + x^2}; y=arctan⁡xy = \arctan x for every xx
  • c) k′=2xarctan⁡x+1k' = 2x\arctan x + 1, k′(1)=π2+1k'(1) = \frac{\pi}{2} + 1; m′=x1−x2−arcsin⁡xx2m' = \frac{\frac{x}{\sqrt{1 - x^2}} - \arcsin x}{x^2}, m′(12)=43−2π3≈0.2150m'\left(\frac{1}{2}\right) = \frac{4}{\sqrt 3} - \frac{2\pi}{3} \approx 0.2150
  • d) y=−13x+π3+13y = -\frac{1}{\sqrt 3}x + \frac{\pi}{3} + \frac{1}{\sqrt 3}
  • e) y′′=−2x(1+x2)2y'' = -\frac{2x}{(1 + x^2)^2}, y′′(1)=−12y''(1) = -\frac{1}{2}

a) ff: inner function u=x2u = x^2, u′=2xu' = 2x, and u2=(x2)2=x4u^2 = (x^2)^2 = x^4, so f′(x)=−2x1−x4f'(x) = -\frac{2x}{\sqrt{1 - x^4}} for ∣x∣<1|x| < 1. At 12\frac{1}{2}: 1−116=15161 - \frac{1}{16} = \frac{15}{16}, 1516=154\sqrt{\frac{15}{16}} = \frac{\sqrt{15}}{4}, and f′(12)=−1⋅415=−415≈−1.0328f'\left(\frac{1}{2}\right) = -1 \cdot \frac{4}{\sqrt{15}} = -\frac{4}{\sqrt{15}} \approx -1.0328. The slip to avoid: 1−x2\sqrt{1 - x^2}, the formula of arccos⁡x\arccos x copied without replacing xx by uu. gg: inner function u=x2−1u = x^2 - 1, u′=2xu' = 2x, 1+u2=1+x4−2x2+1=x4−2x2+21 + u^2 = 1 + x^4 - 2x^2 + 1 = x^4 - 2x^2 + 2, so g′(x)=2xx4−2x2+2g'(x) = \frac{2x}{x^4 - 2x^2 + 2} and g′(1)=21=2g'(1) = \frac{2}{1} = 2. Expanding (x2−1)2(x^2 - 1)^2 as x4−1x^4 - 1 would give g′(1)=2g'(1) = 2 by luck here but a wrong function everywhere else, for example 416=14\frac{4}{16} = \frac{1}{4} instead of 410\frac{4}{10} at x=2x = 2. hh: inner function u=xu = \sqrt x, u′=12xu' = \frac{1}{2\sqrt x}, u2=xu^2 = x, so h′(x)=12x1−xh'(x) = \frac{1}{2\sqrt x\sqrt{1 - x}} for 0<x<10 < x < 1, and h′(12)=12⋅12⋅12=1h'\left(\frac{1}{2}\right) = \frac{1}{2 \cdot \frac{1}{\sqrt 2} \cdot \frac{1}{\sqrt 2}} = 1.

b) Write u=x(1+x2)−1/2u = x(1 + x^2)^{-1/2} and use the product rule with the chain rule on the second factor: u′=(1+x2)−1/2−x2(1+x2)−3/2u' = (1 + x^2)^{-1/2} - x^2(1 + x^2)^{-3/2}. Factor the SMALLEST power, (1+x2)−3/2(1 + x^2)^{-3/2}: u′=(1+x2)−3/2[(1+x2)−x2]=(1+x2)−3/2u' = (1 + x^2)^{-3/2}\left[(1 + x^2) - x^2\right] = (1 + x^2)^{-3/2}. Then bring 1−u21 - u^2 to one fraction: 1−x21+x2=1+x2−x21+x2=11+x21 - \frac{x^2}{1 + x^2} = \frac{1 + x^2 - x^2}{1 + x^2} = \frac{1}{1 + x^2}, whose root is (1+x2)−1/2(1 + x^2)^{-1/2}. Finally y′=(1+x2)−3/2(1+x2)−1/2=(1+x2)−1=11+x2y' = \frac{(1 + x^2)^{-3/2}}{(1 + x^2)^{-1/2}} = (1 + x^2)^{-1} = \frac{1}{1 + x^2}. This is the derivative of arctan⁡x\arctan x, and both functions are 00 at x=0x = 0. Their difference has derivative 00 on the whole interval (−∞,∞)(-\infty, \infty), so it is constant (a fact used as a tool, the constant being read at a point), and that constant is 00: arcsin⁡x1+x2=arctan⁡x\arcsin\frac{x}{\sqrt{1 + x^2}} = \arctan x for every xx. The triangle confirms it: the angle with opposite side xx and adjacent side 11 has hypotenuse 1+x2\sqrt{1 + x^2}.

c) Product rule on kk: k′(x)=2xarctan⁡x+(1+x2)⋅11+x2=2xarctan⁡x+1k'(x) = 2x\arctan x + (1 + x^2) \cdot \frac{1}{1 + x^2} = 2x\arctan x + 1. The factor 1+x21 + x^2 was chosen to cancel the denominator; simplify it rather than leaving 1+x21+x2\frac{1 + x^2}{1 + x^2}. At x=1x = 1: k′(1)=2⋅π4+1=π2+1≈2.5708k'(1) = 2 \cdot \frac{\pi}{4} + 1 = \frac{\pi}{2} + 1 \approx 2.5708. Quotient rule on mm, for x≠0x \ne 0 in [−1,1][-1, 1]: m′(x)=x⋅11−x2−arcsin⁡x⋅1x2m'(x) = \frac{x \cdot \frac{1}{\sqrt{1 - x^2}} - \arcsin x \cdot 1}{x^2}. At x=12x = \frac{1}{2}: 1/23/2=13\frac{1/2}{\sqrt 3/2} = \frac{1}{\sqrt 3}, arcsin⁡12=π6\arcsin\frac{1}{2} = \frac{\pi}{6}, so m′(12)=4(13−π6)=43−2π3≈0.2150m'\left(\frac{1}{2}\right) = 4\left(\frac{1}{\sqrt 3} - \frac{\pi}{6}\right) = \frac{4}{\sqrt 3} - \frac{2\pi}{3} \approx 0.2150. The order of the numerator is 'derivative of the top times the bottom, minus the top times the derivative of the bottom': swapped, it gives −0.2150-0.2150.

d) Point: y(1)=arccos⁡12=π3y(1) = \arccos\frac{1}{2} = \frac{\pi}{3}. Slope: inner function u=x2u = \frac{x}{2}, u′=12u' = \frac{1}{2}, 1−u2=1−x24=4−x241 - u^2 = 1 - \frac{x^2}{4} = \frac{4 - x^2}{4}, so y′=−1/24−x2/2=−14−x2y' = -\frac{1/2}{\sqrt{4 - x^2}/2} = -\frac{1}{\sqrt{4 - x^2}}. At x=1x = 1: −13≈−0.5774-\frac{1}{\sqrt 3} \approx -0.5774. Tangent: y−π3=−13(x−1)y - \frac{\pi}{3} = -\frac{1}{\sqrt 3}(x - 1), that is y=−13x+π3+13y = -\frac{1}{\sqrt 3}x + \frac{\pi}{3} + \frac{1}{\sqrt 3}, with yy-intercept ≈1.6245\approx 1.6245. Two checks: the slope is negative, as it must be for an arccosine, and the point (1,π3)\left(1, \frac{\pi}{3}\right) satisfies the tangent equation. Forgetting the inner derivative 12\frac{1}{2} gives the slope −23-\frac{2}{\sqrt 3}, twice too steep.

e) y′=11+x2=(1+x2)−1y' = \frac{1}{1 + x^2} = (1 + x^2)^{-1}, and by the chain rule y′′=−(1+x2)−2⋅2x=−2x(1+x2)2y'' = -(1 + x^2)^{-2} \cdot 2x = -\frac{2x}{(1 + x^2)^2}. Then (1+x2)y′′=−2x1+x2(1 + x^2)y'' = -\frac{2x}{1 + x^2} and 2xy′=2x1+x22xy' = \frac{2x}{1 + x^2}: the sum is 00 for every xx. At x=1x = 1: y′′(1)=−24=−12y''(1) = -\frac{2}{4} = -\frac{1}{2}. Rewriting 11+x2\frac{1}{1 + x^2} as a power BEFORE differentiating spares the quotient rule, and it is the rewriting that the exam rewards: the student who differentiates 11+x2\frac{1}{1 + x^2} as 12x\frac{1}{2x} has differentiated the denominator alone, and that is not a rule.

Exercise 4: The derivative of arcsec by implicit differentiation, and the absolute value it needs

Thomas defines y=sec⁡−1xy = \sec^{-1}x for ∣x∣≥1|x| \ge 1 as the angle yy of [0,π][0, \pi], y≠π2y \ne \frac{\pi}{2}, with sec⁡y=x\sec y = x. Equivalently sec⁡−1x=cos⁡−11x\sec^{-1}x = \cos^{-1}\frac{1}{x}. The figure shows its graph: a right branch from (1,0)(1, 0) and a left branch ending at (−1,π)(-1, \pi), both approaching the dashed line y=π2y = \frac{\pi}{2}, and BOTH rising from left to right.

Its derivative is the one formula of section 3.9 with an absolute value in it, and this exercise is about where that absolute value comes from.

-6-5-4-3-2-1123456-0.50.511.522.533.5y = sec⁻¹xy = π/2(−1, π)
  • a) Let y=sec⁡−1xy = \sec^{-1}x with ∣x∣>1|x| > 1. Differentiate sec⁡y=x\sec y = x implicitly, show that dydx=1sec⁡ytan⁡y\frac{dy}{dx} = \frac{1}{\sec y\tan y}, then express sec⁡ytan⁡y\sec y\tan y in terms of xx on each branch, and conclude that ddxsec⁡−1x=1∣x∣x2−1\frac{d}{dx}\sec^{-1}x = \frac{1}{|x|\sqrt{x^2 - 1}}. Evaluate at x=2x = 2 and at x=−2x = -2.
  • b) Check the result by a second route: differentiate cos⁡−11x\cos^{-1}\frac{1}{x} with the chain rule, and simplify 1−1x2\sqrt{1 - \frac{1}{x^2}} correctly.
  • c) Thomas obtains three derivatives from identities: cos⁡−1x=π2−sin⁡−1x\cos^{-1}x = \frac{\pi}{2} - \sin^{-1}x, cot⁡−1x=π2−tan⁡−1x\cot^{-1}x = \frac{\pi}{2} - \tan^{-1}x, csc⁡−1x=π2−sec⁡−1x\csc^{-1}x = \frac{\pi}{2} - \sec^{-1}x. Deduce the derivatives of cot⁡−1x\cot^{-1}x and csc⁡−1x\csc^{-1}x, and evaluate the first at x=1x = 1, the second at x=−2x = -2.
  • d) Differentiate f(x)=sec⁡−1(3x)f(x) = \sec^{-1}(3x) for x<−13x < -\frac{1}{3} and evaluate f′(−23)f'\left(-\frac{2}{3}\right). A student writes f′(x)=33x9x2−1f'(x) = \frac{3}{3x\sqrt{9x^2 - 1}}: what value does he find, and how does the figure tell him he is wrong before any computation?
  • e) Find the equation of the tangent line to y=sec⁡−1xy = \sec^{-1}x at x=−2x = -2.

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  • a) sec⁡ytan⁡y⋅y′=1\sec y\tan y \cdot y' = 1; sec⁡ytan⁡y=∣x∣x2−1\sec y\tan y = |x|\sqrt{x^2 - 1} on both branches; 123≈0.2887\frac{1}{2\sqrt 3} \approx 0.2887 at x=2x = 2 AND at x=−2x = -2
  • b) 1−1x2=x2−1∣x∣\sqrt{1 - \frac{1}{x^2}} = \frac{\sqrt{x^2 - 1}}{|x|}, and the chain rule gives 1∣x∣x2−1\frac{1}{|x|\sqrt{x^2 - 1}} again
  • c) ddxcot⁡−1x=−11+x2\frac{d}{dx}\cot^{-1}x = -\frac{1}{1 + x^2}, −12-\frac{1}{2} at 11; ddxcsc⁡−1x=−1∣x∣x2−1\frac{d}{dx}\csc^{-1}x = -\frac{1}{|x|\sqrt{x^2 - 1}}, −123-\frac{1}{2\sqrt 3} at −2-2
  • d) f′(x)=3∣3x∣9x2−1f'(x) = \frac{3}{|3x|\sqrt{9x^2 - 1}}, f′(−23)=32≈0.8660f'\left(-\frac{2}{3}\right) = \frac{\sqrt 3}{2} \approx 0.8660; the student finds −0.8660-0.8660, a negative slope on a rising graph
  • e) y=2π3+123(x+2)y = \frac{2\pi}{3} + \frac{1}{2\sqrt 3}(x + 2)

a) Differentiate sec⁡y=x\sec y = x with respect to xx, yy being a function of xx (chain rule, inner function yy): sec⁡ytan⁡y⋅y′=1\sec y\tan y \cdot y' = 1, so y′=1sec⁡ytan⁡yy' = \frac{1}{\sec y\tan y} wherever tan⁡y≠0\tan y \ne 0, that is for ∣x∣>1|x| > 1. Now sec⁡y=x\sec y = x, and tan⁡2y=sec⁡2y−1=x2−1\tan^2 y = \sec^2 y - 1 = x^2 - 1, so tan⁡y=±x2−1\tan y = \pm\sqrt{x^2 - 1}: the RANGE chooses. On the right branch, x>1x > 1, y∈(0,π2)y \in \left(0, \frac{\pi}{2}\right) and tan⁡y>0\tan y > 0: sec⁡ytan⁡y=xx2−1\sec y\tan y = x\sqrt{x^2 - 1}. On the left branch, x<−1x < -1, y∈(π2,π)y \in \left(\frac{\pi}{2}, \pi\right) and tan⁡y<0\tan y < 0: sec⁡ytan⁡y=x⋅(−x2−1)=−xx2−1\sec y\tan y = x \cdot \left(-\sqrt{x^2 - 1}\right) = -x\sqrt{x^2 - 1}. In both cases the product is ∣x∣x2−1|x|\sqrt{x^2 - 1}, positive, so ddxsec⁡−1x=1∣x∣x2−1\frac{d}{dx}\sec^{-1}x = \frac{1}{|x|\sqrt{x^2 - 1}}. At x=2x = 2: 123=36≈0.2887\frac{1}{2\sqrt 3} = \frac{\sqrt 3}{6} \approx 0.2887, and at x=−2x = -2 exactly the same value: the two branches rise, the derivative is positive on both.

b) With u=1xu = \frac{1}{x}, u′=−1x2u' = -\frac{1}{x^2}: ddxcos⁡−11x=−−1/x21−1/x2=1x21−1x2\frac{d}{dx}\cos^{-1}\frac{1}{x} = -\frac{-1/x^2}{\sqrt{1 - 1/x^2}} = \frac{1}{x^2\sqrt{1 - \frac{1}{x^2}}}. Bring the inside to one fraction: 1−1x2=x2−1x21 - \frac{1}{x^2} = \frac{x^2 - 1}{x^2}. Its square root is x2−1x2=x2−1∣x∣\frac{\sqrt{x^2 - 1}}{\sqrt{x^2}} = \frac{\sqrt{x^2 - 1}}{|x|}, because x2=∣x∣\sqrt{x^2} = |x| and NOT xx: for x=−2x = -2, 4=2\sqrt{4} = 2. Then 1x2⋅x2−1∣x∣=∣x∣x2x2−1=1∣x∣x2−1\frac{1}{x^2 \cdot \frac{\sqrt{x^2 - 1}}{|x|}} = \frac{|x|}{x^2\sqrt{x^2 - 1}} = \frac{1}{|x|\sqrt{x^2 - 1}}, since x2=∣x∣2x^2 = |x|^2. The same absolute value appears by a completely different road: it is not a convention of Thomas, it is forced by the algebra. Writing x2=x\sqrt{x^2} = x in this line is the most expensive slip of section 3.9, because it gives a formula that is wrong on a whole branch.

c) Differentiate the identities; the constant π2\frac{\pi}{2} has derivative 00. ddxcot⁡−1x=−11+x2\frac{d}{dx}\cot^{-1}x = -\frac{1}{1 + x^2}, which is −12-\frac{1}{2} at x=1x = 1. ddxcsc⁡−1x=−1∣x∣x2−1\frac{d}{dx}\csc^{-1}x = -\frac{1}{|x|\sqrt{x^2 - 1}} for ∣x∣>1|x| > 1, which is −123≈−0.2887-\frac{1}{2\sqrt 3} \approx -0.2887 at x=−2x = -2. The pattern of Thomas' table: each 'co' function has the derivative of its partner with a minus sign, because it is a constant minus the partner. Nothing new has to be memorized, and the signs are checked on the graphs: cot⁡−1\cot^{-1} decreases.

d) Chain rule, inner function u=3xu = 3x, u′=3u' = 3, u2=9x2u^2 = 9x^2: f′(x)=3∣3x∣9x2−1f'(x) = \frac{3}{|3x|\sqrt{9x^2 - 1}}. At x=−23x = -\frac{2}{3}: ∣3x∣=2|3x| = 2 and 9x2−1=4−1=39x^2 - 1 = 4 - 1 = 3, so f′(−23)=323=32≈0.8660f'\left(-\frac{2}{3}\right) = \frac{3}{2\sqrt 3} = \frac{\sqrt 3}{2} \approx 0.8660. The student's formula has 3x=−23x = -2 in the denominator and gives −32≈−0.8660-\frac{\sqrt 3}{2} \approx -0.8660. The figure refutes it without any computation: f(x)=sec⁡−1(3x)f(x) = \sec^{-1}(3x) is the left branch of the graph compressed horizontally, and a rising curve cannot have a negative slope. Keep the absolute value until the very last substitution, then replace ∣3x∣|3x| by −3x-3x when x<0x < 0.

e) Point: sec⁡−1(−2)=cos⁡−1(−12)=2π3\sec^{-1}(-2) = \cos^{-1}\left(-\frac{1}{2}\right) = \frac{2\pi}{3}. Slope from a): 1∣−2∣3=123≈0.2887\frac{1}{|-2|\sqrt 3} = \frac{1}{2\sqrt 3} \approx 0.2887. Tangent: y−2π3=123(x+2)y - \frac{2\pi}{3} = \frac{1}{2\sqrt 3}(x + 2), that is y=123x+2π3+13y = \frac{1}{2\sqrt 3}x + \frac{2\pi}{3} + \frac{1}{\sqrt 3}, with yy-intercept 2π3+13≈2.6717\frac{2\pi}{3} + \frac{1}{\sqrt 3} \approx 2.6717. The point is on the left branch of the figure, at height about 2.092.09, and the tangent rises gently, as it should.

Exercise 5: The chain rule through an inverse trigonometric function, and the square root of a square

In sin⁡−1u\sin^{-1}u, cos⁡−1u\cos^{-1}u or tan⁡−1u\tan^{-1}u, name the inner function uu first, write u′u' next to it, and only then apply the formula. When 1−u21 - u^2 is itself a square, its root is an ABSOLUTE VALUE: 1−cos⁡2x=sin⁡2x=∣sin⁡x∣\sqrt{1 - \cos^2 x} = \sqrt{\sin^2 x} = |\sin x|.

Part d) uses a differentiable function gg known only through a table: g(3)=12g(3) = \frac{1}{2}, g′(3)=6g'(3) = 6, g(π4)=5g\left(\frac{\pi}{4}\right) = 5, g′(π4)=2g'\left(\frac{\pi}{4}\right) = 2.

  • a) Let y=arctan⁡(e2x)y = \arctan(e^{2x}). Name the inner function, differentiate, and evaluate y′(0)y'(0).
  • b) Differentiate y=(arcsin⁡x)2y = (\arcsin x)^2 and z=arctan⁡(ln⁡x)z = \arctan(\ln x). Evaluate y′(12)y'\left(\frac{1}{2}\right) and z′(e)z'(e) to four decimals.
  • c) Let y=arcsin⁡(cos⁡x)y = \arcsin(\cos x). Show that y′=−1y' = -1 for 0<x<π0 < x < \pi, and find y′y' for −π<x<0-\pi < x < 0. Deduce a formula for yy on [0,π][0, \pi], reading the constant at x=π2x = \frac{\pi}{2}, and check it at x=π3x = \frac{\pi}{3}.
  • d) With the table of the introduction, find h′(3)h'(3) for h(x)=arcsin⁡(g(x))h(x) = \arcsin(g(x)) and k′(1)k'(1) for k(x)=g(arctan⁡x)k(x) = g(\arctan x).
  • e) Differentiate y=arctan⁡(sin⁡3x)y = \arctan(\sin 3x), naming its three layers, and evaluate y′(π9)y'\left(\frac{\pi}{9}\right).

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  • a) u=e2xu = e^{2x}; y′=2e2x1+e4xy' = \frac{2e^{2x}}{1 + e^{4x}}, y′(0)=1y'(0) = 1
  • b) y′=2arcsin⁡x1−x2y' = \frac{2\arcsin x}{\sqrt{1 - x^2}}, y′(12)=2π33≈1.2092y'\left(\frac{1}{2}\right) = \frac{2\pi}{3\sqrt 3} \approx 1.2092; z′=1x(1+ln⁡2x)z' = \frac{1}{x(1 + \ln^2 x)}, z′(e)=12e≈0.1839z'(e) = \frac{1}{2e} \approx 0.1839
  • c) y′=−sin⁡x∣sin⁡x∣y' = -\frac{\sin x}{|\sin x|}: −1-1 on (0,π)(0, \pi), +1+1 on (−π,0)(-\pi, 0); y=π2−xy = \frac{\pi}{2} - x on [0,π][0, \pi], and y(π3)=π6y\left(\frac{\pi}{3}\right) = \frac{\pi}{6}
  • d) h′(3)=63/2=43≈6.9282h'(3) = \frac{6}{\sqrt{3}/2} = 4\sqrt 3 \approx 6.9282; k′(1)=g′(π4)⋅12=1k'(1) = g'\left(\frac{\pi}{4}\right) \cdot \frac{1}{2} = 1
  • e) y′=3cos⁡3x1+sin⁡23xy' = \frac{3\cos 3x}{1 + \sin^2 3x}, y′(π9)=67≈0.8571y'\left(\frac{\pi}{9}\right) = \frac{6}{7} \approx 0.8571

a) Inner function u=e2xu = e^{2x}, whose derivative is u′=2e2xu' = 2e^{2x} (chain rule once more, inner 2x2x). Then u2=(e2x)2=e4xu^2 = (e^{2x})^2 = e^{4x} by the law (ea)b=eab(e^a)^b = e^{ab}; it is not e4x2e^{4x^2} and not e2x2e^{2x^2}. So y′=2e2x1+e4xy' = \frac{2e^{2x}}{1 + e^{4x}}, and y′(0)=21+1=1y'(0) = \frac{2}{1 + 1} = 1. The exponent law is the algebra of this line, and a wrong exponent gives the right value at 00 by coincidence and a wrong function everywhere else: at x=1x = 1 the correct slope is 2e21+e4≈0.266\frac{2e^2}{1 + e^4} \approx 0.266.

b) For y=(arcsin⁡x)2y = (\arcsin x)^2 the OUTER function is the square and the inner one is arcsin⁡x\arcsin x: y′=2arcsin⁡x⋅11−x2y' = 2\arcsin x \cdot \frac{1}{\sqrt{1 - x^2}}. Do not confuse it with arcsin⁡(x2)\arcsin(x^2), whose outer function is arcsin⁡\arcsin. At x=12x = \frac{1}{2}: 2⋅π632=2π33≈1.2092\frac{2 \cdot \frac{\pi}{6}}{\frac{\sqrt 3}{2}} = \frac{2\pi}{3\sqrt 3} \approx 1.2092. For z=arctan⁡(ln⁡x)z = \arctan(\ln x), x>0x > 0: inner function ln⁡x\ln x, derivative 1x\frac{1}{x}, so z′=1/x1+(ln⁡x)2=1x(1+ln⁡2x)z' = \frac{1/x}{1 + (\ln x)^2} = \frac{1}{x(1 + \ln^2 x)}. At x=ex = e, ln⁡e=1\ln e = 1: z′(e)=12e≈0.1839z'(e) = \frac{1}{2e} \approx 0.1839. Writing ln⁡2x\ln^2 x means (ln⁡x)2(\ln x)^2, not ln⁡(x2)=2ln⁡x\ln(x^2) = 2\ln x; at x=ex = e the confusion gives 13e\frac{1}{3e}.

c) Inner function u=cos⁡xu = \cos x, u′=−sin⁡xu' = -\sin x, 1−u2=1−cos⁡2x=sin⁡2x1 - u^2 = 1 - \cos^2 x = \sin^2 x. So y′=−sin⁡xsin⁡2x=−sin⁡x∣sin⁡x∣y' = \frac{-\sin x}{\sqrt{\sin^2 x}} = -\frac{\sin x}{|\sin x|}. On (0,π)(0, \pi), sin⁡x>0\sin x > 0, ∣sin⁡x∣=sin⁡x|\sin x| = \sin x and y′=−1y' = -1. On (−π,0)(-\pi, 0), sin⁡x<0\sin x < 0, ∣sin⁡x∣=−sin⁡x|\sin x| = -\sin x and y′=+1y' = +1. The student who writes sin⁡2x=sin⁡x\sqrt{\sin^2 x} = \sin x finds −1-1 everywhere and misses half of the graph. On the interval (0,π)(0, \pi) the function y+xy + x has derivative 00, so it is constant there (the zero-derivative fact, used as a tool). Read it at x=π2x = \frac{\pi}{2}: arcsin⁡(cos⁡π2)+π2=arcsin⁡0+π2=π2\arcsin(\cos\frac{\pi}{2}) + \frac{\pi}{2} = \arcsin 0 + \frac{\pi}{2} = \frac{\pi}{2}. Hence y=π2−xy = \frac{\pi}{2} - x on (0,π)(0, \pi), and also at the endpoints, where arcsin⁡1=π2\arcsin 1 = \frac{\pi}{2} and arcsin⁡(−1)=−π2\arcsin(-1) = -\frac{\pi}{2}. Check at π3\frac{\pi}{3}: arcsin⁡12=π6=π2−π3\arcsin\frac{1}{2} = \frac{\pi}{6} = \frac{\pi}{2} - \frac{\pi}{3}.

d) Chain rule on hh, inner function gg: h′(x)=g′(x)1−g(x)2h'(x) = \frac{g'(x)}{\sqrt{1 - g(x)^2}}. At x=3x = 3: 1−14=32\sqrt{1 - \frac{1}{4}} = \frac{\sqrt 3}{2}, so h′(3)=63/2=123=43≈6.9282h'(3) = \frac{6}{\sqrt 3/2} = \frac{12}{\sqrt 3} = 4\sqrt 3 \approx 6.9282. Chain rule on kk, inner function arctan⁡x\arctan x, outer function gg: k′(x)=g′(arctan⁡x)⋅11+x2k'(x) = g'(\arctan x) \cdot \frac{1}{1 + x^2}. At x=1x = 1, arctan⁡1=π4\arctan 1 = \frac{\pi}{4}, so k′(1)=g′(π4)⋅12=2⋅12=1k'(1) = g'\left(\frac{\pi}{4}\right) \cdot \frac{1}{2} = 2 \cdot \frac{1}{2} = 1. The table is built with two traps: g(π4)=5g\left(\frac{\pi}{4}\right) = 5 is there to be confused with g′(π4)g'\left(\frac{\pi}{4}\right), which gives 2.52.5; and g′(1)g'(1) is not in the table because the outer derivative is evaluated at the INNER value arctan⁡1\arctan 1, not at 11.

e) Three layers, from the outside: arctan⁡\arctan, then sin⁡\sin, then 3x3x. Differentiate each at the layer below it: y′=11+sin⁡23x⋅cos⁡3x⋅3=3cos⁡3x1+sin⁡23xy' = \frac{1}{1 + \sin^2 3x} \cdot \cos 3x \cdot 3 = \frac{3\cos 3x}{1 + \sin^2 3x}. At x=π9x = \frac{\pi}{9}, 3x=π33x = \frac{\pi}{3}: cos⁡π3=12\cos\frac{\pi}{3} = \frac{1}{2} and sin⁡2π3=34\sin^2\frac{\pi}{3} = \frac{3}{4}, so y′=3/27/4=67≈0.8571y' = \frac{3/2}{7/4} = \frac{6}{7} \approx 0.8571. The factor 33 of the innermost layer is the one that disappears on exams; the check is to count the layers, three, and the factors in the answer, three.

Part B: problems and reasoning (/50)

Exercise 6: Two functions that agree on one side only: arcsec from the arctan key

Most scientific calculators, including the models approved for the course, have no sec⁡−1\sec^{-1} key. This exercise builds a formula that computes sec⁡−1x\sec^{-1}x with the tan⁡−1\tan^{-1} key, and proves it with the tool of the chapter: if F′(x)=0F'(x) = 0 at every point of an INTERVAL, then FF is constant on that interval (admitted), and the constant is read at one convenient point OF THAT INTERVAL.

Let g(x)=tan⁡−1x2−1g(x) = \tan^{-1}\sqrt{x^2 - 1} and h(x)=sec⁡−1xh(x) = \sec^{-1}x, both defined for ∣x∣≥1|x| \ge 1. Recall from section 3.9 that h′(x)=1∣x∣x2−1h'(x) = \frac{1}{|x|\sqrt{x^2 - 1}} for ∣x∣>1|x| > 1. The figure shows hh in blue and gg in dashed orange: they coincide on the right and separate on the left.

-6-5-4-3-2-1123456-0.50.511.522.533.54y = h(x)y = g(x)g = h
  • a) Show that gg is even and that hh is not. Compute g(2)g(2), g(−2)g(-2), h(2)h(2) and h(−2)h(-2) exactly.
  • b) Differentiate gg for ∣x∣>1|x| > 1 and show that g′(x)=1xx2−1g'(x) = \frac{1}{x\sqrt{x^2 - 1}}. Compare g′g' with h′h' on each side, and evaluate both at x=−2x = -2.
  • c) Show that g−hg - h is constant on (1,∞)(1, \infty) and find the constant.
  • d) Show that g+hg + h is constant on (−∞,−1)(-\infty, -1) and find the constant. Why is it wrong to read this constant at x=2x = 2?
  • e) Conclude: write sec⁡−1x\sec^{-1}x in terms of tan⁡−1\tan^{-1} for x≥1x \ge 1 and for x≤−1x \le -1 (check the endpoints ±1\pm 1 directly), then compute sec⁡−1(−3)\sec^{-1}(-3) to four decimals with the tan⁡−1\tan^{-1} key, and check it with cos⁡−1(−13)\cos^{-1}\left(-\frac{1}{3}\right).

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  • a) g(−x)=g(x)g(-x) = g(x); h(2)=π3≠h(−2)=2π3h(2) = \frac{\pi}{3} \ne h(-2) = \frac{2\pi}{3}; g(2)=g(−2)=π3g(2) = g(-2) = \frac{\pi}{3}
  • b) g′(x)=1xx2−1g'(x) = \frac{1}{x\sqrt{x^2 - 1}}: g′=h′g' = h' for x>1x > 1, g′=−h′g' = -h' for x<−1x < -1; g′(−2)=−123g'(-2) = -\frac{1}{2\sqrt 3}, h′(−2)=123h'(-2) = \frac{1}{2\sqrt 3}
  • c) (g−h)′=0(g - h)' = 0 on (1,∞)(1, \infty), constant g(2)−h(2)=0g(2) - h(2) = 0
  • d) (g+h)′=0(g + h)' = 0 on (−∞,−1)(-\infty, -1), constant g(−2)+h(−2)=πg(-2) + h(-2) = \pi; x=2x = 2 is not in that interval
  • e) sec⁡−1x=tan⁡−1x2−1\sec^{-1}x = \tan^{-1}\sqrt{x^2 - 1} for x≥1x \ge 1, π−tan⁡−1x2−1\pi - \tan^{-1}\sqrt{x^2 - 1} for x≤−1x \le -1; sec⁡−1(−3)≈1.9106\sec^{-1}(-3) \approx 1.9106

a) g(−x)=tan⁡−1(−x)2−1=tan⁡−1x2−1=g(x)g(-x) = \tan^{-1}\sqrt{(-x)^2 - 1} = \tan^{-1}\sqrt{x^2 - 1} = g(x): gg only sees x2x^2, so it is even and its graph is symmetric in the yy-axis, as the orange curve of the figure is. hh is not even: h(2)=cos⁡−112=π3h(2) = \cos^{-1}\frac{1}{2} = \frac{\pi}{3} but h(−2)=cos⁡−1(−12)=2π3h(-2) = \cos^{-1}\left(-\frac{1}{2}\right) = \frac{2\pi}{3}. And g(2)=g(−2)=tan⁡−13=π3g(2) = g(-2) = \tan^{-1}\sqrt 3 = \frac{\pi}{3}. The values already say it: g=hg = h at x=2x = 2, but not at x=−2x = -2, where g(−2)+h(−2)=πg(-2) + h(-2) = \pi.

b) Inner function u=x2−1=(x2−1)1/2u = \sqrt{x^2 - 1} = (x^2 - 1)^{1/2}, u′=12(x2−1)−1/2⋅2x=xx2−1u' = \frac{1}{2}(x^2 - 1)^{-1/2} \cdot 2x = \frac{x}{\sqrt{x^2 - 1}}. Now the gesture of the chapter: 1+u2=1+(x2−1)=x21 + u^2 = 1 + (x^2 - 1) = x^2, since squaring a square root of a nonnegative number gives the number back. So g′(x)=x/x2−1x2=1xx2−1g'(x) = \frac{x/\sqrt{x^2 - 1}}{x^2} = \frac{1}{x\sqrt{x^2 - 1}}, with xx and not ∣x∣|x|: here no root of a square was taken, and the sign of xx stays. For x>1x > 1, x=∣x∣x = |x| and g′(x)=h′(x)g'(x) = h'(x). For x<−1x < -1, x=−∣x∣x = -|x| and g′(x)=−h′(x)g'(x) = -h'(x). At x=−2x = -2: g′(−2)=1−23≈−0.2887g'(-2) = \frac{1}{-2\sqrt 3} \approx -0.2887 and h′(−2)=123≈0.2887h'(-2) = \frac{1}{2\sqrt 3} \approx 0.2887. The figure agrees: on the left, the orange curve goes down while the blue one goes up.

c) On (1,∞)(1, \infty), (g−h)′(x)=g′(x)−h′(x)=0(g - h)'(x) = g'(x) - h'(x) = 0 at every point, and (1,∞)(1, \infty) is an interval, so g−hg - h is constant there. Read the constant at a point of THIS interval, x=2x = 2: g(2)−h(2)=π3−π3=0g(2) - h(2) = \frac{\pi}{3} - \frac{\pi}{3} = 0. So g(x)=h(x)g(x) = h(x) for every x>1x > 1, which is the coincidence of the two curves on the right of the figure.

d) On (−∞,−1)(-\infty, -1), (g+h)′(x)=g′(x)+h′(x)=−h′(x)+h′(x)=0(g + h)'(x) = g'(x) + h'(x) = -h'(x) + h'(x) = 0, so g+hg + h is constant on this interval. Read it at x=−2x = -2: g(−2)+h(−2)=π3+2π3=πg(-2) + h(-2) = \frac{\pi}{3} + \frac{2\pi}{3} = \pi. So h(x)=π−g(x)h(x) = \pi - g(x) for x<−1x < -1: the left branches of the figure are mirror images in the dashed line y=π2y = \frac{\pi}{2}. Reading the constant at x=2x = 2 would give g(2)+h(2)=2π3g(2) + h(2) = \frac{2\pi}{3}, a wrong answer: the fact 'zero derivative gives a constant' holds on ONE interval, and x=2x = 2 belongs to the other one. The domain ∣x∣>1|x| > 1 is made of two separate intervals, and each gets its own constant, read at its own point.

e) Collecting c) and d): sec⁡−1x=tan⁡−1x2−1\sec^{-1}x = \tan^{-1}\sqrt{x^2 - 1} for x>1x > 1 and sec⁡−1x=π−tan⁡−1x2−1\sec^{-1}x = \pi - \tan^{-1}\sqrt{x^2 - 1} for x<−1x < -1. The endpoints are checked directly: sec⁡−11=0=tan⁡−10\sec^{-1}1 = 0 = \tan^{-1}0 and sec⁡−1(−1)=π=π−tan⁡−10\sec^{-1}(-1) = \pi = \pi - \tan^{-1}0. With the calculator in radians: sec⁡−1(−3)=π−tan⁡−18≈3.141593−1.230959=1.910633\sec^{-1}(-3) = \pi - \tan^{-1}\sqrt 8 \approx 3.141593 - 1.230959 = 1.910633, that is 1.91061.9106. Check: cos⁡−1(−13)≈1.9106\cos^{-1}\left(-\frac{1}{3}\right) \approx 1.9106, the same. The tempting shortcut tan⁡−18≈1.2310\tan^{-1}\sqrt 8 \approx 1.2310 is the formula of the RIGHT branch used on the left; it gives an angle below π2\frac{\pi}{2}, impossible for sec⁡−1\sec^{-1} of a negative number.

Exercise 7: Horizontal tangents and prescribed slopes: one denominator, then factor

Let f(x)=sin⁡−1x−21−x2f(x) = \sin^{-1}x - 2\sqrt{1 - x^2} on [−1,1][-1, 1], whose graph is in the figure, and g(x)=4tan⁡−1x−x2g(x) = 4\tan^{-1}x - x^2 for every real xx.

A horizontal tangent is a point where the derivative is 00; a tangent parallel to a line y=mx+by = mx + b is a point where the derivative is mm. In both cases the equation is solved on ONE fraction: put the derivative over a common denominator, then factor the numerator. Exact answers first, then decimals.

-1.5-1-0.50.511.5-2.5-2-1.5-1-0.50.511.52y = f(x)
  • a) Show that f′(x)=1+2x1−x2f'(x) = \frac{1 + 2x}{\sqrt{1 - x^2}} for −1<x<1-1 < x < 1, and find the point of the graph of ff with a horizontal tangent, exactly and to four decimals.
  • b) What does f′(x)f'(x) do as x→1−x \to 1^- and as x→−1+x \to -1^+? Describe the tangent to the graph at each endpoint.
  • c) Find every point of the graph of ff where the tangent has slope 22. Squaring is allowed, but every candidate must be checked.
  • d) Show that g′(x)=4−2x−2x31+x2g'(x) = \frac{4 - 2x - 2x^3}{1 + x^2} and that the graph of gg has exactly one horizontal tangent. Give the point.
  • e) Find every point of the graph of gg where the tangent is parallel to the line y=4xy = 4x.

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  • a) Horizontal tangent at (−12,−π6−3)≈(−0.5,−2.2556)\left(-\frac{1}{2}, -\frac{\pi}{6} - \sqrt 3\right) \approx (-0.5, -2.2556)
  • b) f′(x)→+∞f'(x) \to +\infty as x→1−x \to 1^- and −∞-\infty as x→−1+x \to -1^+: vertical tangents at both endpoints
  • c) One point, x=−1+74≈0.4114x = \frac{-1 + \sqrt 7}{4} \approx 0.4114; x=−1−74x = \frac{-1 - \sqrt 7}{4} rejected
  • d) x3+x−2=(x−1)(x2+x+2)x^3 + x - 2 = (x - 1)(x^2 + x + 2): only x=1x = 1, the point (1,π−1)(1, \pi - 1)
  • e) −2x(x+1)2=0-2x(x + 1)^2 = 0: at (0,0)(0, 0) and (−1,−π−1)(-1, -\pi - 1)

a) Differentiate term by term: ddxsin⁡−1x=11−x2\frac{d}{dx}\sin^{-1}x = \frac{1}{\sqrt{1 - x^2}}, and by the chain rule ddx(−21−x2)=−2⋅−2x21−x2=2x1−x2\frac{d}{dx}\left(-2\sqrt{1 - x^2}\right) = -2 \cdot \frac{-2x}{2\sqrt{1 - x^2}} = \frac{2x}{\sqrt{1 - x^2}}. The two terms have the SAME denominator, so f′(x)=1+2x1−x2f'(x) = \frac{1 + 2x}{\sqrt{1 - x^2}}. A fraction is 00 when its numerator is 00 and its denominator is not: 1+2x=01 + 2x = 0 gives x=−12x = -\frac{1}{2}, where 1−14=32≠0\sqrt{1 - \frac{1}{4}} = \frac{\sqrt 3}{2} \ne 0. Then f(−12)=−π6−2⋅32=−π6−3≈−2.2556f\left(-\frac{1}{2}\right) = -\frac{\pi}{6} - 2 \cdot \frac{\sqrt 3}{2} = -\frac{\pi}{6} - \sqrt 3 \approx -2.2556. The figure agrees: the lowest point of the curve is near (−0.5,−2.26)(-0.5, -2.26). Leaving f′f' as two fractions and setting each to 00 separately is the mistake that finds nothing.

b) As x→1−x \to 1^-, the numerator 1+2x→31 + 2x \to 3 and the denominator 1−x2→0+\sqrt{1 - x^2} \to 0^+, so f′(x)→+∞f'(x) \to +\infty. As x→−1+x \to -1^+, the numerator tends to −1-1 and the denominator to 0+0^+, so f′(x)→−∞f'(x) \to -\infty. The slopes grow without bound: the graph arrives VERTICALLY at both endpoints (1,π2)\left(1, \frac{\pi}{2}\right) and (−1,−π2)\left(-1, -\frac{\pi}{2}\right), which is what the figure shows. Numerically, f′(0.99)≈21.1f'(0.99) \approx 21.1 and f′(−0.99)≈−6.9f'(-0.99) \approx -6.9.

c) Solve 1+2x1−x2=2\frac{1 + 2x}{\sqrt{1 - x^2}} = 2, that is 1+2x=21−x21 + 2x = 2\sqrt{1 - x^2}. The right side is positive, so any solution must have 1+2x>01 + 2x > 0: note it BEFORE squaring. Squaring: 1+4x+4x2=4−4x21 + 4x + 4x^2 = 4 - 4x^2, so 8x2+4x−3=08x^2 + 4x - 3 = 0 and x=−4±16+9616=−1±74x = \frac{-4 \pm \sqrt{16 + 96}}{16} = \frac{-1 \pm \sqrt 7}{4}. The candidate −1+74≈0.4114\frac{-1 + \sqrt 7}{4} \approx 0.4114 has 1+2x≈1.82>01 + 2x \approx 1.82 > 0: kept, and f′(0.4114)≈2.000f'(0.4114) \approx 2.000. The candidate −1−74≈−0.9114\frac{-1 - \sqrt 7}{4} \approx -0.9114 has 1+2x≈−0.82<01 + 2x \approx -0.82 < 0: at that point f′=−2f' = -2, not 22. Squaring merged the equations f′=2f' = 2 and f′=−2f' = -2; the check separates them again. One point only.

d) g′(x)=41+x2−2x=4−2x(1+x2)1+x2=4−2x−2x31+x2g'(x) = \frac{4}{1 + x^2} - 2x = \frac{4 - 2x(1 + x^2)}{1 + x^2} = \frac{4 - 2x - 2x^3}{1 + x^2}, over the common denominator 1+x21 + x^2, never 00. Horizontal tangent: 4−2x−2x3=04 - 2x - 2x^3 = 0, that is x3+x−2=0x^3 + x - 2 = 0 after dividing by −2-2. x=1x = 1 is a root (1+1−2=01 + 1 - 2 = 0), so factor: x3+x−2=(x−1)(x2+x+2)x^3 + x - 2 = (x - 1)(x^2 + x + 2), and x2+x+2x^2 + x + 2 has discriminant 1−8<01 - 8 < 0, no real root. Exactly one horizontal tangent, at x=1x = 1, where g(1)=4⋅π4−1=π−1≈2.1416g(1) = 4 \cdot \frac{\pi}{4} - 1 = \pi - 1 \approx 2.1416.

e) Parallel to y=4xy = 4x means g′(x)=4g'(x) = 4: 4−2x−2x31+x2=4\frac{4 - 2x - 2x^3}{1 + x^2} = 4, so 4−2x−2x3=4+4x24 - 2x - 2x^3 = 4 + 4x^2, that is −2x3−4x2−2x=0-2x^3 - 4x^2 - 2x = 0. Factor −2x-2x first, the common factor that a division by xx would lose: −2x(x2+2x+1)=−2x(x+1)2=0-2x(x^2 + 2x + 1) = -2x(x + 1)^2 = 0. Two points: x=0x = 0, with g(0)=0g(0) = 0, and x=−1x = -1, with g(−1)=4(−π4)−1=−π−1≈−4.1416g(-1) = 4\left(-\frac{\pi}{4}\right) - 1 = -\pi - 1 \approx -4.1416. Check: g′(−1)=42+2=4g'(-1) = \frac{4}{2} + 2 = 4. Dividing both sides by xx at the start keeps only x=−1x = -1 and loses the tangent y=4xy = 4x at the origin itself.

Exercise 8: Five statements to correct

Each statement below was written by a student on a MATH 203 assignment, and each is false. Say what is wrong, give a counterexample or the correct computation, and write the correct statement.

  • a) sin⁡−1(sin⁡5π6)=5π6\sin^{-1}\left(\sin\frac{5\pi}{6}\right) = \frac{5\pi}{6}, since sin⁡−1\sin^{-1} undoes sin⁡\sin.
  • b) ddxsec⁡−1x=1xx2−1\frac{d}{dx}\sec^{-1}x = \frac{1}{x\sqrt{x^2 - 1}} for every xx with ∣x∣>1|x| > 1.
  • c) tan⁡−1x=sin⁡−1xcos⁡−1x\tan^{-1}x = \frac{\sin^{-1}x}{\cos^{-1}x} for −1<x<1-1 < x < 1, because tan⁡=sin⁡cos⁡\tan = \frac{\sin}{\cos}.
  • d) ddxtan⁡−11x=11+1x2=x2x2+1\frac{d}{dx}\tan^{-1}\frac{1}{x} = \frac{1}{1 + \frac{1}{x^2}} = \frac{x^2}{x^2 + 1}.
  • e) The domain of sin⁡−1(3x)\sin^{-1}(3x) is [−1,1][-1, 1], and ddxsin⁡−1(3x)=31−3x2\frac{d}{dx}\sin^{-1}(3x) = \frac{3}{\sqrt{1 - 3x^2}}.

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  • a) False: sin⁡5π6=12\sin\frac{5\pi}{6} = \frac{1}{2} and sin⁡−112=π6\sin^{-1}\frac{1}{2} = \frac{\pi}{6}
  • b) False for x<−1x < -1: the derivative is 1∣x∣x2−1\frac{1}{|x|\sqrt{x^2 - 1}}, equal to +123+\frac{1}{2\sqrt 3} at x=−2x = -2
  • c) False: at x=12x = \frac{1}{2} the right side is 12\frac{1}{2}, while tan⁡−112≈0.4636\tan^{-1}\frac{1}{2} \approx 0.4636
  • d) False: the chain factor −1x2-\frac{1}{x^2} is missing; ddxtan⁡−11x=−11+x2\frac{d}{dx}\tan^{-1}\frac{1}{x} = -\frac{1}{1 + x^2}
  • e) False twice: domain [−13,13]\left[-\frac{1}{3}, \frac{1}{3}\right], derivative 31−9x2\frac{3}{\sqrt{1 - 9x^2}}

a) sin⁡−1\sin^{-1} undoes sin⁡\sin only on [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right], and 5π6\frac{5\pi}{6} is not in that interval. Compute from the inside: sin⁡5π6=12\sin\frac{5\pi}{6} = \frac{1}{2}, and the angle of the range with sine 12\frac{1}{2} is π6\frac{\pi}{6}. So sin⁡−1(sin⁡5π6)=π6\sin^{-1}\left(\sin\frac{5\pi}{6}\right) = \frac{\pi}{6}. Correct statement: sin⁡−1(sin⁡x)=x\sin^{-1}(\sin x) = x for −π2≤x≤π2-\frac{\pi}{2} \le x \le \frac{\pi}{2} only, while sin⁡(sin⁡−1x)=x\sin(\sin^{-1}x) = x for every xx of [−1,1][-1, 1]. The student's answer fails the one-second test: 5π6>π2\frac{5\pi}{6} > \frac{\pi}{2} is not a possible value of sin⁡−1\sin^{-1}.

b) The formula is right for x>1x > 1 and wrong for x<−1x < -1. At x=−2x = -2 it gives 1−23<0\frac{1}{-2\sqrt 3} < 0, but sec⁡−1\sec^{-1} rises on its left branch, so its slope there is positive. The implicit derivation gives 1sec⁡ytan⁡y\frac{1}{\sec y\tan y} with tan⁡y<0\tan y < 0 on the left branch, and sec⁡ytan⁡y=x⋅(−x2−1)=∣x∣x2−1\sec y\tan y = x \cdot \left(-\sqrt{x^2 - 1}\right) = |x|\sqrt{x^2 - 1}. Correct statement: ddxsec⁡−1x=1∣x∣x2−1\frac{d}{dx}\sec^{-1}x = \frac{1}{|x|\sqrt{x^2 - 1}} for ∣x∣>1|x| > 1, which is 123≈0.2887\frac{1}{2\sqrt 3} \approx 0.2887 at x=−2x = -2.

c) The identity tan⁡θ=sin⁡θcos⁡θ\tan\theta = \frac{\sin\theta}{\cos\theta} is about ONE angle θ\theta. The three inverse functions of the statement return three DIFFERENT angles for the same xx, so nothing allows dividing them. Counterexample at x=12x = \frac{1}{2}: sin⁡−1(1/2)cos⁡−1(1/2)=π/6π/3=12\frac{\sin^{-1}(1/2)}{\cos^{-1}(1/2)} = \frac{\pi/6}{\pi/3} = \frac{1}{2}, while tan⁡−112≈0.4636\tan^{-1}\frac{1}{2} \approx 0.4636. At x=1x = 1 it is worse: cos⁡−11=0\cos^{-1}1 = 0, a division by 00. What IS true, by the triangle of the angle θ=sin⁡−1x\theta = \sin^{-1}x: tan⁡(sin⁡−1x)=x1−x2\tan(\sin^{-1}x) = \frac{x}{\sqrt{1 - x^2}} for −1<x<1-1 < x < 1, a trigonometric function of ONE angle.

d) The formula 11+u2\frac{1}{1 + u^2} was applied with u=1xu = \frac{1}{x}, but the factor u′=−1x2u' = -\frac{1}{x^2} of the chain rule was dropped. Correctly: ddxtan⁡−11x=−1/x21+1/x2\frac{d}{dx}\tan^{-1}\frac{1}{x} = \frac{-1/x^2}{1 + 1/x^2}, and multiplying top and bottom by x2x^2 (the complex fraction gesture) gives −1x2+1-\frac{1}{x^2 + 1} for x≠0x \ne 0. At x=1x = 1 the student finds +12+\frac{1}{2} and the true value is −12-\frac{1}{2}: a sign error that a single look at tan⁡−11x\tan^{-1}\frac{1}{x} reveals, since 1x\frac{1}{x} decreases on (0,∞)(0, \infty) and so does its arctangent.

e) Two errors. The domain: sin⁡−1u\sin^{-1}u needs −1≤u≤1-1 \le u \le 1, here −1≤3x≤1-1 \le 3x \le 1, so −13≤x≤13-\frac{1}{3} \le x \le \frac{1}{3}. The derivative: u2=(3x)2=9x2u^2 = (3x)^2 = 9x^2, the square applies to the 33 as well, so ddxsin⁡−1(3x)=31−9x2\frac{d}{dx}\sin^{-1}(3x) = \frac{3}{\sqrt{1 - 9x^2}} for ∣x∣<13|x| < \frac{1}{3}. At x=0.3x = 0.3 the student gets 30.73≈3.511\frac{3}{\sqrt{0.73}} \approx 3.511 and the true value is 30.19≈6.8825\frac{3}{\sqrt{0.19}} \approx 6.8825. The student's formula is even defined at x=0.5x = 0.5, a point where the function itself does not exist: a derivative can never have a larger domain than its function.

Exercise 9: The angle under which a painting is seen, and its rate with distance

In a gallery, a painting 22 m tall hangs on a wall with its lower edge 11 m above the eye level of a visitor and its upper edge 33 m above. The visitor stands at a horizontal distance xx metres from the wall, x>0x > 0. The angle θ\theta under which the painting is seen is the angle at the eye EE between the line of sight to the upper edge and the line of sight to the lower edge, as in the figure.

Scientific calculator allowed; angles in radians unless degrees are asked. For b), recall tan⁡(A−B)=tan⁡A−tan⁡B1+tan⁡Atan⁡B\tan(A - B) = \frac{\tan A - \tan B}{1 + \tan A\tan B}. This exercise studies θ\theta as a function of xx and its rate dθdx\frac{d\theta}{dx}; where the angle is LARGEST is an optimization question for section 4.6, not asked here.

θEx1 mpainting, 2 mwall
  • a) Explain why θ(x)=tan⁡−13x−tan⁡−11x\theta(x) = \tan^{-1}\frac{3}{x} - \tan^{-1}\frac{1}{x}. Compute θ(2)\theta(2) in radians, to four decimals, and in degrees, to two decimals.
  • b) Show that tan⁡θ=2xx2+3\tan\theta = \frac{2x}{x^2 + 3}, and deduce that θ(x)=tan⁡−12xx2+3\theta(x) = \tan^{-1}\frac{2x}{x^2 + 3}. Why is it legitimate to apply tan⁡−1\tan^{-1} here? Give tan⁡θ\tan\theta at x=2x = 2.
  • c) Show that ddxtan⁡−1ax=−ax2+a2\frac{d}{dx}\tan^{-1}\frac{a}{x} = -\frac{a}{x^2 + a^2} for a constant a>0a > 0, then write θ′(x)\theta'(x) as a single fraction and evaluate θ′(1)\theta'(1) and θ′(2)\theta'(2).
  • d) Give the units of θ′(1)\theta'(1) and its meaning in one sentence, then convert it to degrees per metre. At x=2x = 2, does the angle grow or shrink when the visitor steps back a little?
  • e) Differentiate the one-arctangent form of b) directly, and show that the two routes agree by factoring x4+10x2+9x^4 + 10x^2 + 9. Then evaluate θ′(3)\theta'(3).

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  • a) θ=β−α\theta = \beta - \alpha with tan⁡β=3x\tan\beta = \frac{3}{x}, tan⁡α=1x\tan\alpha = \frac{1}{x}; θ(2)≈0.5191\theta(2) \approx 0.5191 rad ≈29.74°\approx 29.74°
  • b) tan⁡θ=2/x1+3/x2=2xx2+3\tan\theta = \frac{2/x}{1 + 3/x^2} = \frac{2x}{x^2 + 3}, and 0<θ<π20 < \theta < \frac{\pi}{2}; tan⁡θ(2)=47\tan\theta(2) = \frac{4}{7}
  • c) θ′(x)=1x2+1−3x2+9=2(3−x2)(x2+1)(x2+9)\theta'(x) = \frac{1}{x^2 + 1} - \frac{3}{x^2 + 9} = \frac{2(3 - x^2)}{(x^2 + 1)(x^2 + 9)}; θ′(1)=0.2\theta'(1) = 0.2, θ′(2)=−265≈−0.0308\theta'(2) = -\frac{2}{65} \approx -0.0308
  • d) Radians per metre: at 11 m, the angle grows by about 0.20.2 rad per metre stepped back, ≈11.46°\approx 11.46° per metre; at 22 m it shrinks
  • e) x4+10x2+9=(x2+1)(x2+9)x^4 + 10x^2 + 9 = (x^2 + 1)(x^2 + 9); θ′(3)=−115≈−0.0667\theta'(3) = -\frac{1}{15} \approx -0.0667

a) Let β\beta be the angle between the horizontal line of sight and the line to the upper edge, and α\alpha the angle to the lower edge. In the right triangles of the figure, the side opposite β\beta is 33 and the adjacent side is xx, so tan⁡β=3x\tan\beta = \frac{3}{x}; likewise tan⁡α=1x\tan\alpha = \frac{1}{x}. Both angles are in (0,π2)\left(0, \frac{\pi}{2}\right), the range of tan⁡−1\tan^{-1}, so β=tan⁡−13x\beta = \tan^{-1}\frac{3}{x} and α=tan⁡−11x\alpha = \tan^{-1}\frac{1}{x}, and θ=β−α\theta = \beta - \alpha. At x=2x = 2: tan⁡−11.5−tan⁡−10.5≈0.982794−0.463648=0.519146\tan^{-1}1.5 - \tan^{-1}0.5 \approx 0.982794 - 0.463648 = 0.519146, so θ(2)≈0.5191\theta(2) \approx 0.5191 rad. In degrees: 0.519146⋅180π≈29.74°0.519146 \cdot \frac{180}{\pi} \approx 29.74°. Keep the six-digit values until the end: subtracting two rounded angles loses a digit.

b) With tan⁡β=3x\tan\beta = \frac{3}{x} and tan⁡α=1x\tan\alpha = \frac{1}{x}: tan⁡θ=3x−1x1+3x2\tan\theta = \frac{\frac{3}{x} - \frac{1}{x}}{1 + \frac{3}{x^2}}. This is a complex fraction, the gesture that costs marks in MATH 203: multiply its top and bottom by x2x^2, the common denominator of every small fraction inside it. The top becomes 3x−x=2x3x - x = 2x and the bottom x2+3x^2 + 3, so tan⁡θ=2xx2+3\tan\theta = \frac{2x}{x^2 + 3}. Since 0<α<β<π20 < \alpha < \beta < \frac{\pi}{2}, the angle θ=β−α\theta = \beta - \alpha lies in (0,π2)\left(0, \frac{\pi}{2}\right), inside the range of tan⁡−1\tan^{-1}; so applying tan⁡−1\tan^{-1} gives back θ\theta itself: θ=tan⁡−12xx2+3\theta = \tan^{-1}\frac{2x}{x^2 + 3}. Without that check the step could be false, exactly as tan⁡−1(tan⁡3π4)≠3π4\tan^{-1}\left(\tan\frac{3\pi}{4}\right) \ne \frac{3\pi}{4}. At x=2x = 2: tan⁡θ=47≈0.5714\tan\theta = \frac{4}{7} \approx 0.5714, and tan⁡−147≈0.5191\tan^{-1}\frac{4}{7} \approx 0.5191, as in a).

c) Inner function u=ax=ax−1u = \frac{a}{x} = ax^{-1}, u′=−ax2u' = -\frac{a}{x^2}. So ddxtan⁡−1ax=−a/x21+a2/x2\frac{d}{dx}\tan^{-1}\frac{a}{x} = \frac{-a/x^2}{1 + a^2/x^2}; multiply top and bottom by x2x^2: −ax2+a2-\frac{a}{x^2 + a^2}. With a=3a = 3 and a=1a = 1: θ′(x)=−3x2+9+1x2+1\theta'(x) = -\frac{3}{x^2 + 9} + \frac{1}{x^2 + 1}. One fraction, over (x2+1)(x2+9)(x^2 + 1)(x^2 + 9): the numerator is −3(x2+1)+(x2+9)=6−2x2-3(x^2 + 1) + (x^2 + 9) = 6 - 2x^2, so θ′(x)=2(3−x2)(x2+1)(x2+9)\theta'(x) = \frac{2(3 - x^2)}{(x^2 + 1)(x^2 + 9)}. Watch the distribution of −3-3 over x2+1x^2 + 1: writing −3x2+1-3x^2 + 1 gives 10−2x210 - 2x^2 and a wrong function. θ′(1)=42⋅10=0.2\theta'(1) = \frac{4}{2 \cdot 10} = 0.2 and θ′(2)=−25⋅13=−265≈−0.0308\theta'(2) = \frac{-2}{5 \cdot 13} = -\frac{2}{65} \approx -0.0308.

d) θ\theta is in radians and xx in metres, so θ′(1)\theta'(1) is in radians per metre. Meaning: when the visitor stands 11 m from the wall, the viewing angle increases at the rate of 0.20.2 rad for each metre of stepping back, that is, about 0.020.02 rad for a step of 1010 cm. In degrees: 0.2⋅180π≈11.46°0.2 \cdot \frac{180}{\pi} \approx 11.46° per metre. At x=2x = 2, θ′(2)≈−0.0308<0\theta'(2) \approx -0.0308 < 0: stepping back a little makes the painting look slightly SMALLER. So the angle grows when one steps back from 11 m and shrinks when one steps back from 22 m; where exactly the change of behaviour happens, and why the angle is largest there, belongs to the optimization chapter.

e) With u=2xx2+3u = \frac{2x}{x^2 + 3}, the quotient rule gives u′=2(x2+3)−2x⋅2x(x2+3)2=6−2x2(x2+3)2u' = \frac{2(x^2 + 3) - 2x \cdot 2x}{(x^2 + 3)^2} = \frac{6 - 2x^2}{(x^2 + 3)^2}, and 1+u2=(x2+3)2+4x2(x2+3)2=x4+10x2+9(x2+3)21 + u^2 = \frac{(x^2 + 3)^2 + 4x^2}{(x^2 + 3)^2} = \frac{x^4 + 10x^2 + 9}{(x^2 + 3)^2}. In the quotient u′1+u2\frac{u'}{1 + u^2} the factors (x2+3)2(x^2 + 3)^2 cancel: θ′(x)=6−2x2x4+10x2+9\theta'(x) = \frac{6 - 2x^2}{x^4 + 10x^2 + 9}. Factor the denominator as a quadratic in x2x^2: two numbers with product 99 and sum 1010 are 11 and 99, so x4+10x2+9=(x2+1)(x2+9)x^4 + 10x^2 + 9 = (x^2 + 1)(x^2 + 9), and the two routes agree. Then θ′(3)=6−1810⋅18=−12180=−115≈−0.0667\theta'(3) = \frac{6 - 18}{10 \cdot 18} = -\frac{12}{180} = -\frac{1}{15} \approx -0.0667.

Exercise 10: A final exam question: one function, two corners, three formulas

Let f(x)=sin⁡−12x1+x2f(x) = \sin^{-1}\frac{2x}{1 + x^2}. The figure shows its graph: it climbs to π2\frac{\pi}{2} at x=1x = 1, where it turns sharply, and it is symmetric with respect to the origin. A final exam often takes one such function and asks every question of the chapter about it: domain, values, derivative with a square root to simplify, differentiability, and an identity proved by a zero derivative.

Exact answers, then decimals when asked. The fact 'a zero derivative on an interval gives a constant' is used as a tool.

-6-5-4-3-2-1123456-2-1.5-1-0.50.511.52(1, π/2)(−1, −π/2)y = f(x)
  • a) Prove that −1≤2x1+x2≤1-1 \le \frac{2x}{1 + x^2} \le 1 for every real xx, so that ff is defined on R\mathbb{R}. Compute f(1)f(1), f(−1)f(-1) and f(3)f(\sqrt 3) exactly.
  • b) Show that 1−(2x1+x2)2=(1−x2)2(1+x2)21 - \left(\frac{2x}{1 + x^2}\right)^2 = \frac{(1 - x^2)^2}{(1 + x^2)^2}, deduce that f′(x)=2(1−x2)(1+x2) ∣1−x2∣f'(x) = \frac{2(1 - x^2)}{(1 + x^2)\,|1 - x^2|} for x≠±1x \ne \pm 1, and write f′f' without absolute value on each interval. Evaluate f′(0)f'(0) and f′(2)f'(2).
  • c) Which slopes do the two pieces of the graph approach at x=1x = 1, from the left and from the right? Is ff differentiable at x=1x = 1? Describe the graph there.
  • d) Compare f′f' with the derivative of 2tan⁡−1x2\tan^{-1}x. Deduce, interval by interval, that f(x)=2tan⁡−1xf(x) = 2\tan^{-1}x on [−1,1][-1, 1] and f(x)=π−2tan⁡−1xf(x) = \pi - 2\tan^{-1}x for x≥1x \ge 1, reading each constant at a point of its own interval. Find the formula for x≤−1x \le -1.
  • e) Solve f(x)=π3f(x) = \frac{\pi}{3} and explain why there are two solutions although sin⁡−1\sin^{-1} returns only one angle. Then compute f(3)f(3) to four decimals in two ways.

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  • a) 1+x2∓2x=(1∓x)2≥01 + x^2 \mp 2x = (1 \mp x)^2 \ge 0; f(1)=π2f(1) = \frac{\pi}{2}, f(−1)=−π2f(-1) = -\frac{\pi}{2}, f(3)=π3f(\sqrt 3) = \frac{\pi}{3}
  • b) (1+x2)2−4x2=(1−x2)2(1 + x^2)^2 - 4x^2 = (1 - x^2)^2, root ∣1−x2∣|1 - x^2|; f′=21+x2f' = \frac{2}{1 + x^2} for ∣x∣<1|x| < 1, −21+x2-\frac{2}{1 + x^2} for ∣x∣>1|x| > 1; f′(0)=2f'(0) = 2, f′(2)=−25f'(2) = -\frac{2}{5}
  • c) Left slope 11, right slope −1-1: a corner, ff is not differentiable at 11
  • d) f=2tan⁡−1xf = 2\tan^{-1}x on [−1,1][-1, 1]; f+2tan⁡−1x=πf + 2\tan^{-1}x = \pi on [1,∞)[1, \infty); f=−π−2tan⁡−1xf = -\pi - 2\tan^{-1}x on (−∞,−1](-\infty, -1]
  • e) x=13x = \frac{1}{\sqrt 3} and x=3x = \sqrt 3; f(3)=sin⁡−135=π−2tan⁡−13≈0.6435f(3) = \sin^{-1}\frac{3}{5} = \pi - 2\tan^{-1}3 \approx 0.6435

a) Since 1+x2>01 + x^2 > 0, the double inequality is equivalent to −(1+x2)≤2x≤1+x2-(1 + x^2) \le 2x \le 1 + x^2. On the right: 1+x2−2x=(1−x)2≥01 + x^2 - 2x = (1 - x)^2 \ge 0. On the left: 1+x2+2x=(1+x)2≥01 + x^2 + 2x = (1 + x)^2 \ge 0. Both hold for every real xx, so 2x1+x2\frac{2x}{1 + x^2} is always in [−1,1][-1, 1] and ff is defined on R\mathbb{R}; the values ±1\pm 1 are reached exactly at x=±1x = \pm 1. Then f(1)=sin⁡−11=π2f(1) = \sin^{-1}1 = \frac{\pi}{2}, f(−1)=sin⁡−1(−1)=−π2f(-1) = \sin^{-1}(-1) = -\frac{\pi}{2}, and f(3)=sin⁡−1234=sin⁡−132=π3f(\sqrt 3) = \sin^{-1}\frac{2\sqrt 3}{4} = \sin^{-1}\frac{\sqrt 3}{2} = \frac{\pi}{3}. Recognizing a perfect square is the whole proof: expanding and 'testing some values' proves nothing.

b) 1−4x2(1+x2)2=(1+x2)2−4x2(1+x2)21 - \frac{4x^2}{(1 + x^2)^2} = \frac{(1 + x^2)^2 - 4x^2}{(1 + x^2)^2}, and the numerator is 1+2x2+x4−4x2=1−2x2+x4=(1−x2)21 + 2x^2 + x^4 - 4x^2 = 1 - 2x^2 + x^4 = (1 - x^2)^2. Its square root is ∣1−x2∣1+x2\frac{|1 - x^2|}{1 + x^2}: the root of a square is an ABSOLUTE VALUE, and here 1−x21 - x^2 is negative as soon as ∣x∣>1|x| > 1. The inner derivative, by the quotient rule: u′=2(1+x2)−2x⋅2x(1+x2)2=2(1−x2)(1+x2)2u' = \frac{2(1 + x^2) - 2x \cdot 2x}{(1 + x^2)^2} = \frac{2(1 - x^2)}{(1 + x^2)^2}. So f′(x)=2(1−x2)(1+x2)2⋅1+x2∣1−x2∣=2(1−x2)(1+x2) ∣1−x2∣f'(x) = \frac{2(1 - x^2)}{(1 + x^2)^2} \cdot \frac{1 + x^2}{|1 - x^2|} = \frac{2(1 - x^2)}{(1 + x^2)\,|1 - x^2|} for x≠±1x \ne \pm 1. For ∣x∣<1|x| < 1, ∣1−x2∣=1−x2|1 - x^2| = 1 - x^2 and f′(x)=21+x2f'(x) = \frac{2}{1 + x^2}; for ∣x∣>1|x| > 1, ∣1−x2∣=x2−1|1 - x^2| = x^2 - 1 and f′(x)=−21+x2f'(x) = -\frac{2}{1 + x^2}. f′(0)=2f'(0) = 2 and f′(2)=−25f'(2) = -\frac{2}{5}. The student who writes (1−x2)2=1−x2\sqrt{(1 - x^2)^2} = 1 - x^2 finds 21+x2\frac{2}{1 + x^2} everywhere, a positive slope at x=2x = 2 where the figure goes down.

c) Just left of 11, f′(x)=21+x2f'(x) = \frac{2}{1 + x^2}, which approaches 22=1\frac{2}{2} = 1. Just right of 11, f′(x)=−21+x2f'(x) = -\frac{2}{1 + x^2}, which approaches −1-1. The two pieces arrive at the point (1,π2)\left(1, \frac{\pi}{2}\right) with slopes 11 and −1-1: the graph has a CORNER there, and ff is continuous but not differentiable at x=1x = 1. In the formula of b), the division by ∣1−x2∣=0|1 - x^2| = 0 at x=1x = 1 was the warning. By the symmetry of the graph, the same happens at x=−1x = -1.

d) ddx(2tan⁡−1x)=21+x2\frac{d}{dx}\left(2\tan^{-1}x\right) = \frac{2}{1 + x^2}. On the interval (−1,1)(-1, 1), f′−2(tan⁡−1)′=0f' - 2(\tan^{-1})' = 0, so f(x)−2tan⁡−1xf(x) - 2\tan^{-1}x is constant there; at x=0x = 0 it is 0−0=00 - 0 = 0. So f=2tan⁡−1xf = 2\tan^{-1}x on (−1,1)(-1, 1), and also at ±1\pm 1: f(1)=π2=2⋅π4f(1) = \frac{\pi}{2} = 2 \cdot \frac{\pi}{4}. On (1,∞)(1, \infty), f′+2(tan⁡−1)′=0f' + 2(\tan^{-1})' = 0, so f(x)+2tan⁡−1xf(x) + 2\tan^{-1}x is constant; read it at x=3x = \sqrt 3, a point of THAT interval: π3+2⋅π3=π\frac{\pi}{3} + 2 \cdot \frac{\pi}{3} = \pi. So f(x)=π−2tan⁡−1xf(x) = \pi - 2\tan^{-1}x for x≥1x \ge 1. On (−∞,−1)(-\infty, -1), same derivative relation, constant read at x=−3x = -\sqrt 3: f(−3)+2tan⁡−1(−3)=−π3−2π3=−πf(-\sqrt 3) + 2\tan^{-1}(-\sqrt 3) = -\frac{\pi}{3} - \frac{2\pi}{3} = -\pi, so f(x)=−π−2tan⁡−1xf(x) = -\pi - 2\tan^{-1}x for x≤−1x \le -1. Three intervals, three constants 00, π\pi, −π-\pi: reading the first one at x=0x = 0 and extending it to the whole line would claim f(3)=2π3f(\sqrt 3) = \frac{2\pi}{3}, a value that sin⁡−1\sin^{-1} can never take, since it exceeds π2\frac{\pi}{2}.

e) f(x)=π3f(x) = \frac{\pi}{3} means 2x1+x2=sin⁡π3=32\frac{2x}{1 + x^2} = \sin\frac{\pi}{3} = \frac{\sqrt 3}{2}, legitimate since π3\frac{\pi}{3} is in the range of sin⁡−1\sin^{-1}. Then 4x=3(1+x2)4x = \sqrt 3(1 + x^2), that is 3x2−4x+3=0\sqrt 3x^2 - 4x + \sqrt 3 = 0, with discriminant 16−12=416 - 12 = 4: x=4±223x = \frac{4 \pm 2}{2\sqrt 3}, so x=3≈1.7321x = \sqrt 3 \approx 1.7321 or x=13≈0.5774x = \frac{1}{\sqrt 3} \approx 0.5774. The formulas of d) agree: 2tan⁡−1x=π32\tan^{-1}x = \frac{\pi}{3} gives 13\frac{1}{\sqrt 3} on [−1,1][-1, 1], and π−2tan⁡−1x=π3\pi - 2\tan^{-1}x = \frac{\pi}{3} gives 3\sqrt 3 on [1,∞)[1, \infty). sin⁡−1\sin^{-1} returns one angle, but the INNER function 2x1+x2\frac{2x}{1 + x^2} takes the value 32\frac{\sqrt 3}{2} twice, once on each side of x=1x = 1. Finally f(3)=sin⁡−1610=sin⁡−10.6≈0.6435f(3) = \sin^{-1}\frac{6}{10} = \sin^{-1}0.6 \approx 0.6435, and π−2tan⁡−13≈3.141593−2.498092=0.643501\pi - 2\tan^{-1}3 \approx 3.141593 - 2.498092 = 0.643501: the same, to four decimals 0.64350.6435.

© Ahmed Squalli Houssaini. Exercise set published at www.letuteurscientifique.ca/en/exercices/math203-inverse-trigonometric. Free for personal and classroom use; republishing it elsewhere requires written permission (legal notice).

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