MATH 203 Calculus I • Concordia University, Montreal

Corrected exercises: derivatives of trigonometric functions (MATH 203)

This is the corrected exercise set for the derivatives of trigonometric functions in MATH 203, Differential and Integral Calculus I, at Concordia University, section 3.5 of Thomas' Calculus. The six derivatives are short and the course gives them in one lecture; what the midterm and the final test is everything around them. Each solution names the rule it applies, and a scientific calculator, allowed on the exam, is used only to check a decimal, in radian mode.

The thread running through the whole set: differentiating a trigonometric function takes one line, and the marks go to the ALGEBRA around that line. One identity, sin⁡2x+cos⁡2x=1\sin^2 x + \cos^2 x = 1, in its three disguises 1−sin⁡2x=cos⁡2x1 - \sin^2 x = \cos^2 x, sec⁡2x−tan⁡2x=1\sec^2 x - \tan^2 x = 1 and csc⁡2x−cot⁡2x=1\csc^2 x - \cot^2 x = 1, is used at three moments: BEFORE differentiating, to bring a complex fraction to a single fraction and cancel a factor; AFTER, to collapse the numerator the quotient rule leaves; and IN the equation f′(x)=0f'(x) = 0, to get one function, factor it, and read every solution on the unit circle.

The traps named in the solutions: the minus of a co-function meeting a minus in front of it, the derivatives of cot⁡x\cot x and csc⁡x\csc x crossed, the power rule applied to sec⁡2x\sec^2 x, cancelling a term instead of a factor, the order of the numerator in the quotient rule, a simplification whose domain is forgotten, dividing an equation by xx or sin⁡x\sin x and losing solutions, the ±\pm of a square root, the single angle returned by cos⁡−1\cos^{-1}, and a calculator left in degree mode.

10 corrected exercises • 100 points • 150 minutes

Revision sheet for this chapter → Every MATH 203 chapter →

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Course recap

  • • (sin⁡x)′=cos⁡x(\sin x)' = \cos x, (tan⁡x)′=sec⁡2x(\tan x)' = \sec^2 x, (sec⁡x)′=sec⁡xtan⁡x(\sec x)' = \sec x\tan x, with xx in radians.
  • • (cos⁡x)′=−sin⁡x(\cos x)' = -\sin x, (cot⁡x)′=−csc⁡2x(\cot x)' = -\csc^2 x, (csc⁡x)′=−csc⁡xcot⁡x(\csc x)' = -\csc x\cot x: the co-functions take a minus.
  • • sin⁡2x+cos⁡2x=1\sin^2 x + \cos^2 x = 1, 1+tan⁡2x=sec⁡2x1 + \tan^2 x = \sec^2 x, 1+cot⁡2x=csc⁡2x1 + \cot^2 x = \csc^2 x.
  • • (uv)′=u′v+uv′(uv)' = u'v + uv' and (uv)′=u′v−uv′v2\left(\frac{u}{v}\right)' = \frac{u'v - uv'}{v^2}, in that order.
  • • The derivatives of sin⁡x\sin x and cos⁡x\cos x repeat every 44: only the remainder of nn divided by 44 matters.
  • • Tangent at aa: y=f(a)+f′(a)(x−a)y = f(a) + f'(a)(x - a); normal slope −1f′(a)-\frac{1}{f'(a)}.
  • • cos⁡x=c\cos x = c with −1<c<1-1 < c < 1 has TWO solutions per turn; cos⁡−1\cos^{-1} returns only one.

Part A: the basics (/50)

Exercise 1: The six derivatives, and the identity that comes BEFORE differentiating

The six derivatives are (sin⁡x)′=cos⁡x(\sin x)' = \cos x, (cos⁡x)′=−sin⁡x(\cos x)' = -\sin x, (tan⁡x)′=sec⁡2x(\tan x)' = \sec^2 x, (cot⁡x)′=−csc⁡2x(\cot x)' = -\csc^2 x, (sec⁡x)′=sec⁡xtan⁡x(\sec x)' = \sec x\tan x and (csc⁡x)′=−csc⁡xcot⁡x(\csc x)' = -\csc x\cot x, with xx in radians. They are used here with the sum and constant multiple rules only.

Four of the five functions below are much simpler than they look. Rewriting them in sines and cosines, bringing a complex fraction to a single fraction and using sin⁡2x+cos⁡2x=1\sin^2 x + \cos^2 x = 1 turns a page of quotient rule into one line. The algebra is where the marks are: cancel only a FACTOR, never a term, and say where the simplification is valid.

  • a) Differentiate f(x)=7sin⁡x−4csc⁡x+3x2f(x) = 7\sin x - 4\csc x + 3x^2 and find the exact value of f′(π6)f'\left(\frac{\pi}{6}\right).
  • b) Simplify g(x)=sec⁡x−cos⁡xsin⁡xg(x) = \frac{\sec x - \cos x}{\sin x} to a single trigonometric function, then find g′(x)g'(x) and g′(π3)g'\left(\frac{\pi}{3}\right).
  • c) Simplify h(x)=tan⁡2xsec⁡x+1h(x) = \frac{\tan^2 x}{\sec x + 1}, stating where your simplification holds, then find h′(x)h'(x) and h′(π3)h'\left(\frac{\pi}{3}\right).
  • d) Let k(x)=tan⁡x+cot⁡xk(x) = \tan x + \cot x. Differentiate term by term, write k′(x)k'(x) as a single fraction in sin⁡x\sin x and cos⁡x\cos x, and find k′(π4)k'\left(\frac{\pi}{4}\right) and k′(π6)k'\left(\frac{\pi}{6}\right).
  • e) Let m(x)=cos⁡x1+sin⁡x+1+sin⁡xcos⁡xm(x) = \frac{\cos x}{1 + \sin x} + \frac{1 + \sin x}{\cos x}. Bring mm to a single fraction, show that m(x)=2sec⁡xm(x) = 2\sec x, then find m′(π4)m'\left(\frac{\pi}{4}\right).

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  • a) f′(x)=7cos⁡x+4csc⁡xcot⁡x+6xf'(x) = 7\cos x + 4\csc x\cot x + 6x; f′(π6)=2332+πf'\left(\frac{\pi}{6}\right) = \frac{23\sqrt 3}{2} + \pi
  • b) g(x)=tan⁡xg(x) = \tan x; g′(x)=sec⁡2xg'(x) = \sec^2 x; g′(π3)=4g'\left(\frac{\pi}{3}\right) = 4
  • c) h(x)=sec⁡x−1h(x) = \sec x - 1 where cos⁡x≠0\cos x \ne 0 and cos⁡x≠−1\cos x \ne -1; h′(x)=sec⁡xtan⁡xh'(x) = \sec x\tan x; h′(π3)=23h'\left(\frac{\pi}{3}\right) = 2\sqrt 3
  • d) k′(x)=sec⁡2x−csc⁡2x=sin⁡2x−cos⁡2xsin⁡2xcos⁡2xk'(x) = \sec^2 x - \csc^2 x = \frac{\sin^2 x - \cos^2 x}{\sin^2 x\cos^2 x}; k′(π4)=0k'\left(\frac{\pi}{4}\right) = 0, k′(π6)=−83k'\left(\frac{\pi}{6}\right) = -\frac{8}{3}
  • e) m(x)=2sec⁡xm(x) = 2\sec x; m′(x)=2sec⁡xtan⁡xm'(x) = 2\sec x\tan x; m′(π4)=22m'\left(\frac{\pi}{4}\right) = 2\sqrt 2

a) Sum and constant multiple rules, term by term: f′(x)=7cos⁡x−4(−csc⁡xcot⁡x)+6x=7cos⁡x+4csc⁡xcot⁡x+6xf'(x) = 7\cos x - 4(-\csc x\cot x) + 6x = 7\cos x + 4\csc x\cot x + 6x. The minus written in front of csc⁡x\csc x meets the minus of (csc⁡x)′(\csc x)', and the two make a plus: this is the sign slip of the chapter. At π6\frac{\pi}{6}: cos⁡π6=32\cos\frac{\pi}{6} = \frac{\sqrt 3}{2}, csc⁡π6=1sin⁡(π/6)=2\csc\frac{\pi}{6} = \frac{1}{\sin(\pi/6)} = 2, cot⁡π6=cos⁡(π/6)sin⁡(π/6)=3\cot\frac{\pi}{6} = \frac{\cos(\pi/6)}{\sin(\pi/6)} = \sqrt 3. So f′(π6)=732+4⋅23+6⋅π6=732+1632+π=2332+πf'\left(\frac{\pi}{6}\right) = \frac{7\sqrt 3}{2} + 4 \cdot 2\sqrt 3 + 6\cdot\frac{\pi}{6} = \frac{7\sqrt 3}{2} + \frac{16\sqrt 3}{2} + \pi = \frac{23\sqrt 3}{2} + \pi, about 23.060223.0602.

b) Rewrite the numerator in cosines and bring it to one fraction: sec⁡x−cos⁡x=1cos⁡x−cos⁡2xcos⁡x=1−cos⁡2xcos⁡x=sin⁡2xcos⁡x\sec x - \cos x = \frac{1}{\cos x} - \frac{\cos^2 x}{\cos x} = \frac{1 - \cos^2 x}{\cos x} = \frac{\sin^2 x}{\cos x}, by the Pythagorean identity. Dividing by sin⁡x\sin x is multiplying by 1sin⁡x\frac{1}{\sin x}: g(x)=sin⁡2xcos⁡xsin⁡x=sin⁡xcos⁡x=tan⁡xg(x) = \frac{\sin^2 x}{\cos x\sin x} = \frac{\sin x}{\cos x} = \tan x, wherever sin⁡x≠0\sin x \ne 0 and cos⁡x≠0\cos x \ne 0. Hence g′(x)=sec⁡2xg'(x) = \sec^2 x and g′(π3)=1cos⁡2(π/3)=11/4=4g'\left(\frac{\pi}{3}\right) = \frac{1}{\cos^2(\pi/3)} = \frac{1}{1/4} = 4. The quotient rule applied to the original form also works, but it takes half a page and three chances to lose a sign. The formula sec⁡2x\sec^2 x is valid only on the domain of gg: at x=πx = \pi, where gg does not exist, neither does g′g'.

c) Use the disguise tan⁡2x=sec⁡2x−1\tan^2 x = \sec^2 x - 1: the numerator becomes sec⁡2x−1=(sec⁡x−1)(sec⁡x+1)\sec^2 x - 1 = (\sec x - 1)(\sec x + 1), a difference of squares. The factor sec⁡x+1\sec x + 1 cancels with the denominator, which is legitimate wherever it is not 00, that is cos⁡x≠−1\cos x \ne -1; and cos⁡x≠0\cos x \ne 0 for tan⁡x\tan x and sec⁡x\sec x to exist. There h(x)=sec⁡x−1h(x) = \sec x - 1, so h′(x)=sec⁡xtan⁡xh'(x) = \sec x\tan x and h′(π3)=2⋅3=23h'\left(\frac{\pi}{3}\right) = 2\cdot\sqrt 3 = 2\sqrt 3, about 3.46413.4641. The gesture is to see tan⁡2x\tan^2 x as sec⁡2x−1\sec^2 x - 1 BECAUSE the denominator is written with sec⁡x\sec x: the identity is chosen by the rest of the fraction. The quotient rule on the original form works too, but it needs (tan⁡2x)′(\tan^2 x)', a product, and a page of simplification.

d) Term by term: k′(x)=sec⁡2x−csc⁡2x=1cos⁡2x−1sin⁡2xk'(x) = \sec^2 x - \csc^2 x = \frac{1}{\cos^2 x} - \frac{1}{\sin^2 x}. Common denominator sin⁡2xcos⁡2x\sin^2 x\cos^2 x: k′(x)=sin⁡2x−cos⁡2xsin⁡2xcos⁡2xk'(x) = \frac{\sin^2 x - \cos^2 x}{\sin^2 x\cos^2 x}. At π4\frac{\pi}{4}, sin⁡2x=cos⁡2x=12\sin^2 x = \cos^2 x = \frac{1}{2}, so k′(π4)=0k'\left(\frac{\pi}{4}\right) = 0: the graph of kk has a horizontal tangent there. At π6\frac{\pi}{6}, sin⁡2x=14\sin^2 x = \frac{1}{4} and cos⁡2x=34\cos^2 x = \frac{3}{4}: k′(π6)=1/4−3/43/16=−12⋅163=−83k'\left(\frac{\pi}{6}\right) = \frac{1/4 - 3/4}{3/16} = -\frac{1}{2}\cdot\frac{16}{3} = -\frac{8}{3}. Check with the first form: sec⁡2π6=43\sec^2\frac{\pi}{6} = \frac{4}{3} and csc⁡2π6=4\csc^2\frac{\pi}{6} = 4, and 43−4=−83\frac{4}{3} - 4 = -\frac{8}{3}. The minus of (cot⁡x)′(\cot x)' is what produces a difference and not a sum.

e) Common denominator (1+sin⁡x)cos⁡x(1 + \sin x)\cos x: the numerator is cos⁡2x+(1+sin⁡x)2=cos⁡2x+1+2sin⁡x+sin⁡2x\cos^2 x + (1 + \sin x)^2 = \cos^2 x + 1 + 2\sin x + \sin^2 x. Collect sin⁡2x+cos⁡2x=1\sin^2 x + \cos^2 x = 1: the numerator is 2+2sin⁡x=2(1+sin⁡x)2 + 2\sin x = 2(1 + \sin x). Cancel the FACTOR 1+sin⁡x1 + \sin x, which is not zero where mm is defined (if sin⁡x=−1\sin x = -1 then cos⁡x=0\cos x = 0): m(x)=2(1+sin⁡x)(1+sin⁡x)cos⁡x=2cos⁡x=2sec⁡xm(x) = \frac{2(1 + \sin x)}{(1 + \sin x)\cos x} = \frac{2}{\cos x} = 2\sec x. Hence m′(x)=2sec⁡xtan⁡xm'(x) = 2\sec x\tan x and m′(π4)=2⋅2⋅1=22m'\left(\frac{\pi}{4}\right) = 2\cdot\sqrt 2\cdot 1 = 2\sqrt 2, about 2.82842.8284. Three algebra gestures in a row, expand the square, spot the identity, factor the 22: this is the exact place where a MATH 203 derivative is won or lost.

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Exercise 2: The product rule with trigonometric factors: name u and v, then collect

The product rule (uv)′=u′v+uv′(uv)' = u'v + uv' does not change when a factor is trigonometric; what changes is the number of places where a sign can be lost. Write uu, vv, u′u' and v′v' on your copy before assembling anything. For three factors, (uvw)′=u′vw+uv′w+uvw′(uvw)' = u'vw + uv'w + uvw'.

A derivative is not finished when the rule has been applied: expand, COLLECT like terms and factor, because the exam expects the simplest form and because terms often cancel.

  • a) Differentiate y=x3cos⁡xy = x^3\cos x, factor the result, and find y′(π)y'(\pi).
  • b) Differentiate y=x tan⁡xy = \sqrt{x}\,\tan x, write y′y' as a single fraction, and find y′(π4)y'\left(\frac{\pi}{4}\right).
  • c) Differentiate y=(x2−2)sin⁡x+2xcos⁡xy = (x^2 - 2)\sin x + 2x\cos x and simplify until one term is left. Find y′(π3)y'\left(\frac{\pi}{3}\right).
  • d) Differentiate y=xexsin⁡xy = x e^x\sin x (three factors) and find y′(π)y'(\pi).
  • e) Differentiate y=csc⁡xcot⁡xy = \csc x\cot x and use cot⁡2x=csc⁡2x−1\cot^2 x = \csc^2 x - 1 to write y′y' in terms of csc⁡x\csc x only. Find y′(π6)y'\left(\frac{\pi}{6}\right).

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  • a) y′=3x2cos⁡x−x3sin⁡x=x2(3cos⁡x−xsin⁡x)y' = 3x^2\cos x - x^3\sin x = x^2(3\cos x - x\sin x); y′(π)=−3π2y'(\pi) = -3\pi^2
  • b) y′=tan⁡x+2xsec⁡2x2xy' = \frac{\tan x + 2x\sec^2 x}{2\sqrt x}; y′(π4)=1+ππy'\left(\frac{\pi}{4}\right) = \frac{1 + \pi}{\sqrt\pi}
  • c) y′=x2cos⁡xy' = x^2\cos x; y′(π3)=π218y'\left(\frac{\pi}{3}\right) = \frac{\pi^2}{18}
  • d) y′=ex[(1+x)sin⁡x+xcos⁡x]y' = e^x\left[(1 + x)\sin x + x\cos x\right]; y′(π)=−πeπy'(\pi) = -\pi e^{\pi}
  • e) y′=−csc⁡x(cot⁡2x+csc⁡2x)=−csc⁡x(2csc⁡2x−1)y' = -\csc x\left(\cot^2 x + \csc^2 x\right) = -\csc x\left(2\csc^2 x - 1\right); y′(π6)=−14y'\left(\frac{\pi}{6}\right) = -14

a) u=x3u = x^3, u′=3x2u' = 3x^2, v=cos⁡xv = \cos x, v′=−sin⁡xv' = -\sin x. So y′=3x2cos⁡x+x3(−sin⁡x)=3x2cos⁡x−x3sin⁡x=x2(3cos⁡x−xsin⁡x)y' = 3x^2\cos x + x^3(-\sin x) = 3x^2\cos x - x^3\sin x = x^2(3\cos x - x\sin x), the smallest power x2x^2 factored out. At π\pi: cos⁡π=−1\cos\pi = -1 and sin⁡π=0\sin\pi = 0, so y′(π)=π2(−3−0)=−3π2y'(\pi) = \pi^2(-3 - 0) = -3\pi^2, about −29.6088-29.6088. Writing (x3cos⁡x)′=3x2(−sin⁡x)(x^3\cos x)' = 3x^2(-\sin x), the product of the derivatives, is worth nothing.

b) Rewrite the root as a power first: x=x1/2\sqrt x = x^{1/2}, so u′=12x−1/2=12xu' = \frac{1}{2}x^{-1/2} = \frac{1}{2\sqrt x}. With v=tan⁡xv = \tan x and v′=sec⁡2xv' = \sec^2 x: y′=tan⁡x2x+xsec⁡2xy' = \frac{\tan x}{2\sqrt x} + \sqrt x\sec^2 x. Single fraction over 2x2\sqrt x: xsec⁡2x=2xsec⁡2x2x\sqrt x\sec^2 x = \frac{2x\sec^2 x}{2\sqrt x}, because x⋅2x=2x\sqrt x\cdot 2\sqrt x = 2x. So y′=tan⁡x+2xsec⁡2x2xy' = \frac{\tan x + 2x\sec^2 x}{2\sqrt x}, for x>0x > 0 with cos⁡x≠0\cos x \ne 0. At π4\frac{\pi}{4}: tan⁡=1\tan = 1, sec⁡2=2\sec^2 = 2, 2π/4=π2\sqrt{\pi/4} = \sqrt\pi, so y′(π4)=1+ππy'\left(\frac{\pi}{4}\right) = \frac{1 + \pi}{\sqrt\pi}, about 2.33662.3366. The negative exponent x−1/2x^{-1/2} becomes a root in the DENOMINATOR, not −x-\sqrt x.

c) First product, u=x2−2u = x^2 - 2, v=sin⁡xv = \sin x: 2xsin⁡x+(x2−2)cos⁡x2x\sin x + (x^2 - 2)\cos x. Second product, u=2xu = 2x, v=cos⁡xv = \cos x: 2cos⁡x−2xsin⁡x2\cos x - 2x\sin x. Add and collect: the terms 2xsin⁡x2x\sin x and −2xsin⁡x-2x\sin x cancel, and (x2−2)cos⁡x+2cos⁡x=x2cos⁡x(x^2 - 2)\cos x + 2\cos x = x^2\cos x. So y′=x2cos⁡xy' = x^2\cos x. At π3\frac{\pi}{3}: y′=π29⋅12=π218y' = \frac{\pi^2}{9}\cdot\frac{1}{2} = \frac{\pi^2}{18}, about 0.54830.5483. A student who stops at the four-term sum has not answered a question that says simplify, and misses the whole point: this function was built to have the derivative x2cos⁡xx^2\cos x.

d) u=xu = x, v=exv = e^x, w=sin⁡xw = \sin x, with u′=1u' = 1, v′=exv' = e^x, w′=cos⁡xw' = \cos x: y′=exsin⁡x+xexsin⁡x+xexcos⁡xy' = e^x\sin x + xe^x\sin x + xe^x\cos x. Factor exe^x, then collect the sines: y′=ex[(1+x)sin⁡x+xcos⁡x]y' = e^x\left[(1 + x)\sin x + x\cos x\right]. At π\pi: sin⁡π=0\sin\pi = 0 and cos⁡π=−1\cos\pi = -1, so y′(π)=eπ[0−π]=−πeπy'(\pi) = e^\pi\left[0 - \pi\right] = -\pi e^\pi, about −72.6986-72.6986. Three factors give three terms, each with exactly ONE derivative in it.

e) u=csc⁡xu = \csc x, u′=−csc⁡xcot⁡xu' = -\csc x\cot x, v=cot⁡xv = \cot x, v′=−csc⁡2xv' = -\csc^2 x. So y′=−csc⁡xcot⁡x⋅cot⁡x+csc⁡x⋅(−csc⁡2x)=−csc⁡xcot⁡2x−csc⁡3x=−csc⁡x(cot⁡2x+csc⁡2x)y' = -\csc x\cot x\cdot\cot x + \csc x\cdot(-\csc^2 x) = -\csc x\cot^2 x - \csc^3 x = -\csc x\left(\cot^2 x + \csc^2 x\right). With cot⁡2x=csc⁡2x−1\cot^2 x = \csc^2 x - 1, obtained by dividing sin⁡2x+cos⁡2x=1\sin^2 x + \cos^2 x = 1 by sin⁡2x\sin^2 x: y′=−csc⁡x(2csc⁡2x−1)y' = -\csc x\left(2\csc^2 x - 1\right). At π6\frac{\pi}{6}, csc⁡=2\csc = 2: y′=−2(8−1)=−14y' = -2(8 - 1) = -14. Check with the unsimplified form: cot⁡2π6=3\cot^2\frac{\pi}{6} = 3, and −2(3+4)=−14-2(3 + 4) = -14. Both derivatives are negative, so both minus signs survive the product rule.

Exercise 3: The quotient rule, then the identity that comes AFTER

The quotient rule (uv)′=u′v−uv′v2\left(\frac{u}{v}\right)' = \frac{u'v - uv'}{v^2} has an ORDER: derivative of the top times the bottom first. Swapping the two terms changes the sign of the whole answer.

With trigonometric functions the numerator it produces almost always contains sin⁡2x+cos⁡2x\sin^2 x + \cos^2 x or sec⁡2x−tan⁡2x\sec^2 x - \tan^2 x in disguise. Expanding, then spotting the identity, is the gesture that turns an unreadable fraction into the expected answer.

  • a) Differentiate q(x)=sin⁡x+cos⁡xsin⁡x−cos⁡xq(x) = \frac{\sin x + \cos x}{\sin x - \cos x} and show that q′(x)=−2(sin⁡x−cos⁡x)2q'(x) = \frac{-2}{(\sin x - \cos x)^2}. Find q′(0)q'(0), and say whether qq is defined at π4\frac{\pi}{4}.
  • b) Differentiate r(x)=1−cos⁡x1+cos⁡xr(x) = \frac{1 - \cos x}{1 + \cos x}, simplify, and find r′(2π3)r'\left(\frac{2\pi}{3}\right).
  • c) Differentiate g(x)=tan⁡xxg(x) = \frac{\tan x}{x} and find g′(π4)g'\left(\frac{\pi}{4}\right).
  • d) Differentiate h(x)=sec⁡xtan⁡xh(x) = \frac{\sec x}{\tan x} by the quotient rule and simplify with tan⁡2x−sec⁡2x=−1\tan^2 x - \sec^2 x = -1. Check by simplifying hh first, and find h′(π3)h'\left(\frac{\pi}{3}\right).
  • e) Differentiate s(x)=x2cos⁡xs(x) = \frac{x^2}{\cos x} twice over: by the quotient rule, then as the product x2sec⁡xx^2\sec x. Show that the two answers agree and find s′(π3)s'\left(\frac{\pi}{3}\right).

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  • a) q′(x)=−2(sin⁡x−cos⁡x)2q'(x) = \frac{-2}{(\sin x - \cos x)^2}; q′(0)=−2q'(0) = -2; qq is not defined at π4\frac{\pi}{4}.
  • b) r′(x)=2sin⁡x(1+cos⁡x)2r'(x) = \frac{2\sin x}{(1 + \cos x)^2}; r′(2π3)=43r'\left(\frac{2\pi}{3}\right) = 4\sqrt 3
  • c) g′(x)=xsec⁡2x−tan⁡xx2g'(x) = \frac{x\sec^2 x - \tan x}{x^2}; g′(π4)=8π−16π2g'\left(\frac{\pi}{4}\right) = \frac{8\pi - 16}{\pi^2}
  • d) h′(x)=−csc⁡xcot⁡xh'(x) = -\csc x\cot x (and h=csc⁡xh = \csc x where cos⁡x≠0\cos x \ne 0); h′(π3)=−23h'\left(\frac{\pi}{3}\right) = -\frac{2}{3}
  • e) s′(x)=2xcos⁡x+x2sin⁡xcos⁡2x=2xsec⁡x+x2sec⁡xtan⁡xs'(x) = \frac{2x\cos x + x^2\sin x}{\cos^2 x} = 2x\sec x + x^2\sec x\tan x; s′(π3)=4π3+23 π29s'\left(\frac{\pi}{3}\right) = \frac{4\pi}{3} + \frac{2\sqrt 3\,\pi^2}{9}

a) u=sin⁡x+cos⁡xu = \sin x + \cos x, u′=cos⁡x−sin⁡xu' = \cos x - \sin x; v=sin⁡x−cos⁡xv = \sin x - \cos x, v′=cos⁡x+sin⁡xv' = \cos x + \sin x. Numerator: u′v−uv′=(cos⁡x−sin⁡x)(sin⁡x−cos⁡x)−(sin⁡x+cos⁡x)2=−(sin⁡x−cos⁡x)2−(sin⁡x+cos⁡x)2u'v - uv' = (\cos x - \sin x)(\sin x - \cos x) - (\sin x + \cos x)^2 = -(\sin x - \cos x)^2 - (\sin x + \cos x)^2. Expand both squares: (sin⁡2x−2sin⁡xcos⁡x+cos⁡2x)+(sin⁡2x+2sin⁡xcos⁡x+cos⁡2x)=2(sin⁡2x+cos⁡2x)=2(\sin^2 x - 2\sin x\cos x + \cos^2 x) + (\sin^2 x + 2\sin x\cos x + \cos^2 x) = 2(\sin^2 x + \cos^2 x) = 2. So the numerator is −2-2 and q′(x)=−2(sin⁡x−cos⁡x)2q'(x) = \frac{-2}{(\sin x - \cos x)^2}. Then q′(0)=−2(0−1)2=−2q'(0) = \frac{-2}{(0 - 1)^2} = -2. At π4\frac{\pi}{4}, sin⁡x=cos⁡x\sin x = \cos x: the denominator of qq vanishes, qq is not defined there and neither is q′q'. The cross terms ±2sin⁡xcos⁡x\pm 2\sin x\cos x cancel: expanding is what makes the identity visible.

b) u=1−cos⁡xu = 1 - \cos x, u′=sin⁡xu' = \sin x; v=1+cos⁡xv = 1 + \cos x, v′=−sin⁡xv' = -\sin x. Numerator: sin⁡x(1+cos⁡x)−(1−cos⁡x)(−sin⁡x)=sin⁡x+sin⁡xcos⁡x+sin⁡x−sin⁡xcos⁡x=2sin⁡x\sin x(1 + \cos x) - (1 - \cos x)(-\sin x) = \sin x + \sin x\cos x + \sin x - \sin x\cos x = 2\sin x. So r′(x)=2sin⁡x(1+cos⁡x)2r'(x) = \frac{2\sin x}{(1 + \cos x)^2}, for cos⁡x≠−1\cos x \ne -1. At 2π3\frac{2\pi}{3}: sin⁡=32\sin = \frac{\sqrt 3}{2}, 1+cos⁡=121 + \cos = \frac{1}{2}, so r′=31/4=43r' = \frac{\sqrt 3}{1/4} = 4\sqrt 3, about 6.92826.9282. The minus of the rule meets the minus of v′v': −(1−cos⁡x)(−sin⁡x)-(1 - \cos x)(-\sin x) is a PLUS. Lose it and the sin⁡xcos⁡x\sin x\cos x terms add instead of cancelling.

c) u=tan⁡xu = \tan x, u′=sec⁡2xu' = \sec^2 x, v=xv = x, v′=1v' = 1: g′(x)=xsec⁡2x−tan⁡xx2g'(x) = \frac{x\sec^2 x - \tan x}{x^2}, for x≠0x \ne 0 and cos⁡x≠0\cos x \ne 0. At π4\frac{\pi}{4}: π4⋅2−1π2/16=16⋅π/2−1π2=8π−16π2\frac{\frac{\pi}{4}\cdot 2 - 1}{\pi^2/16} = 16\cdot\frac{\pi/2 - 1}{\pi^2} = \frac{8\pi - 16}{\pi^2}, about 0.92540.9254. The order matters: tan⁡x−xsec⁡2xx2\frac{\tan x - x\sec^2 x}{x^2} gives −0.9254-0.9254, a slope of the wrong sign.

d) u=sec⁡xu = \sec x, u′=sec⁡xtan⁡xu' = \sec x\tan x; v=tan⁡xv = \tan x, v′=sec⁡2xv' = \sec^2 x. Numerator: sec⁡xtan⁡x⋅tan⁡x−sec⁡x⋅sec⁡2x=sec⁡x(tan⁡2x−sec⁡2x)=−sec⁡x\sec x\tan x\cdot\tan x - \sec x\cdot\sec^2 x = \sec x\left(\tan^2 x - \sec^2 x\right) = -\sec x, by sec⁡2x=1+tan⁡2x\sec^2 x = 1 + \tan^2 x. So h′(x)=−sec⁡xtan⁡2x=−1cos⁡x⋅cos⁡2xsin⁡2x=−cos⁡xsin⁡2x=−csc⁡xcot⁡xh'(x) = \frac{-\sec x}{\tan^2 x} = -\frac{1}{\cos x}\cdot\frac{\cos^2 x}{\sin^2 x} = -\frac{\cos x}{\sin^2 x} = -\csc x\cot x. Second road: h(x)=1cos⁡x⋅cos⁡xsin⁡x=1sin⁡x=csc⁡xh(x) = \frac{1}{\cos x}\cdot\frac{\cos x}{\sin x} = \frac{1}{\sin x} = \csc x, so h′(x)=−csc⁡xcot⁡xh'(x) = -\csc x\cot x at once. But hh is NOT defined where cos⁡x=0\cos x = 0, although csc⁡x\csc x is: the formula holds only where sin⁡x≠0\sin x \ne 0 and cos⁡x≠0\cos x \ne 0. At π3\frac{\pi}{3}: −23⋅13=−23-\frac{2}{\sqrt 3}\cdot\frac{1}{\sqrt 3} = -\frac{2}{3}.

e) Quotient rule, u=x2u = x^2, v=cos⁡xv = \cos x: s′(x)=2xcos⁡x−x2(−sin⁡x)cos⁡2x=2xcos⁡x+x2sin⁡xcos⁡2xs'(x) = \frac{2x\cos x - x^2(-\sin x)}{\cos^2 x} = \frac{2x\cos x + x^2\sin x}{\cos^2 x}. Product rule on x2sec⁡xx^2\sec x: s′(x)=2xsec⁡x+x2sec⁡xtan⁡xs'(x) = 2x\sec x + x^2\sec x\tan x. They agree: split the fraction, 2xcos⁡xcos⁡2x=2xcos⁡x=2xsec⁡x\frac{2x\cos x}{\cos^2 x} = \frac{2x}{\cos x} = 2x\sec x and x2sin⁡xcos⁡2x=x2⋅1cos⁡x⋅sin⁡xcos⁡x=x2sec⁡xtan⁡x\frac{x^2\sin x}{\cos^2 x} = x^2\cdot\frac{1}{\cos x}\cdot\frac{\sin x}{\cos x} = x^2\sec x\tan x. At π3\frac{\pi}{3}, sec⁡=2\sec = 2, tan⁡=3\tan = \sqrt 3: s′=2⋅π3⋅2+π29⋅23=4π3+23 π29s' = 2\cdot\frac{\pi}{3}\cdot 2 + \frac{\pi^2}{9}\cdot 2\sqrt 3 = \frac{4\pi}{3} + \frac{2\sqrt 3\,\pi^2}{9}, about 7.98767.9876. When the denominator is a single cos⁡x\cos x, the product with sec⁡x\sec x is usually shorter.

Exercise 4: Tangent and normal lines with exact trigonometric values

The tangent to y=f(x)y = f(x) at aa is y=f(a)+f′(a)(x−a)y = f(a) + f'(a)(x - a), and the normal is the line through the same point with slope −1f′(a)-\frac{1}{f'(a)} when f′(a)≠0f'(a) \ne 0. Every value is exact: csc⁡π6=2\csc\frac{\pi}{6} = 2, sec⁡π4=2\sec\frac{\pi}{4} = \sqrt 2, and π\pi stays π\pi in the equation. The calculator is only used to CHECK a decimal, in radian mode.

The figure shows y=xsin⁡xy = x\sin x for 0≤x≤8.60 \le x \le 8.6, between the dashed lines y=xy = x and y=−xy = -x, and the three points where it touches them; PP is the first, at x=π2x = \frac{\pi}{2}.

π2πy = x sin xy = xy = -xP
  • a) Find the tangent to y=csc⁡xy = \csc x at x=π6x = \frac{\pi}{6}, in the form y=mx+by = mx + b.
  • b) Find the tangent and the normal to y=xsin⁡xy = x\sin x at PP. Show that the normal meets the curve again on the xx-axis.
  • c) Show that at EVERY point where sin⁡x=1\sin x = 1 the tangent to y=xsin⁡xy = x\sin x is the line y=xy = x, and at every point where sin⁡x=−1\sin x = -1 it is y=−xy = -x. What does the figure show there?
  • d) Find the tangent and the normal to y=sec⁡xy = \sec x at x=π4x = \frac{\pi}{4}.
  • e) Find the tangent to y=cos⁡xxy = \frac{\cos x}{x} at x=π2x = \frac{\pi}{2} and the point where it crosses the yy-axis.

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  • a) y=−23 x+2+3 π3y = -2\sqrt 3\,x + 2 + \frac{\sqrt 3\,\pi}{3}
  • b) Tangent y=xy = x; normal y=π−xy = \pi - x, which meets the curve at (π,0)(\pi, 0).
  • c) At sin⁡a=1\sin a = 1: y(a)=ay(a) = a, y′(a)=1y'(a) = 1, tangent y=xy = x; at sin⁡a=−1\sin a = -1: tangent y=−xy = -x. The curve touches the dashed lines there.
  • d) Tangent y=2+2(x−π4)y = \sqrt 2 + \sqrt 2\left(x - \frac{\pi}{4}\right); normal y=2−22(x−π4)y = \sqrt 2 - \frac{\sqrt 2}{2}\left(x - \frac{\pi}{4}\right)
  • e) y=1−2xπy = 1 - \frac{2x}{\pi}, crossing the yy-axis at (0,1)(0, 1)

a) Point: csc⁡π6=1sin⁡(π/6)=2\csc\frac{\pi}{6} = \frac{1}{\sin(\pi/6)} = 2. Slope: (csc⁡x)′=−csc⁡xcot⁡x(\csc x)' = -\csc x\cot x, and cot⁡π6=3\cot\frac{\pi}{6} = \sqrt 3, so m=−23m = -2\sqrt 3. Tangent: y=2−23(x−π6)=−23 x+2+23 π6=−23 x+2+3 π3y = 2 - 2\sqrt 3\left(x - \frac{\pi}{6}\right) = -2\sqrt 3\,x + 2 + \frac{2\sqrt 3\,\pi}{6} = -2\sqrt 3\,x + 2 + \frac{\sqrt 3\,\pi}{3}. The intercept is about 3.81383.8138. Expanding −23⋅(−π6)-2\sqrt 3\cdot\left(-\frac{\pi}{6}\right) is where the sign goes: minus times minus is plus.

b) y(π2)=π2sin⁡π2=π2y(\frac{\pi}{2}) = \frac{\pi}{2}\sin\frac{\pi}{2} = \frac{\pi}{2}. Product rule: y′=sin⁡x+xcos⁡xy' = \sin x + x\cos x, so y′(π2)=1+π2⋅0=1y'\left(\frac{\pi}{2}\right) = 1 + \frac{\pi}{2}\cdot 0 = 1. Tangent: y=π2+(x−π2)=xy = \frac{\pi}{2} + \left(x - \frac{\pi}{2}\right) = x. Normal: slope −11=−1-\frac{1}{1} = -1, so y=π2−(x−π2)=π−xy = \frac{\pi}{2} - \left(x - \frac{\pi}{2}\right) = \pi - x. It meets the xx-axis at (π,0)(\pi, 0), and πsin⁡π=0\pi\sin\pi = 0: that point is on the curve. The solution figure is drawn with equal scales, so the right angle between tangent and normal is true.

c) Let aa be a point where sin⁡a=1\sin a = 1; then cos⁡a=0\cos a = 0, by sin⁡2a+cos⁡2a=1\sin^2 a + \cos^2 a = 1. So y(a)=a⋅1=ay(a) = a\cdot 1 = a and y′(a)=sin⁡a+acos⁡a=1+0=1y'(a) = \sin a + a\cos a = 1 + 0 = 1: the tangent is y=a+1⋅(x−a)=xy = a + 1\cdot(x - a) = x, whatever aa is. Where sin⁡a=−1\sin a = -1, again cos⁡a=0\cos a = 0, y(a)=−ay(a) = -a, y′(a)=−1y'(a) = -1, and the tangent is y=−a−(x−a)=−xy = -a - (x - a) = -x. Since ∣xsin⁡x∣≤∣x∣|x\sin x| \le |x|, the curve lies between the two dashed lines, and at those points it touches them, tangentially, without crossing: the orange dots of the figure. The key step is cos⁡a=0\cos a = 0, which kills the term acos⁡aa\cos a that would otherwise depend on aa.

d) sec⁡π4=1cos⁡(π/4)=22=2\sec\frac{\pi}{4} = \frac{1}{\cos(\pi/4)} = \frac{2}{\sqrt 2} = \sqrt 2 and tan⁡π4=1\tan\frac{\pi}{4} = 1. Slope: sec⁡xtan⁡x=2\sec x\tan x = \sqrt 2. Tangent: y=2+2(x−π4)y = \sqrt 2 + \sqrt 2\left(x - \frac{\pi}{4}\right). Normal slope: −12=−22-\frac{1}{\sqrt 2} = -\frac{\sqrt 2}{2}, after rationalizing; normal: y=2−22(x−π4)y = \sqrt 2 - \frac{\sqrt 2}{2}\left(x - \frac{\pi}{4}\right). The normal slope is the NEGATIVE reciprocal: 12\frac{1}{\sqrt 2} alone gives a line that is not perpendicular to anything useful.

e) y(π2)=cos⁡(π/2)π/2=0y\left(\frac{\pi}{2}\right) = \frac{\cos(\pi/2)}{\pi/2} = 0. Quotient rule, u=cos⁡xu = \cos x, u′=−sin⁡xu' = -\sin x, v=xv = x, v′=1v' = 1: y′=−xsin⁡x−cos⁡xx2y' = \frac{-x\sin x - \cos x}{x^2}, so y′(π2)=−π2⋅1−0π2/4=−π2⋅4π2=−2πy'\left(\frac{\pi}{2}\right) = \frac{-\frac{\pi}{2}\cdot 1 - 0}{\pi^2/4} = -\frac{\pi}{2}\cdot\frac{4}{\pi^2} = -\frac{2}{\pi}, about −0.6366-0.6366. Tangent: y=0−2π(x−π2)=1−2xπy = 0 - \frac{2}{\pi}\left(x - \frac{\pi}{2}\right) = 1 - \frac{2x}{\pi}. At x=0x = 0 it gives y=1y = 1: it crosses the yy-axis at (0,1)(0, 1). Dividing by the fraction π24\frac{\pi^2}{4} is multiplying by 4π2\frac{4}{\pi^2}: the complex fraction is where this slope is usually lost.

π/2πPtangent y = xnormal y = π - xy = x sin x

Exercise 5: Higher derivatives by the cycle of four, and the equation y'' + y = 0

The derivatives of sin⁡x\sin x repeat every four steps, sin⁡x→cos⁡x→−sin⁡x→−cos⁡x→sin⁡x\sin x \to \cos x \to -\sin x \to -\cos x \to \sin x, and so do those of cos⁡x\cos x. A derivative of order nn is read off the REMAINDER of nn divided by 44.

The same two derivatives make sin⁡x\sin x and cos⁡x\cos x solutions of y′′+y=0y'' + y = 0, the equation of every oscillation of this chapter. Nothing is solved here: each claim is VERIFIED by differentiating twice and substituting.

  • a) Find d35dx35cos⁡x\frac{d^{35}}{dx^{35}}\cos x and d102dx102sin⁡x\frac{d^{102}}{dx^{102}}\sin x.
  • b) Let f(x)=3sin⁡x−5cos⁡xf(x) = 3\sin x - 5\cos x. Find f(0)f(0), f′(0)f'(0), f′′(0)f''(0), f′′′(0)f'''(0), then f(2026)(0)f^{(2026)}(0) and f(2027)(0)f^{(2027)}(0).
  • c) Show that y=Acos⁡x+Bsin⁡xy = A\cos x + B\sin x satisfies y′′+y=0y'' + y = 0 for all constants AA and BB. Find the constants for which y(0)=2y(0) = 2 and y′(0)=−3y'(0) = -3.
  • d) Show that y=xsin⁡xy = x\sin x satisfies y′′+y=2cos⁡xy'' + y = 2\cos x. Deduce the constant AA for which y=Axsin⁡xy = Ax\sin x satisfies y′′+y=6cos⁡xy'' + y = 6\cos x.
  • e) Compute y′′y'' for y=csc⁡xy = \csc x and decide whether y=csc⁡xy = \csc x satisfies y′′+y=0y'' + y = 0. Evaluate y′′(π2)y''\left(\frac{\pi}{2}\right).

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  • a) sin⁡x\sin x and −sin⁡x-\sin x
  • b) −5,3,5,−3-5, 3, 5, -3 repeating; f(2026)(0)=5f^{(2026)}(0) = 5, f(2027)(0)=−3f^{(2027)}(0) = -3
  • c) y′′=−yy'' = -y; A=2A = 2, B=−3B = -3: y=2cos⁡x−3sin⁡xy = 2\cos x - 3\sin x
  • d) y′′=2cos⁡x−xsin⁡xy'' = 2\cos x - x\sin x, so y′′+y=2cos⁡xy'' + y = 2\cos x; A=3A = 3
  • e) y′′=csc⁡x(cot⁡2x+csc⁡2x)y'' = \csc x\left(\cot^2 x + \csc^2 x\right), y′′+y=2csc⁡3x≠0y'' + y = 2\csc^3 x \ne 0: no; y′′(π2)=1y''\left(\frac{\pi}{2}\right) = 1

a) The derivatives of cos⁡x\cos x are −sin⁡x-\sin x, −cos⁡x-\cos x, sin⁡x\sin x, cos⁡x\cos x, then again. 35=4×8+335 = 4\times 8 + 3, so d35dx35cos⁡x=(cos⁡x)′′′=sin⁡x\frac{d^{35}}{dx^{35}}\cos x = (\cos x)''' = \sin x. For sine, 102=4×25+2102 = 4\times 25 + 2, so d102dx102sin⁡x=(sin⁡x)′′=−sin⁡x\frac{d^{102}}{dx^{102}}\sin x = (\sin x)'' = -\sin x. Check each division by multiplying back: 32+3=3532 + 3 = 35 and 100+2=102100 + 2 = 102. The parity of nn only says sine or cosine; the sign needs the remainder.

b) f(0)=0−5=−5f(0) = 0 - 5 = -5. f′(x)=3cos⁡x+5sin⁡xf'(x) = 3\cos x + 5\sin x, f′(0)=3f'(0) = 3. f′′(x)=−3sin⁡x+5cos⁡xf''(x) = -3\sin x + 5\cos x, f′′(0)=5f''(0) = 5. f′′′(x)=−3cos⁡x−5sin⁡xf'''(x) = -3\cos x - 5\sin x, f′′′(0)=−3f'''(0) = -3. f(4)(x)=3sin⁡x−5cos⁡x=f(x)f^{(4)}(x) = 3\sin x - 5\cos x = f(x), so the values at 00 repeat: −5,3,5,−3,−5,…-5, 3, 5, -3, -5, \dots Now 2026=4×506+22026 = 4\times 506 + 2, so f(2026)(0)=f′′(0)=5f^{(2026)}(0) = f''(0) = 5, and 2027=4×506+32027 = 4\times 506 + 3, so f(2027)(0)=f′′′(0)=−3f^{(2027)}(0) = f'''(0) = -3. The minus in front of 5cos⁡x5\cos x is carried through every step: (−5cos⁡x)′=+5sin⁡x(-5\cos x)' = +5\sin x.

c) y′=−Asin⁡x+Bcos⁡xy' = -A\sin x + B\cos x and y′′=−Acos⁡x−Bsin⁡x=−yy'' = -A\cos x - B\sin x = -y, so y′′+y=0y'' + y = 0 for every AA and BB: a VERIFICATION by two differentiations. Then y(0)=Acos⁡0+Bsin⁡0=Ay(0) = A\cos 0 + B\sin 0 = A, so A=2A = 2, and y′(0)=−A⋅0+B⋅1=By'(0) = -A\cdot 0 + B\cdot 1 = B, so B=−3B = -3. The function is y=2cos⁡x−3sin⁡xy = 2\cos x - 3\sin x. The value at 00 fixes the cosine coefficient, the slope at 00 fixes the sine coefficient.

d) Product rule: y′=sin⁡x+xcos⁡xy' = \sin x + x\cos x. Again, on each term: y′′=cos⁡x+(cos⁡x−xsin⁡x)=2cos⁡x−xsin⁡xy'' = \cos x + (\cos x - x\sin x) = 2\cos x - x\sin x. So y′′+y=2cos⁡x−xsin⁡x+xsin⁡x=2cos⁡xy'' + y = 2\cos x - x\sin x + x\sin x = 2\cos x. For y=Axsin⁡xy = Ax\sin x, the constant multiple rule multiplies everything by AA: y′′+y=2Acos⁡xy'' + y = 2A\cos x, and this equals 6cos⁡x6\cos x for every xx exactly when A=3A = 3. The term xsin⁡xx\sin x cancels, which is the reason this function is chosen: it produces a pure cosine.

e) y′=−csc⁡xcot⁡xy' = -\csc x\cot x. By Exercise 2 e), (csc⁡xcot⁡x)′=−csc⁡x(cot⁡2x+csc⁡2x)(\csc x\cot x)' = -\csc x(\cot^2 x + \csc^2 x), so y′′=csc⁡x(cot⁡2x+csc⁡2x)y'' = \csc x\left(\cot^2 x + \csc^2 x\right). Then y′′+y=csc⁡x(cot⁡2x+1+csc⁡2x)=csc⁡x⋅2csc⁡2x=2csc⁡3xy'' + y = \csc x\left(\cot^2 x + 1 + \csc^2 x\right) = \csc x\cdot 2\csc^2 x = 2\csc^3 x, using cot⁡2x+1=csc⁡2x\cot^2 x + 1 = \csc^2 x. This is never 00, because csc⁡x\csc x never is: csc⁡x\csc x does NOT satisfy y′′+y=0y'' + y = 0. At π2\frac{\pi}{2}: csc⁡=1\csc = 1, cot⁡=0\cot = 0, y′′=1y'' = 1 and y′′+y=2y'' + y = 2. Being built from sin⁡x\sin x is not enough; only the combinations Acos⁡x+Bsin⁡xA\cos x + B\sin x pass.

Part B: problems and reasoning (/50)

Exercise 6: Horizontal and parallel tangents on an interval: one function, factor, every quadrant

A horizontal tangent at aa means f′(a)=0f'(a) = 0; a tangent parallel to a line of slope mm means f′(a)=mf'(a) = m. With trigonometric functions both are trigonometric EQUATIONS, and three algebra gestures decide them: turn the equation into ONE function with an identity, FACTOR instead of dividing, and read EVERY solution of the interval on the unit circle, not only the one that cos⁡−1\cos^{-1} or sin⁡−1\sin^{-1} returns.

The figure shows g(x)=sin⁡x (1−cos⁡x)g(x) = \sin x\,(1 - \cos x) on [0,2π][0, 2\pi], the function of question b).

π/23π/2π2π1-1y = sin x (1 - cos x)
  • a) Find the point of f(x)=2sec⁡x−tan⁡xf(x) = 2\sec x - \tan x, −π2<x<π2-\frac{\pi}{2} < x < \frac{\pi}{2}, where the tangent is horizontal.
  • b) Find every point of g(x)=sin⁡x (1−cos⁡x)g(x) = \sin x\,(1 - \cos x), 0≤x≤2π0 \le x \le 2\pi, where the tangent is horizontal, using sin⁡2x=1−cos⁡2x\sin^2 x = 1 - \cos^2 x to get an equation in cos⁡x\cos x alone. How many are there?
  • c) Find the points of y=tan⁡xy = \tan x, −π2<x<π2-\frac{\pi}{2} < x < \frac{\pi}{2}, where the tangent is parallel to the line y=4xy = 4x.
  • d) Find every xx in (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right) where the tangents to y=sin⁡xy = \sin x and y=tan⁡xy = \tan x are parallel.
  • e) Find every point of f(x)=sin⁡x−xcos⁡xf(x) = \sin x - x\cos x, 0≤x≤2π0 \le x \le 2\pi, where the tangent is horizontal.

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  • a) (π6,3)\left(\frac{\pi}{6}, \sqrt 3\right)
  • b) Four points: (0,0)(0, 0), (2π3,334)\left(\frac{2\pi}{3}, \frac{3\sqrt 3}{4}\right), (4π3,−334)\left(\frac{4\pi}{3}, -\frac{3\sqrt 3}{4}\right), (2π,0)(2\pi, 0)
  • c) (π3,3)\left(\frac{\pi}{3}, \sqrt 3\right) and (−π3,−3)\left(-\frac{\pi}{3}, -\sqrt 3\right)
  • d) Only x=0x = 0 (cos⁡3x=1\cos^3 x = 1), where both tangents are y=xy = x.
  • e) (0,0)(0, 0), (π,π)(\pi, \pi), (2π,−2π)(2\pi, -2\pi)

a) f′(x)=2sec⁡xtan⁡x−sec⁡2x=sec⁡x (2tan⁡x−sec⁡x)f'(x) = 2\sec x\tan x - \sec^2 x = \sec x\,(2\tan x - \sec x), factoring the common sec⁡x\sec x. The factor sec⁡x=1cos⁡x\sec x = \frac{1}{\cos x} is never 00, so f′(x)=0  ⟺  2tan⁡x=sec⁡xf'(x) = 0 \iff 2\tan x = \sec x. Multiply by cos⁡x\cos x, which is positive on the interval, so no solution is created or lost: 2sin⁡x=12\sin x = 1, sin⁡x=12\sin x = \frac{1}{2}. On (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right) the only solution is x=π6x = \frac{\pi}{6}; the other angle with sine 12\frac{1}{2}, 5π6\frac{5\pi}{6}, is outside the interval. Height: f(π6)=2⋅23−13=33=3f\left(\frac{\pi}{6}\right) = 2\cdot\frac{2}{\sqrt 3} - \frac{1}{\sqrt 3} = \frac{3}{\sqrt 3} = \sqrt 3. The complex equation 2tan⁡x=sec⁡x2\tan x = \sec x became a basic one by clearing the denominators cos⁡x\cos x.

b) Product rule: g′(x)=cos⁡x (1−cos⁡x)+sin⁡x (sin⁡x)=cos⁡x−cos⁡2x+sin⁡2xg'(x) = \cos x\,(1 - \cos x) + \sin x\,(\sin x) = \cos x - \cos^2 x + \sin^2 x. Replace sin⁡2x\sin^2 x by 1−cos⁡2x1 - \cos^2 x to get ONE function: g′(x)=−2cos⁡2x+cos⁡x+1g'(x) = -2\cos^2 x + \cos x + 1, a quadratic in c=cos⁡xc = \cos x, which factors as −(2c+1)(c−1)-(2c + 1)(c - 1). So g′(x)=0  ⟺  cos⁡x=−12g'(x) = 0 \iff \cos x = -\frac{1}{2} or cos⁡x=1\cos x = 1: x=2π3x = \frac{2\pi}{3}, x=4π3x = \frac{4\pi}{3}, and x=0x = 0, x=2πx = 2\pi, the endpoints of the closed interval. Heights: g(2π3)=32⋅32=334g\left(\frac{2\pi}{3}\right) = \frac{\sqrt 3}{2}\cdot\frac{3}{2} = \frac{3\sqrt 3}{4}, g(4π3)=−334g\left(\frac{4\pi}{3}\right) = -\frac{3\sqrt 3}{4}, g(0)=g(2π)=0g(0) = g(2\pi) = 0. Four points. The two at the endpoints are the ones that get lost: the factor cos⁡x−1\cos x - 1 vanishes only there, and the curve leaves the axis FLAT without turning back, as the figure shows. A horizontal tangent is not necessarily a peak or a valley. The derivative of −cos⁡x-\cos x is +sin⁡x+\sin x, which is where the plus in sin⁡x (sin⁡x)\sin x\,(\sin x) comes from.

c) Parallel to y=4xy = 4x means slope 44: sec⁡2x=4\sec^2 x = 4, so cos⁡2x=14\cos^2 x = \frac{1}{4} and cos⁡x=±12\cos x = \pm\frac{1}{2}. On (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right) cosine is positive, so only cos⁡x=12\cos x = \frac{1}{2} is possible, and it has TWO solutions there: x=π3x = \frac{\pi}{3} and x=−π3x = -\frac{\pi}{3}. Points: (π3,3)\left(\frac{\pi}{3}, \sqrt 3\right) and (−π3,−3)\left(-\frac{\pi}{3}, -\sqrt 3\right). Two losses are possible here: the ±\pm of the square root, which is rejected for a REASON (the sign of cosine on the interval), and the negative angle, which cos⁡−1\cos^{-1} never returns.

d) Equal slopes: cos⁡x=sec⁡2x=1cos⁡2x\cos x = \sec^2 x = \frac{1}{\cos^2 x}. Multiplying by cos⁡2x≠0\cos^2 x \ne 0: cos⁡3x=1\cos^3 x = 1, so cos⁡x=1\cos x = 1, because the only real cube root of 11 is 11. On the interval, x=0x = 0. At 00 both curves pass through the origin with slope 11: their tangents are the SAME line, y=xy = x. Everywhere else in the interval 0<cos⁡x<1<sec⁡2x0 < \cos x < 1 < \sec^2 x, so the tangent to tan⁡x\tan x is always steeper.

e) Product rule on xcos⁡xx\cos x, then subtract the WHOLE derivative: f′(x)=cos⁡x−(cos⁡x−xsin⁡x)=xsin⁡xf'(x) = \cos x - \left(\cos x - x\sin x\right) = x\sin x. Forgetting the bracket gives cos⁡x−cos⁡x−xsin⁡x=−xsin⁡x\cos x - \cos x - x\sin x = -x\sin x, which happens to have the same zeros but the wrong sign everywhere. Now xsin⁡x=0  ⟺  x=0x\sin x = 0 \iff x = 0 or sin⁡x=0\sin x = 0, that is x=0x = 0, π\pi, 2π2\pi on [0,2π][0, 2\pi]. Heights: f(0)=0f(0) = 0, f(π)=0−π(−1)=πf(\pi) = 0 - \pi(-1) = \pi, f(2π)=0−2π⋅1=−2πf(2\pi) = 0 - 2\pi\cdot 1 = -2\pi. Dividing by xx would lose the endpoint x=0x = 0, where the tangent is indeed horizontal.

π/23π/2π2π1-1green: cos x = -1/2red: cos x = 1

Exercise 7: Reading f and f' on one figure: secant, tangent and their derivatives

The figure shows three curves AA, BB and CC on −1.25≤x≤1.25-1.25 \le x \le 1.25, inside (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right). They are the graphs of y=sec⁡xy = \sec x, y=tan⁡xy = \tan x and y=sec⁡xtan⁡xy = \sec x\tan x, in some order.

Two facts decide most of the questions without any computation: the derivative of an EVEN function is odd, the derivative of an ODD function is even, and where a curve has a horizontal tangent its derivative crosses zero.

-1.25-1-0.75-0.5-0.250.250.50.7511.25-4-3-2-11234ABC
  • a) Identify the curve of y=sec⁡xy = \sec x, of y=tan⁡xy = \tan x and of y=sec⁡xtan⁡xy = \sec x\tan x, with a reason for each.
  • b) One of the three curves is the derivative of another: which, and how does the figure confirm it? Of which curve is the derivative equal to the SQUARE of another?
  • c) Compute the slopes of BB and of CC at x=0x = 0, the second by the product rule. What do you notice about their tangent lines at the origin?
  • d) Find, by factoring, the point where AA and CC cross.
  • e) Using parity only, give the slope of AA at x=−π4x = -\frac{\pi}{4} from its slope at π4\frac{\pi}{4}, then confirm by a direct computation.

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  • a) AA is sec⁡x\sec x (even, value 11 at 00), BB is tan⁡x\tan x, CC is sec⁡xtan⁡x\sec x\tan x (odd, above BB for x>0x > 0).
  • b) C=A′C = A', since (sec⁡x)′=sec⁡xtan⁡x(\sec x)' = \sec x\tan x; and B′=sec⁡2x=A2B' = \sec^2 x = A^2.
  • c) Both slopes are 11: BB and CC share the tangent y=xy = x at the origin.
  • d) sec⁡x (tan⁡x−1)=0\sec x\,(\tan x - 1) = 0: (π4,2)\left(\frac{\pi}{4}, \sqrt 2\right)
  • e) −2-\sqrt 2

a) At x=0x = 0: sec⁡0=1\sec 0 = 1, tan⁡0=0\tan 0 = 0, sec⁡0tan⁡0=0\sec 0\tan 0 = 0. The only curve through (0,1)(0, 1) is AA, which is also symmetric about the yy-axis, as sec⁡x=1cos⁡x\sec x = \frac{1}{\cos x} is even: AA is sec⁡x\sec x. BB and CC both pass through the origin and are odd. To separate them, compare at π4\frac{\pi}{4}: tan⁡π4=1\tan\frac{\pi}{4} = 1 while sec⁡π4tan⁡π4=2>1\sec\frac{\pi}{4}\tan\frac{\pi}{4} = \sqrt 2 > 1. For 0<x<π20 < x < \frac{\pi}{2}, sec⁡x>1\sec x > 1, so sec⁡xtan⁡x>tan⁡x\sec x\tan x > \tan x: the steeper curve CC is sec⁡xtan⁡x\sec x\tan x, and BB is tan⁡x\tan x.

b) (sec⁡x)′=sec⁡xtan⁡x(\sec x)' = \sec x\tan x: CC is the derivative of AA. The figure agrees: AA is flat at its lowest point x=0x = 0, exactly where CC crosses zero; to the left AA falls and CC is below the axis, to the right AA rises and CC is above; the steeper AA gets near the edges, the larger ∣C∣|C| is. And (tan⁡x)′=sec⁡2x=(sec⁡x)2(\tan x)' = \sec^2 x = (\sec x)^2: the derivative of BB is the square of AA. An even function (AA) has an odd derivative (CC), an odd function (BB) an even one (A2A^2).

c) BB: (tan⁡x)′=sec⁡2x(\tan x)' = \sec^2 x, which is 11 at 00. CC: product rule with u=sec⁡xu = \sec x, v=tan⁡xv = \tan x: (sec⁡xtan⁡x)′=sec⁡xtan⁡x⋅tan⁡x+sec⁡x⋅sec⁡2x=sec⁡xtan⁡2x+sec⁡3x(\sec x\tan x)' = \sec x\tan x\cdot\tan x + \sec x\cdot\sec^2 x = \sec x\tan^2 x + \sec^3 x, which is 0+1=10 + 1 = 1 at 00. Both curves pass through the origin with slope 11: they have the SAME tangent line there, y=xy = x, and only separate further out, CC bending up faster. On the figure the two curves are practically indistinguishable near the origin.

d) sec⁡x=sec⁡xtan⁡x  ⟺  sec⁡xtan⁡x−sec⁡x=0  ⟺  sec⁡x (tan⁡x−1)=0\sec x = \sec x\tan x \iff \sec x\tan x - \sec x = 0 \iff \sec x\,(\tan x - 1) = 0. The factor sec⁡x\sec x is never 00, so tan⁡x=1\tan x = 1, and on the interval x=π4x = \frac{\pi}{4}, where y=sec⁡π4=2y = \sec\frac{\pi}{4} = \sqrt 2. The crossing point is (π4,2)\left(\frac{\pi}{4}, \sqrt 2\right), about (0.785,1.414)(0.785, 1.414) on the figure. Here dividing by sec⁡x\sec x would be legitimate, but only because it never vanishes, and the factored form is what shows it.

e) AA is even, so its derivative is odd: the slope at −π4-\frac{\pi}{4} is the opposite of the slope at π4\frac{\pi}{4}. At π4\frac{\pi}{4} the slope is sec⁡π4tan⁡π4=2\sec\frac{\pi}{4}\tan\frac{\pi}{4} = \sqrt 2, so at −π4-\frac{\pi}{4} it is −2-\sqrt 2. Directly: sec⁡(−π4)=2\sec\left(-\frac{\pi}{4}\right) = \sqrt 2 and tan⁡(−π4)=−1\tan\left(-\frac{\pi}{4}\right) = -1, product −2-\sqrt 2. Symmetry is a free check on any derivative of an even or odd function.

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, support the correction with a counterexample or a computation, and write the correct statement. A scientific calculator is allowed, as on the exam.

  • a) (cot⁡x)′=−csc⁡xcot⁡x(\cot x)' = -\csc x\cot x, the same pattern as (csc⁡x)′(\csc x)'.
  • b) (tan⁡x)′′=(sec⁡2x)′=2sec⁡x(\tan x)'' = (\sec^2 x)' = 2\sec x, by the power rule.
  • c) With my calculator, the slope of y=sin⁡xy = \sin x at x=2x = 2 is cos⁡2=0.9994\cos 2 = 0.9994.
  • d) For y=tan⁡x−2xy = \tan x - 2x on [0,2π][0, 2\pi]: y′=sec⁡2x−2=0y' = \sec^2 x - 2 = 0 gives cos⁡2x=12\cos^2 x = \frac{1}{2}, so cos⁡x=22\cos x = \frac{\sqrt 2}{2}, and my calculator gives x=0.7854x = 0.7854. There is one horizontal tangent.
  • e) sin⁡x+tan⁡xsin⁡x=1+tan⁡x\frac{\sin x + \tan x}{\sin x} = 1 + \tan x, so its derivative is sec⁡2x\sec^2 x.

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  • a) False: (cot⁡x)′=−csc⁡2x(\cot x)' = -\csc^2 x.
  • b) False: sec⁡2x=sec⁡x⋅sec⁡x\sec^2 x = \sec x\cdot\sec x, and (tan⁡x)′′=2sec⁡2xtan⁡x(\tan x)'' = 2\sec^2 x\tan x.
  • c) False: the calculator was in degrees; cos⁡2≈−0.4161\cos 2 \approx -0.4161 in radians.
  • d) False: cos⁡x=±22\cos x = \pm\frac{\sqrt 2}{2} gives four points, x=π4,3π4,5π4,7π4x = \frac{\pi}{4}, \frac{3\pi}{4}, \frac{5\pi}{4}, \frac{7\pi}{4}.
  • e) False: tan⁡xsin⁡x=sec⁡x\frac{\tan x}{\sin x} = \sec x, so the function is 1+sec⁡x1 + \sec x and its derivative sec⁡xtan⁡x\sec x\tan x.

a) FALSE. cot⁡x=cos⁡xsin⁡x\cot x = \frac{\cos x}{\sin x}, and the quotient rule gives (cot⁡x)′=−sin⁡x⋅sin⁡x−cos⁡x⋅cos⁡xsin⁡2x=−1sin⁡2x=−csc⁡2x(\cot x)' = \frac{-\sin x\cdot\sin x - \cos x\cdot\cos x}{\sin^2 x} = \frac{-1}{\sin^2 x} = -\csc^2 x. Counterexample to the student's formula: at π2\frac{\pi}{2} it gives −csc⁡π2cot⁡π2=−1⋅0=0-\csc\frac{\pi}{2}\cot\frac{\pi}{2} = -1\cdot 0 = 0, a horizontal tangent, while cot⁡x\cot x crosses the axis there with slope −csc⁡2π2=−1-\csc^2\frac{\pi}{2} = -1. Correct statement: (cot⁡x)′=−csc⁡2x(\cot x)' = -\csc^2 x pairs with (tan⁡x)′=sec⁡2x(\tan x)' = \sec^2 x, and (csc⁡x)′=−csc⁡xcot⁡x(\csc x)' = -\csc x\cot x pairs with (sec⁡x)′=sec⁡xtan⁡x(\sec x)' = \sec x\tan x. The pairs never cross.

b) FALSE. The power rule is about xnx^n, a power of the VARIABLE; sec⁡2x\sec^2 x is a power of a function. Before the chain rule, write it as a product: (sec⁡x⋅sec⁡x)′=sec⁡xtan⁡x⋅sec⁡x+sec⁡x⋅sec⁡xtan⁡x=2sec⁡2xtan⁡x(\sec x\cdot\sec x)' = \sec x\tan x\cdot\sec x + \sec x\cdot\sec x\tan x = 2\sec^2 x\tan x. Counterexample: at x=0x = 0 the student gets 2sec⁡0=22\sec 0 = 2, but tan⁡x\tan x is odd, so (tan⁡x)′(\tan x)' is even and (tan⁡x)′′(\tan x)'' is odd, hence 00 at 00; indeed 2sec⁡20tan⁡0=02\sec^2 0\tan 0 = 0. Correct statement: (tan⁡x)′′=2sec⁡2xtan⁡x(\tan x)'' = 2\sec^2 x\tan x.

c) FALSE. 0.99940.9994 is cos⁡(2∘)\cos(2^\circ): the calculator was in DEGREE mode. Every formula of the chapter, (sin⁡x)′=cos⁡x(\sin x)' = \cos x included, assumes xx in radians. In radian mode, cos⁡2≈−0.4161\cos 2 \approx -0.4161. Sanity check without any calculator: 22 is between π2≈1.57\frac{\pi}{2} \approx 1.57 and π\pi, where sine is coming down from its top, so the slope must be NEGATIVE. Correct statement: the slope of y=sin⁡xy = \sin x at x=2x = 2 is cos⁡2≈−0.4161\cos 2 \approx -0.4161, calculator in radians. Set the mode before the exam starts, and test it: cos⁡π\cos\pi must display −1-1.

d) FALSE. From cos⁡2x=12\cos^2 x = \frac{1}{2} the square root gives cos⁡x=±22\cos x = \pm\frac{\sqrt 2}{2}, not only the positive value, and on [0,2π][0, 2\pi] each value is taken TWICE. cos⁡x=22\cos x = \frac{\sqrt 2}{2} at π4\frac{\pi}{4} and 7π4\frac{7\pi}{4}; cos⁡x=−22\cos x = -\frac{\sqrt 2}{2} at 3π4\frac{3\pi}{4} and 5π4\frac{5\pi}{4}. None of the four is an asymptote π2\frac{\pi}{2} or 3π2\frac{3\pi}{2}, so all are in the domain. The calculator's cos⁡−1\cos^{-1} returns ONE angle, in [0,π][0, \pi]: the others come from the unit circle. Correct statement: y=tan⁡x−2xy = \tan x - 2x has four horizontal tangents on [0,2π][0, 2\pi], at x=π4,3π4,5π4,7π4x = \frac{\pi}{4}, \frac{3\pi}{4}, \frac{5\pi}{4}, \frac{7\pi}{4}.

e) FALSE. Dividing a sum by sin⁡x\sin x divides EACH term: sin⁡xsin⁡x+tan⁡xsin⁡x=1+sin⁡xcos⁡x⋅1sin⁡x=1+sec⁡x\frac{\sin x}{\sin x} + \frac{\tan x}{\sin x} = 1 + \frac{\sin x}{\cos x}\cdot\frac{1}{\sin x} = 1 + \sec x, for sin⁡x≠0\sin x \ne 0, cos⁡x≠0\cos x \ne 0. The student cancelled sin⁡x\sin x against one term only. The derivative is sec⁡xtan⁡x\sec x\tan x. Counterexample at π4\frac{\pi}{4}: the value of the function is 2/2+12/2=1+2\frac{\sqrt 2/2 + 1}{\sqrt 2/2} = 1 + \sqrt 2, not 1+tan⁡π4=21 + \tan\frac{\pi}{4} = 2; the true slope is 2\sqrt 2, not 22. Correct statement: sin⁡x+tan⁡xsin⁡x=1+sec⁡x\frac{\sin x + \tan x}{\sin x} = 1 + \sec x, with derivative sec⁡xtan⁡x\sec x\tan x.

Exercise 9: A Ferris wheel: height, vertical velocity and the equation y'' + y = 0

A Ferris wheel of radius 2020 m has its centre CC at 2222 m above the ground. It turns at a constant 11 radian per minute, so one turn takes 2π≈6.282\pi \approx 6.28 minutes. A rider boards at the lowest point BB at time t=0t = 0. After tt minutes the angle BCPBCP between the downward vertical and the rider's position PP is tt radians, as in the figure.

The rider's height above the ground and horizontal position, measured from the vertical line through CC, are then h(t)=22−20cos⁡th(t) = 22 - 20\cos t and x(t)=20sin⁡tx(t) = 20\sin t, in metres. Give exact values where they are natural; when a decimal is asked, round as stated, calculator in RADIAN mode.

CPBt20 mh(t)ground
  • a) Find h(0)h(0), the vertical velocity h′(t)h'(t) and h′(π6)h'\left(\frac{\pi}{6}\right), with units. What does the sign of h′(π6)h'\left(\frac{\pi}{6}\right) say?
  • b) Find h′′(t)h''(t). Show that y(t)=h(t)−22y(t) = h(t) - 22 satisfies y′′+y=0y'' + y = 0, and say what yy measures.
  • c) During the first turn, when is the rider rising fastest, and at what height? When is the vertical velocity zero, and where is the rider then?
  • d) Find the horizontal velocity x′(t)x'(t) and show that the speed x′(t)2+h′(t)2\sqrt{x'(t)^2 + h'(t)^2} is constant. Explain its value.
  • e) At t=2t = 2 min, find h(2)h(2), h′(2)h'(2) and h′′(2)h''(2) to two decimals. Is the rider going up or down, and is the vertical velocity increasing or decreasing? What would a calculator in degree mode give for h(2)h(2)?

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  • a) h(0)=2h(0) = 2 m; h′(t)=20sin⁡th'(t) = 20\sin t m/min; h′(π6)=10h'\left(\frac{\pi}{6}\right) = 10 m/min, rising.
  • b) h′′(t)=20cos⁡t=−(h−22)h''(t) = 20\cos t = -(h - 22), so y′′=−yy'' = -y; yy is the height above the centre.
  • c) Fastest rise 2020 m/min at t=π2≈1.57t = \frac{\pi}{2} \approx 1.57 min, at 2222 m; h′=0h' = 0 at t=0t = 0 (bottom, 22 m) and t=πt = \pi (top, 4242 m).
  • d) x′(t)=20cos⁡tx'(t) = 20\cos t; speed =20cos⁡2t+sin⁡2t=20= 20\sqrt{\cos^2 t + \sin^2 t} = 20 m/min =20= 20 m × 1\times\, 1 rad/min.
  • e) h(2)≈30.32h(2) \approx 30.32 m, h′(2)≈18.19h'(2) \approx 18.19 m/min, h′′(2)≈−8.32h''(2) \approx -8.32 m/min²: going up, vertical velocity decreasing. Degree mode: 2.012.01 m.

a) h(0)=22−20cos⁡0=2h(0) = 22 - 20\cos 0 = 2 m: the lowest seat is 22 m above the ground. By the constant multiple rule, h′(t)=−20(−sin⁡t)=20sin⁡th'(t) = -20(-\sin t) = 20\sin t, in metres per minute. At π6\frac{\pi}{6}: h′=20⋅12=10h' = 20\cdot\frac{1}{2} = 10 m/min. It is positive: the rider is rising at 1010 m per minute half a radian after boarding. Once more the minus in front of cos⁡t\cos t meets the minus of (cos⁡t)′(\cos t)'.

b) h′′(t)=20cos⁡th''(t) = 20\cos t, in metres per minute per minute. With y=h−22=−20cos⁡ty = h - 22 = -20\cos t: y′′=h′′=20cos⁡t=−yy'' = h'' = 20\cos t = -y, so y′′+y=0y'' + y = 0. The quantity yy is the height of the rider ABOVE THE CENTRE of the wheel, negative on the lower half. The constant 2222 disappears in y′′y'' but not in yy: that is why hh itself does not satisfy h′′+h=0h'' + h = 0, since h′′+h=22h'' + h = 22. Only the displacement from the centre oscillates in the pure form of this chapter.

c) h′(t)=20sin⁡t≤20h'(t) = 20\sin t \le 20, with equality exactly when sin⁡t=1\sin t = 1, that is t=π2≈1.57t = \frac{\pi}{2} \approx 1.57 min in the first turn. The rider then rises at 2020 m/min, at height h(π2)=22−0=22h\left(\frac{\pi}{2}\right) = 22 - 0 = 22 m, level with the centre, on the rising side of the wheel. No extremum theorem is needed: the bound ∣sin⁡t∣≤1|\sin t| \le 1 settles it. The vertical velocity is zero when sin⁡t=0\sin t = 0: t=0t = 0, at the bottom, 22 m, and t=π≈3.14t = \pi \approx 3.14 min, at the top, h(π)=22+20=42h(\pi) = 22 + 20 = 42 m. At both ends of the diameter the rider moves horizontally.

d) x′(t)=20cos⁡tx'(t) = 20\cos t m/min. Then x′(t)2+h′(t)2=400cos⁡2t+400sin⁡2t=400(cos⁡2t+sin⁡2t)=400x'(t)^2 + h'(t)^2 = 400\cos^2 t + 400\sin^2 t = 400(\cos^2 t + \sin^2 t) = 400, and the speed is 400=20\sqrt{400} = 20 m/min at every instant. It is the radius times the angular rate: 2020 m ×1\times 1 rad/min, the length of arc covered per minute. The Pythagorean identity is exactly the statement that a point moving on a circle at a constant angular rate has a constant speed; only the split between its horizontal and vertical parts changes.

e) Radian mode: cos⁡2≈−0.41615\cos 2 \approx -0.41615 and sin⁡2≈0.90930\sin 2 \approx 0.90930. So h(2)=22−20cos⁡2≈30.32h(2) = 22 - 20\cos 2 \approx 30.32 m, h′(2)=20sin⁡2≈18.19h'(2) = 20\sin 2 \approx 18.19 m/min, h′′(2)=20cos⁡2≈−8.32h''(2) = 20\cos 2 \approx -8.32 m/min². Since 2>π22 > \frac{\pi}{2}, the rider is on the upper half, past the level of the centre. h′(2)>0h'(2) > 0: still going UP. h′′(2)<0h''(2) < 0: the vertical velocity is DECREASING, it will reach 00 at the top, at t=πt = \pi. In degree mode the calculator computes cos⁡(2∘)≈0.99939\cos(2^\circ) \approx 0.99939 and gives h≈2.01h \approx 2.01 m, a rider who has barely left the boarding platform after two minutes: an answer that the picture refutes at once.

Exercise 10: A final exam question: the function sec x + tan x

Let f(x)=sec⁡x+tan⁡xf(x) = \sec x + \tan x on (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right); its graph is shown in the figure. This is the shape of a long final exam question: every step is an identity or a rule, named, and every value is exact. The whole question turns on one algebraic gesture, the conjugate 1−sin⁡x1 - \sin x.

-π/2π/2234sec x + tan x
  • a) Show that f(x)=1+sin⁡xcos⁡xf(x) = \frac{1 + \sin x}{\cos x}, then, multiplying by the conjugate, that f(x)=cos⁡x1−sin⁡xf(x) = \frac{\cos x}{1 - \sin x}. Deduce that f(x)>0f(x) > 0 on the interval, and give f(0)f(0).
  • b) Compute f′(x)f'(x) and show that f′(x)=sec⁡x⋅f(x)f'(x) = \sec x\cdot f(x). Find f′(0)f'(0).
  • c) Deduce from a) and b) that f′(x)=11−sin⁡xf'(x) = \frac{1}{1 - \sin x}. Show that f′(x)>12f'(x) > \frac{1}{2} on the interval: can the graph have a horizontal tangent?
  • d) Find f′′(x)f''(x) from the form of c), and show that f′′(x)=f(x) f′(x)f''(x) = f(x)\,f'(x). Find f′′(0)f''(0).
  • e) Find the point where the tangent has slope 22, the equation of that tangent, and its yy-intercept.

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Answers

  • a) f(x)=1+sin⁡xcos⁡x=cos⁡x1−sin⁡x>0f(x) = \frac{1 + \sin x}{\cos x} = \frac{\cos x}{1 - \sin x} > 0; f(0)=1f(0) = 1
  • b) f′(x)=sec⁡xtan⁡x+sec⁡2x=sec⁡x (tan⁡x+sec⁡x)f'(x) = \sec x\tan x + \sec^2 x = \sec x\,(\tan x + \sec x); f′(0)=1f'(0) = 1
  • c) f′(x)=11−sin⁡x>12f'(x) = \frac{1}{1 - \sin x} > \frac{1}{2}: no horizontal tangent.
  • d) f′′(x)=cos⁡x(1−sin⁡x)2=f(x)f′(x)f''(x) = \frac{\cos x}{(1 - \sin x)^2} = f(x)f'(x); f′′(0)=1f''(0) = 1
  • e) (π6,3)\left(\frac{\pi}{6}, \sqrt 3\right); y=2x+3−π3y = 2x + \sqrt 3 - \frac{\pi}{3}, intercept 3−π3\sqrt 3 - \frac{\pi}{3}

a) sec⁡x+tan⁡x=1cos⁡x+sin⁡xcos⁡x=1+sin⁡xcos⁡x\sec x + \tan x = \frac{1}{\cos x} + \frac{\sin x}{\cos x} = \frac{1 + \sin x}{\cos x}. Multiply top and bottom by the conjugate 1−sin⁡x1 - \sin x, which is positive on the interval because sin⁡x<1\sin x < 1 there: (1+sin⁡x)(1−sin⁡x)cos⁡x (1−sin⁡x)=1−sin⁡2xcos⁡x (1−sin⁡x)=cos⁡2xcos⁡x (1−sin⁡x)=cos⁡x1−sin⁡x\frac{(1 + \sin x)(1 - \sin x)}{\cos x\,(1 - \sin x)} = \frac{1 - \sin^2 x}{\cos x\,(1 - \sin x)} = \frac{\cos^2 x}{\cos x\,(1 - \sin x)} = \frac{\cos x}{1 - \sin x}, cancelling the factor cos⁡x≠0\cos x \ne 0. On (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right), cos⁡x>0\cos x > 0 and 1+sin⁡x>01 + \sin x > 0, so f(x)>0f(x) > 0. And f(0)=1+01=1f(0) = \frac{1 + 0}{1} = 1. The conjugate turns 1+sin⁡x1 + \sin x into cos⁡2x\cos^2 x: the same gesture as with a square root.

b) By the sum rule, f′(x)=sec⁡xtan⁡x+sec⁡2xf'(x) = \sec x\tan x + \sec^2 x. Factor the common sec⁡x\sec x: f′(x)=sec⁡x (tan⁡x+sec⁡x)=sec⁡x⋅f(x)f'(x) = \sec x\,(\tan x + \sec x) = \sec x\cdot f(x). At 00: f′(0)=1⋅1=1f'(0) = 1\cdot 1 = 1. Factoring is what reveals the function inside its own derivative.

c) With the second form of a): f′(x)=1cos⁡x⋅cos⁡x1−sin⁡x=11−sin⁡xf'(x) = \frac{1}{\cos x}\cdot\frac{\cos x}{1 - \sin x} = \frac{1}{1 - \sin x}, cancelling cos⁡x≠0\cos x \ne 0. On the interval −1<sin⁡x<1-1 < \sin x < 1, so 0<1−sin⁡x<20 < 1 - \sin x < 2 and f′(x)=11−sin⁡x>12f'(x) = \frac{1}{1 - \sin x} > \frac{1}{2}. The derivative is never 00: the graph has no horizontal tangent, every tangent line rises with slope greater than 12\frac{1}{2}. Check at 00: 11−0=1\frac{1}{1 - 0} = 1, as in b).

d) Quotient rule on 11−sin⁡x\frac{1}{1 - \sin x}, with u=1u = 1, u′=0u' = 0, v=1−sin⁡xv = 1 - \sin x, v′=−cos⁡xv' = -\cos x: f′′(x)=0⋅(1−sin⁡x)−1⋅(−cos⁡x)(1−sin⁡x)2=cos⁡x(1−sin⁡x)2f''(x) = \frac{0\cdot(1 - \sin x) - 1\cdot(-\cos x)}{(1 - \sin x)^2} = \frac{\cos x}{(1 - \sin x)^2}. And f(x)f′(x)=cos⁡x1−sin⁡x⋅11−sin⁡x=cos⁡x(1−sin⁡x)2=f′′(x)f(x)f'(x) = \frac{\cos x}{1 - \sin x}\cdot\frac{1}{1 - \sin x} = \frac{\cos x}{(1 - \sin x)^2} = f''(x). At 00: f′′(0)=11=1f''(0) = \frac{1}{1} = 1. Differentiating the simplified form of c) takes one line; differentiating sec⁡xtan⁡x+sec⁡2x\sec x\tan x + \sec^2 x directly takes two product rules and an identity.

e) f′(x)=2  ⟺  11−sin⁡x=2  ⟺  1−sin⁡x=12  ⟺  sin⁡x=12f'(x) = 2 \iff \frac{1}{1 - \sin x} = 2 \iff 1 - \sin x = \frac{1}{2} \iff \sin x = \frac{1}{2}. On (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right) the only solution is x=π6x = \frac{\pi}{6}. There f(π6)=1+1/23/2=33=3f\left(\frac{\pi}{6}\right) = \frac{1 + 1/2}{\sqrt 3/2} = \frac{3}{\sqrt 3} = \sqrt 3. Tangent: y=3+2(x−π6)=2x+3−π3y = \sqrt 3 + 2\left(x - \frac{\pi}{6}\right) = 2x + \sqrt 3 - \frac{\pi}{3}, with yy-intercept 3−π3≈0.6849\sqrt 3 - \frac{\pi}{3} \approx 0.6849. The solution figure shows it, steeper than the tangent y=1+xy = 1 + x at the origin, as f′′>0f'' > 0 on (0,π6)\left(0, \frac{\pi}{6}\right) lets one expect.

-π/2π/2234sec x + tan xy = 1 + xslope 2

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

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