An iden­tity is an equa­tion that is true for every value of the vari­able for which both sides are defined. Trigonom­e­try rests on three iden­ti­ties, all com­ing from one fact, x2+y2=r2x^2 + y^2 = r^2. With them we can turn any ratio into any other, sim­plify com­pli­cated expres­sions and prove new results. This les­son proves the three iden­ti­ties, rearranges them into the forms used most often, and works through prob­lems that depend on them.

The three fun­da­men­tal iden­ti­ties

Let P(x,y)P(x, y) be on the ter­mi­nal side of θ\theta with OP=rOP = r, so x2+y2=r2x^2 + y^2 = r^2.

Iden­tity 1. Divide x2+y2=r2x^2 + y^2 = r^2 by r2r^2:

(xr)2+(yr)2=1  ⟹  sin⁡2θ+cos⁡2θ=1\displaystyle \left(\frac{x}{r}\right)^2 + \left(\frac{y}{r}\right)^2 = 1 \implies \sin^2\theta + \cos^2\theta = 1

Iden­tity 2. Divide by x2x^2 (when x≠0x \neq 0): 1+(yx)2=(rx)2\displaystyle 1 + \left(\frac{y}{x}\right)^2 = \left(\frac{r}{x}\right)^2, so

sec⁡2θ−tan⁡2θ=1\sec^2\theta - \tan^2\theta = 1

Iden­tity 3. Divide by y2y^2 (when y≠0y \neq 0): (xy)2+1=(ry)2\displaystyle \left(\frac{x}{y}\right)^2 + 1 = \left(\frac{r}{y}\right)^2, so

csc⁡2θ−cot⁡2θ=1\csc^2\theta - \cot^2\theta = 1

(Here sin⁡2θ\sin^2\theta means (sin⁡θ)2(\sin\theta)^2.)

Use­ful forms

From Iden­tity 1:

sin⁡2θ=1−cos⁡2θ,cos⁡2θ=1−sin⁡2θ,sin⁡θ=±1−cos⁡2θ,cos⁡θ=±1−sin⁡2θ\sin^2\theta = 1 - \cos^2\theta, \quad \cos^2\theta = 1 - \sin^2\theta, \quad \sin\theta = \pm\sqrt{1 - \cos^2\theta}, \quad \cos\theta = \pm\sqrt{1 - \sin^2\theta}

(The sign comes from the quad­rant, as we will see; recall that x2=ax^2 = a gives x=±ax = \pm\sqrt{a}.)

From Iden­tity 2: sec⁡2θ=1+tan⁡2θ\sec^2\theta = 1 + \tan^2\theta and tan⁡2θ=sec⁡2θ−1\tan^2\theta = \sec^2\theta - 1. Fac­toris­ing the dif­fer­ence of squares,

(sec⁡θ−tan⁡θ)(sec⁡θ+tan⁡θ)=1,sosec⁡θ−tan⁡θ=1sec⁡θ+tan⁡θ\displaystyle (\sec\theta - \tan\theta)(\sec\theta + \tan\theta) = 1, \quad \text{so} \quad \sec\theta - \tan\theta = \frac{1}{\sec\theta + \tan\theta}

From Iden­tity 3 in the same way: csc⁡2θ=1+cot⁡2θ\csc^2\theta = 1 + \cot^2\theta, cot⁡2θ=csc⁡2θ−1\cot^2\theta = \csc^2\theta - 1, and

csc⁡θ−cot⁡θ=1csc⁡θ+cot⁡θ\displaystyle \csc\theta - \cot\theta = \frac{1}{\csc\theta + \cot\theta}

Exam­ple 1

If sec⁡θ+tan⁡θ=4\sec\theta + \tan\theta = 4, find sec⁡θ\sec\theta, tan⁡θ\tan\theta and sin⁡θ\sin\theta.

sec⁡θ−tan⁡θ=14\displaystyle \sec\theta - \tan\theta = \frac{1}{4}. Adding the two equa­tions: 2sec⁡θ=4+14=174\displaystyle 2\sec\theta = 4 + \frac{1}{4} = \frac{17}{4}, so sec⁡θ=178\displaystyle \sec\theta = \frac{17}{8}. Sub­tract­ing: 2tan⁡θ=154\displaystyle 2\tan\theta = \frac{15}{4}, so tan⁡θ=158\displaystyle \tan\theta = \frac{15}{8}.

sin⁡θ=tan⁡θsec⁡θ=15/817/8=1517\displaystyle \sin\theta = \frac{\tan\theta}{\sec\theta} = \frac{15/8}{17/8} = \frac{15}{17}

Higher pow­ers of sine and cosine

Writ­ing s=sin⁡2θs = \sin^2\theta and c=cos⁡2θc = \cos^2\theta, so that s+c=1s + c = 1, three more results fol­low.

(i) sin⁡2θ+cos⁡4θ=cos⁡2θ+sin⁡4θ=1−sin⁡2θcos⁡2θ\sin^2\theta + \cos^4\theta = \cos^2\theta + \sin^4\theta = 1 - \sin^2\theta\cos^2\theta.

s+c2=s+c(1−s)=s+c−sc=1−scs + c^2 = s + c(1 - s) = s + c - sc = 1 - sc, and in the same way c+s2=1−scc + s^2 = 1 - sc.

(ii) sin⁡4θ+cos⁡4θ=1−2sin⁡2θcos⁡2θ\sin^4\theta + \cos^4\theta = 1 - 2\sin^2\theta\cos^2\theta.

s2+c2=(s+c)2−2sc=1−2scs^2 + c^2 = (s + c)^2 - 2sc = 1 - 2sc.

(iii) sin⁡6θ+cos⁡6θ=1−3sin⁡2θcos⁡2θ\sin^6\theta + \cos^6\theta = 1 - 3\sin^2\theta\cos^2\theta.

s3+c3=(s+c)3−3sc(s+c)=1−3scs^3 + c^3 = (s + c)^3 - 3sc(s + c) = 1 - 3sc.

Exam­ple 2

If un=cos⁡nθ+sin⁡nθu_n = \cos^n\theta + \sin^n\theta, find 2u6−3u42u_6 - 3u_4.

Using (ii) and (iii):

2u6−3u4=2(1−3sin⁡2θcos⁡2θ)−3(1−2sin⁡2θcos⁡2θ)=2−3=−12u_6 - 3u_4 = 2(1 - 3\sin^2\theta\cos^2\theta) - 3(1 - 2\sin^2\theta\cos^2\theta) = 2 - 3 = -1

The terms in sin⁡2θcos⁡2θ\sin^2\theta\cos^2\theta can­cel, so the answer is −1-1 for every θ\theta.

Exam­ple 3

If sin⁡θ+cos⁡θ=75\displaystyle \sin\theta + \cos\theta = \frac{7}{5}, find sin⁡θcos⁡θ\sin\theta\cos\theta and sin⁡4θ+cos⁡4θ\sin^4\theta + \cos^4\theta.

Square: sin⁡2θ+2sin⁡θcos⁡θ+cos⁡2θ=4925\displaystyle \sin^2\theta + 2\sin\theta\cos\theta + \cos^2\theta = \frac{49}{25}, so 1+2sin⁡θcos⁡θ=4925\displaystyle 1 + 2\sin\theta\cos\theta = \frac{49}{25} and sin⁡θcos⁡θ=1225\displaystyle \sin\theta\cos\theta = \frac{12}{25}.

sin⁡4θ+cos⁡4θ=1−2(1225)2=1−288625=337625\displaystyle \sin^4\theta + \cos^4\theta = 1 - 2\left(\frac{12}{25}\right)^2 = 1 - \frac{288}{625} = \frac{337}{625}

Exam­ple 4

If tan⁡θ=p−14p\displaystyle \tan\theta = p - \frac{1}{4p}, find sec⁡θ−tan⁡θ\sec\theta - \tan\theta.

sec⁡2θ=1+(p−14p)2=1+p2−12+116p2=p2+12+116p2=(p+14p)2\displaystyle \sec^2\theta = 1 + \left(p - \frac{1}{4p}\right)^2 = 1 + p^2 - \frac{1}{2} + \frac{1}{16p^2} = p^2 + \frac{1}{2} + \frac{1}{16p^2} = \left(p + \frac{1}{4p}\right)^2

So sec⁡θ=±(p+14p)\displaystyle \sec\theta = \pm\left(p + \frac{1}{4p}\right), and

sec⁡θ−tan⁡θ=(p+14p)−(p−14p)=12por−(p+14p)−(p−14p)=−2p\displaystyle \sec\theta - \tan\theta = \left(p + \frac{1}{4p}\right) - \left(p - \frac{1}{4p}\right) = \frac{1}{2p} \quad \text{or} \quad -\left(p + \frac{1}{4p}\right) - \left(p - \frac{1}{4p}\right) = -2p

Exam­ple 5

If tan⁡2θ=1−k2\tan^2\theta = 1 - k^2, find sec⁡θ+tan⁡3θcsc⁡θ\sec\theta + \tan^3\theta\csc\theta.

Since tan⁡θcsc⁡θ=sin⁡θcos⁡θ×1sin⁡θ=sec⁡θ\displaystyle \tan\theta\csc\theta = \frac{\sin\theta}{\cos\theta} \times \frac{1}{\sin\theta} = \sec\theta,

sec⁡θ+tan⁡2θ⋅tan⁡θcsc⁡θ=sec⁡θ+tan⁡2θsec⁡θ=sec⁡θ(1+tan⁡2θ)=sec⁡3θ\sec\theta + \tan^2\theta \cdot \tan\theta\csc\theta = \sec\theta + \tan^2\theta\sec\theta = \sec\theta(1 + \tan^2\theta) = \sec^3\theta

and sec⁡2θ=1+tan⁡2θ=2−k2\sec^2\theta = 1 + \tan^2\theta = 2 - k^2, so the value is (2−k2)3/2(2 - k^2)^{3/2}.

Prov­ing iden­ti­ties

Start from the more com­pli­cated side and sim­plify it to the other side, using the iden­ti­ties and the rec­i­p­ro­cal and quo­tient rela­tions. Do not "cross over" terms from one side to the other as if solv­ing an equa­tion.

Exam­ple 6

Prove that (1−cos⁡2θ)(1+cot⁡2θ)=1(1 - \cos^2\theta)(1 + \cot^2\theta) = 1.

LHS=sin⁡2θ×csc⁡2θ=sin⁡2θ×1sin⁡2θ=1=RHS\displaystyle \text{LHS} = \sin^2\theta \times \csc^2\theta = \sin^2\theta \times \frac{1}{\sin^2\theta} = 1 = \text{RHS}

Prac­tice

  1. Prove that (1+tan⁡2θ)cos⁡2θ=1(1 + \tan^2\theta)\cos^2\theta = 1.
  2. Prove that sec⁡4θ−sec⁡2θ=tan⁡4θ+tan⁡2θ\sec^4\theta - \sec^2\theta = \tan^4\theta + \tan^2\theta.
  3. If sec⁡θ+tan⁡θ=5\sec\theta + \tan\theta = 5, find sec⁡θ−tan⁡θ\sec\theta - \tan\theta, sec⁡θ\sec\theta and tan⁡θ\tan\theta.
  4. If csc⁡θ+cot⁡θ=3\csc\theta + \cot\theta = 3, find cos⁡θ\cos\theta.
  5. If sin⁡θcos⁡θ=13\displaystyle \sin\theta\cos\theta = \frac{1}{3}, find sin⁡6θ+cos⁡6θ\sin^6\theta + \cos^6\theta.
  6. If sin⁡θ+cos⁡θ=75\displaystyle \sin\theta + \cos\theta = \frac{7}{5}, find sin⁡2θ+cos⁡4θ\sin^2\theta + \cos^4\theta.
  7. Prove that (sin⁡θ+csc⁡θ)2+(cos⁡θ+sec⁡θ)2=7+tan⁡2θ+cot⁡2θ(\sin\theta + \csc\theta)^2 + (\cos\theta + \sec\theta)^2 = 7 + \tan^2\theta + \cot^2\theta.
  8. Prove that 1sec⁡θ−tan⁡θ−1cos⁡θ=tan⁡θ\displaystyle \frac{1}{\sec\theta - \tan\theta} - \frac{1}{\cos\theta} = \tan\theta.

Answers

Show answers
  1. sec⁡2θcos⁡2θ=1\sec^2\theta \cos^2\theta = 1
  2. LHS =sec⁡2θ(sec⁡2θ−1)=(1+tan⁡2θ)tan⁡2θ=tan⁡2θ+tan⁡4θ= \sec^2\theta(\sec^2\theta - 1) = (1 + \tan^2\theta)\tan^2\theta = \tan^2\theta + \tan^4\theta
  3. 15\displaystyle \frac{1}{5}; adding, sec⁡θ=135\displaystyle \sec\theta = \frac{13}{5}; sub­tract­ing, tan⁡θ=125\displaystyle \tan\theta = \frac{12}{5}
  4. csc⁡θ−cot⁡θ=13\displaystyle \csc\theta - \cot\theta = \frac{1}{3}, so csc⁡θ=53\displaystyle \csc\theta = \frac{5}{3} and cot⁡θ=43\displaystyle \cot\theta = \frac{4}{3}; cos⁡θ=cot⁡θcsc⁡θ=45\displaystyle \cos\theta = \frac{\cot\theta}{\csc\theta} = \frac{4}{5}
  5. 1−3×19=23\displaystyle 1 - 3 \times \frac{1}{9} = \frac{2}{3}
  6. sin⁡θcos⁡θ=1225\displaystyle \sin\theta\cos\theta = \frac{12}{25} (Exam­ple 3), so 1−144625=481625\displaystyle 1 - \frac{144}{625} = \frac{481}{625}
  7. LHS =sin⁡2θ+2+csc⁡2θ+cos⁡2θ+2+sec⁡2θ=5+(1+cot⁡2θ)+(1+tan⁡2θ)=7+tan⁡2θ+cot⁡2θ= \sin^2\theta + 2 + \csc^2\theta + \cos^2\theta + 2 + \sec^2\theta = 5 + (1 + \cot^2\theta) + (1 + \tan^2\theta) = 7 + \tan^2\theta + \cot^2\theta
  8. 1sec⁡θ−tan⁡θ=sec⁡θ+tan⁡θ\displaystyle \frac{1}{\sec\theta - \tan\theta} = \sec\theta + \tan\theta, and sub­tract­ing 1cos⁡θ=sec⁡θ\displaystyle \frac{1}{\cos\theta} = \sec\theta leaves tan⁡θ\tan\theta.