This final les­son gath­ers the remain­ing ideas that make hard-look­ing prob­lems easy: a few rules from ratio and pro­por­tion, a dia­gram that cap­tures all the prod­uct rela­tions, some iden­ti­ties that are worth recog­nis­ing on sight, and the tech­nique of elim­i­nat­ing θ\theta, find­ing a rela­tion between quan­ti­ties that no longer involves the angle at all. It ends with cross-mul­ti­pli­ca­tion, which solves a pair of equa­tions in cos⁡θ\cos\theta and sin⁡θ\sin\theta at once.

Con­cept 5: ratio and pro­por­tion

If ab=cd\displaystyle \frac{a}{b} = \frac{c}{d}, then each ratio also equals

a+cb+d=la+mclb+md\displaystyle \frac{a + c}{b + d} = \frac{la + mc}{lb + md}

for any num­bers ll, mm (as long as the denom­i­na­tors are not zero). And the com­po­nendo and div­i­dendo rule gives

a+ba−b=c+dc−d\displaystyle \frac{a + b}{a - b} = \frac{c + d}{c - d}

Exam­ple 1

If sin⁡4θa+cos⁡4θb=1a+b\displaystyle \frac{\sin^4\theta}{a} + \frac{\cos^4\theta}{b} = \frac{1}{a + b}, find sin⁡8θa3+cos⁡8θb3\displaystyle \frac{\sin^8\theta}{a^3} + \frac{\cos^8\theta}{b^3}.

Write s=sin⁡2θs = \sin^2\theta, so cos⁡2θ=1−s\cos^2\theta = 1 - s. Mul­ti­ply­ing the given equa­tion by ab(a+b)ab(a + b):

b(a+b)s2+a(a+b)(1−s)2=abb(a + b)s^2 + a(a + b)(1 - s)^2 = ab

Expand­ing and col­lect­ing terms gives (a+b)2s2−2a(a+b)s+a2=0(a + b)^2 s^2 - 2a(a + b)s + a^2 = 0, that is,

((a+b)s−a)2=0  ⟹  s=aa+b,1−s=ba+b\displaystyle \big((a + b)s - a\big)^2 = 0 \implies s = \frac{a}{a + b}, \quad 1 - s = \frac{b}{a + b}

So sin⁡2θa=cos⁡2θb=1a+b\displaystyle \frac{\sin^2\theta}{a} = \frac{\cos^2\theta}{b} = \frac{1}{a + b} (the ratio rule above). Then

sin⁡8θa3=a(sin⁡2θa)4=a(a+b)4,cos⁡8θb3=b(a+b)4\displaystyle \frac{\sin^8\theta}{a^3} = a\left(\frac{\sin^2\theta}{a}\right)^4 = \frac{a}{(a + b)^4}, \qquad \frac{\cos^8\theta}{b^3} = \frac{b}{(a + b)^4}

and the sum is a+b(a+b)4=1(a+b)3\displaystyle \frac{a + b}{(a + b)^4} = \frac{1}{(a + b)^3}.

Con­cept 6: the prod­uct hexa­gon

Write the six ratios round a hexa­gon in this order: tan⁡θ\tan\theta, sin⁡θ\sin\theta, cos⁡θ\cos\theta, cot⁡θ\cot\theta, csc⁡θ\csc\theta, sec⁡θ\sec\theta. Then any ratio times the ratio two places fur­ther on gives the ratio between them:

Prod­uct Result
tan⁡θ⋅cos⁡θ\tan\theta \cdot \cos\theta sin⁡θ\sin\theta
sin⁡θ⋅cot⁡θ\sin\theta \cdot \cot\theta cos⁡θ\cos\theta
cos⁡θ⋅csc⁡θ\cos\theta \cdot \csc\theta cot⁡θ\cot\theta
cot⁡θ⋅sec⁡θ\cot\theta \cdot \sec\theta csc⁡θ\csc\theta
csc⁡θ⋅tan⁡θ\csc\theta \cdot \tan\theta sec⁡θ\sec\theta
sec⁡θ⋅sin⁡θ\sec\theta \cdot \sin\theta tan⁡θ\tan\theta

Each line is checked by writ­ing every­thing in sines and cosines; for exam­ple csc⁡θtan⁡θ=1sin⁡θ⋅sin⁡θcos⁡θ=sec⁡θ\displaystyle \csc\theta\tan\theta = \frac{1}{\sin\theta} \cdot \frac{\sin\theta}{\cos\theta} = \sec\theta.

Con­cept 7: iden­ti­ties to recog­nise

tan⁡2θ−sin⁡2θ=tan⁡2θsin⁡2θ,cot⁡2θ−cos⁡2θ=cot⁡2θcos⁡2θ\tan^2\theta - \sin^2\theta = \tan^2\theta\sin^2\theta, \qquad \cot^2\theta - \cos^2\theta = \cot^2\theta\cos^2\theta

sec⁡2θ+csc⁡2θ=sec⁡2θcsc⁡2θ,tan⁡θ+cot⁡θ=1sin⁡θcos⁡θ=csc⁡θsec⁡θ\displaystyle \sec^2\theta + \csc^2\theta = \sec^2\theta\csc^2\theta, \qquad \tan\theta + \cot\theta = \frac{1}{\sin\theta\cos\theta} = \csc\theta\sec\theta

For the first: tan⁡2θ−sin⁡2θ=sin⁡2θ(1cos⁡2θ−1)=sin⁡2θtan⁡2θ\displaystyle \tan^2\theta - \sin^2\theta = \sin^2\theta\left(\frac{1}{\cos^2\theta} - 1\right) = \sin^2\theta\tan^2\theta. The oth­ers are proved the same way.

Con­cept 8: elim­i­nat­ing θ

To elim­i­nate θ\theta from two equa­tions, com­bine them (usu­ally by adding, sub­tract­ing, squar­ing or mul­ti­ply­ing) so that an iden­tity such as sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1 removes θ\theta.

Exam­ple 2

If m=tan⁡θ+sin⁡θm = \tan\theta + \sin\theta and n=tan⁡θ−sin⁡θn = \tan\theta - \sin\theta, show that m2−n2=4mnm^2 - n^2 = 4\sqrt{mn} (for acute θ\theta).

m+n=2tan⁡θm + n = 2\tan\theta and m−n=2sin⁡θm - n = 2\sin\theta, so m2−n2=(m+n)(m−n)=4tan⁡θsin⁡θm^2 - n^2 = (m + n)(m - n) = 4\tan\theta\sin\theta.

Also mn=tan⁡2θ−sin⁡2θ=tan⁡2θsin⁡2θmn = \tan^2\theta - \sin^2\theta = \tan^2\theta\sin^2\theta (Con­cept 7), so mn=tan⁡θsin⁡θ\sqrt{mn} = \tan\theta\sin\theta. Hence m2−n2=4mnm^2 - n^2 = 4\sqrt{mn}.

Exam­ple 3

If asec⁡α+btan⁡α=1a\sec\alpha + b\tan\alpha = 1 and a2sec⁡2α−b2tan⁡2α=5a^2\sec^2\alpha - b^2\tan^2\alpha = 5, find 4a2−9b24a^2 - 9b^2 in terms of aa and bb.

The sec­ond equa­tion fac­torises: (asec⁡α−btan⁡α)(asec⁡α+btan⁡α)=5(a\sec\alpha - b\tan\alpha)(a\sec\alpha + b\tan\alpha) = 5, so asec⁡α−btan⁡α=5a\sec\alpha - b\tan\alpha = 5. Adding and sub­tract­ing with the first equa­tion:

2asec⁡α=6  ⟹  sec⁡α=3a,2btan⁡α=−4  ⟹  tan⁡α=−2b\displaystyle 2a\sec\alpha = 6 \implies \sec\alpha = \frac{3}{a}, \qquad 2b\tan\alpha = -4 \implies \tan\alpha = -\frac{2}{b}

Now sec⁡2α−tan⁡2α=1\sec^2\alpha - \tan^2\alpha = 1 gives 9a2−4b2=1\displaystyle \frac{9}{a^2} - \frac{4}{b^2} = 1, so 9b2−4a2=a2b29b^2 - 4a^2 = a^2b^2, that is,

4a2−9b2=−a2b24a^2 - 9b^2 = -a^2b^2

Exam­ple 4

If m=sin⁡θ+cos⁡θm = \sin\theta + \cos\theta and n=sec⁡θ+csc⁡θn = \sec\theta + \csc\theta, elim­i­nate θ\theta.

n=1cos⁡θ+1sin⁡θ=sin⁡θ+cos⁡θsin⁡θcos⁡θ=msin⁡θcos⁡θ\displaystyle n = \frac{1}{\cos\theta} + \frac{1}{\sin\theta} = \frac{\sin\theta + \cos\theta}{\sin\theta\cos\theta} = \frac{m}{\sin\theta\cos\theta}. Squar­ing mm: m2=1+2sin⁡θcos⁡θm^2 = 1 + 2\sin\theta\cos\theta, so sin⁡θcos⁡θ=m2−12\displaystyle \sin\theta\cos\theta = \frac{m^2 - 1}{2}. There­fore

n=2mm2−1,that is,n(m2−1)=2m\displaystyle n = \frac{2m}{m^2 - 1}, \quad \text{that is,} \quad n(m^2 - 1) = 2m

Exam­ple 5

If m=csc⁡θ−sin⁡θm = \csc\theta - \sin\theta and n=sec⁡θ−cos⁡θn = \sec\theta - \cos\theta, find (m2n)2/3+(mn2)2/3(m^2n)^{2/3} + (mn^2)^{2/3}.

m=1−sin⁡2θsin⁡θ=cos⁡2θsin⁡θ\displaystyle m = \frac{1 - \sin^2\theta}{\sin\theta} = \frac{\cos^2\theta}{\sin\theta} and n=1−cos⁡2θcos⁡θ=sin⁡2θcos⁡θ\displaystyle n = \frac{1 - \cos^2\theta}{\cos\theta} = \frac{\sin^2\theta}{\cos\theta}.

m2n=cos⁡4θsin⁡2θ⋅sin⁡2θcos⁡θ=cos⁡3θ,mn2=cos⁡2θsin⁡θ⋅sin⁡4θcos⁡2θ=sin⁡3θ\displaystyle m^2n = \frac{\cos^4\theta}{\sin^2\theta} \cdot \frac{\sin^2\theta}{\cos\theta} = \cos^3\theta, \qquad mn^2 = \frac{\cos^2\theta}{\sin\theta} \cdot \frac{\sin^4\theta}{\cos^2\theta} = \sin^3\theta

So the expres­sion is cos⁡2θ+sin⁡2θ=1\cos^2\theta + \sin^2\theta = 1.

Exam­ple 6

If asin⁡x=bcos⁡x=2ctan⁡x1−tan⁡2x\displaystyle a\sin x = b\cos x = \frac{2c\tan x}{1 - \tan^2 x}, find (a2−b2)2a2+b2\displaystyle \frac{(a^2 - b^2)^2}{a^2 + b^2}.

From asin⁡x=bcos⁡xa\sin x = b\cos x, tan⁡x=ba\displaystyle \tan x = \frac{b}{a}, so 2tan⁡x1−tan⁡2x=2b/a1−b2/a2=2aba2−b2\displaystyle \frac{2\tan x}{1 - \tan^2 x} = \frac{2b/a}{1 - b^2/a^2} = \frac{2ab}{a^2 - b^2}. Then bcos⁡x=2abca2−b2\displaystyle b\cos x = \frac{2abc}{a^2 - b^2}, so cos⁡x=2aca2−b2\displaystyle \cos x = \frac{2ac}{a^2 - b^2}. But tan⁡x=ba\displaystyle \tan x = \frac{b}{a} also gives cos⁡x=aa2+b2\displaystyle \cos x = \frac{a}{\sqrt{a^2 + b^2}} (tak­ing xx acute). Equat­ing,

aa2+b2=2aca2−b2  ⟹  a2−b2=2ca2+b2  ⟹  (a2−b2)2a2+b2=4c2\displaystyle \frac{a}{\sqrt{a^2 + b^2}} = \frac{2ac}{a^2 - b^2} \implies a^2 - b^2 = 2c\sqrt{a^2 + b^2} \implies \frac{(a^2 - b^2)^2}{a^2 + b^2} = 4c^2

Exam­ple 7

If sin⁡α\sin\alpha, sin⁡β\sin\beta, sin⁡γ\sin\gamma are in A.P. and cos⁡α\cos\alpha, cos⁡β\cos\beta, cos⁡γ\cos\gamma are in G.P., find cos⁡2α+cos⁡2γ−4cos⁡αcos⁡γ1−sin⁡αsin⁡γ\displaystyle \frac{\cos^2\alpha + \cos^2\gamma - 4\cos\alpha\cos\gamma}{1 - \sin\alpha\sin\gamma}.

A.P. gives 2sin⁡β=sin⁡α+sin⁡γ2\sin\beta = \sin\alpha + \sin\gamma; G.P. gives cos⁡2β=cos⁡αcos⁡γ\cos^2\beta = \cos\alpha\cos\gamma. So

4cos⁡αcos⁡γ=4cos⁡2β=4−4sin⁡2β=4−(sin⁡α+sin⁡γ)24\cos\alpha\cos\gamma = 4\cos^2\beta = 4 - 4\sin^2\beta = 4 - (\sin\alpha + \sin\gamma)^2

The numer­a­tor becomes (1−sin⁡2α)+(1−sin⁡2γ)−4+sin⁡2α+2sin⁡αsin⁡γ+sin⁡2γ=−2+2sin⁡αsin⁡γ=−2(1−sin⁡αsin⁡γ)(1 - \sin^2\alpha) + (1 - \sin^2\gamma) - 4 + \sin^2\alpha + 2\sin\alpha\sin\gamma + \sin^2\gamma = -2 + 2\sin\alpha\sin\gamma = -2(1 - \sin\alpha\sin\gamma). The value is −2-2.

Con­cept 9: cross-mul­ti­pli­ca­tion

For two equa­tions a1x+b1y+c1=0a_1x + b_1y + c_1 = 0 and a2x+b2y+c2=0a_2x + b_2y + c_2 = 0 (with a1b2−a2b1≠0a_1b_2 - a_2b_1 \neq 0),

xb1c2−b2c1=yc1a2−c2a1=1a1b2−a2b1\displaystyle \frac{x}{b_1c_2 - b_2c_1} = \frac{y}{c_1a_2 - c_2a_1} = \frac{1}{a_1b_2 - a_2b_1}

so x=b1c2−b2c1a1b2−a2b1\displaystyle x = \frac{b_1c_2 - b_2c_1}{a_1b_2 - a_2b_1} and y=c1a2−c2a1a1b2−a2b1\displaystyle y = \frac{c_1a_2 - c_2a_1}{a_1b_2 - a_2b_1}.

Exam­ple 8

Elim­i­nate θ\theta from a1cos⁡θ+b1sin⁡θ+c1=0a_1\cos\theta + b_1\sin\theta + c_1 = 0 and a2cos⁡θ+b2sin⁡θ+c2=0a_2\cos\theta + b_2\sin\theta + c_2 = 0.

Treat cos⁡θ\cos\theta as xx and sin⁡θ\sin\theta as yy:

cos⁡θ=b1c2−b2c1a1b2−a2b1,sin⁡θ=c1a2−c2a1a1b2−a2b1\displaystyle \cos\theta = \frac{b_1c_2 - b_2c_1}{a_1b_2 - a_2b_1}, \qquad \sin\theta = \frac{c_1a_2 - c_2a_1}{a_1b_2 - a_2b_1}

Since cos⁡2θ+sin⁡2θ=1\cos^2\theta + \sin^2\theta = 1,

(b1c2−b2c1)2+(c1a2−c2a1)2=(a1b2−a2b1)2(b_1c_2 - b_2c_1)^2 + (c_1a_2 - c_2a_1)^2 = (a_1b_2 - a_2b_1)^2

Prac­tice

  1. Prove that tan⁡2θ−sin⁡2θ=tan⁡2θsin⁡2θ\tan^2\theta - \sin^2\theta = \tan^2\theta\sin^2\theta.
  2. Prove that sec⁡2θ+csc⁡2θ=sec⁡2θcsc⁡2θ\sec^2\theta + \csc^2\theta = \sec^2\theta\csc^2\theta.
  3. Prove that cot⁡2θ−cos⁡2θ=cot⁡2θcos⁡2θ\cot^2\theta - \cos^2\theta = \cot^2\theta\cos^2\theta.
  4. Elim­i­nate θ\theta from x=acos⁡θx = a\cos\theta, y=bsin⁡θy = b\sin\theta.
  5. Elim­i­nate θ\theta from x=asec⁡θx = a\sec\theta, y=btan⁡θy = b\tan\theta.
  6. Elim­i­nate θ\theta from x=csc⁡θ+cot⁡θx = \csc\theta + \cot\theta, y=csc⁡θ−cot⁡θy = \csc\theta - \cot\theta.
  7. If cos⁡θ+sin⁡θ=2cos⁡θ\cos\theta + \sin\theta = \sqrt{2}\cos\theta, show that cos⁡θ−sin⁡θ=2sin⁡θ\cos\theta - \sin\theta = \sqrt{2}\sin\theta.
  8. Use the hexa­gon to sim­plify sec⁡θ⋅sin⁡θ⋅cot⁡θ\sec\theta \cdot \sin\theta \cdot \cot\theta.

Answers

Show answers
  1. tan⁡2θ−sin⁡2θ=sin⁡2θ(sec⁡2θ−1)=sin⁡2θtan⁡2θ\tan^2\theta - \sin^2\theta = \sin^2\theta\left(\sec^2\theta - 1\right) = \sin^2\theta\tan^2\theta
  2. 1cos⁡2θ+1sin⁡2θ=sin⁡2θ+cos⁡2θsin⁡2θcos⁡2θ=1sin⁡2θcos⁡2θ=sec⁡2θcsc⁡2θ\displaystyle \frac{1}{\cos^2\theta} + \frac{1}{\sin^2\theta} = \frac{\sin^2\theta + \cos^2\theta}{\sin^2\theta\cos^2\theta} = \frac{1}{\sin^2\theta\cos^2\theta} = \sec^2\theta\csc^2\theta
  3. cot⁡2θ−cos⁡2θ=cos⁡2θ(csc⁡2θ−1)=cos⁡2θcot⁡2θ\cot^2\theta - \cos^2\theta = \cos^2\theta\left(\csc^2\theta - 1\right) = \cos^2\theta\cot^2\theta
  4. xa=cos⁡θ\displaystyle \frac{x}{a} = \cos\theta and yb=sin⁡θ\displaystyle \frac{y}{b} = \sin\theta, so x2a2+y2b2=1\displaystyle \frac{x^2}{a^2} + \frac{y^2}{b^2} = 1.
  5. sec⁡2θ−tan⁡2θ=1\sec^2\theta - \tan^2\theta = 1 gives x2a2−y2b2=1\displaystyle \frac{x^2}{a^2} - \frac{y^2}{b^2} = 1.
  6. xy=csc⁡2θ−cot⁡2θ=1xy = \csc^2\theta - \cot^2\theta = 1
  7. sin⁡θ=(2−1)cos⁡θ\sin\theta = (\sqrt{2} - 1)\cos\theta, so cos⁡θ=sin⁡θ2−1=(2+1)sin⁡θ\displaystyle \cos\theta = \frac{\sin\theta}{\sqrt{2} - 1} = (\sqrt{2} + 1)\sin\theta. Then cos⁡θ−sin⁡θ=2sin⁡θ\cos\theta - \sin\theta = \sqrt{2}\sin\theta.
  8. sec⁡θsin⁡θ=tan⁡θ\sec\theta\sin\theta = \tan\theta, and tan⁡θcot⁡θ=1\tan\theta\cot\theta = 1: the prod­uct is 11.