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Mathematics · Ch 3 — Trigonometric Functions

Properties of Inverse Trigonometric Functions

3.3.8

Properties of Inverse Trigonometric Functions

Properties of Inverse Trigonometric Functions.

(i) If −1≤x≤1-1\le x\le1 and x≠0x\ne0 then sin⁡−1x=cosec−1(1x)\sin^{-1}x=\text{cosec}^{-1}\left(\dfrac1x\right).

Proof. By the conditions on xx, both sides are defined, and 1x∈R−(−1,1)\dfrac1x\in\mathbb{R}-(-1,1) — (1). Let sin⁡−1x=θ\sin^{-1}x=\theta; then θ∈[−π2,π2]\theta\in\left[-\dfrac{\pi}{2},\dfrac{\pi}{2}\right] and θ≠0\theta\ne0 (since x≠0x\ne0), so θ∈(−π2,π2)−{0}\theta\in\left(-\dfrac{\pi}{2},\dfrac{\pi}{2}\right)-\{0\} — (2). Also sin⁡θ=x  ⟹  cosec θ=1x\sin\theta=x\implies\text{cosec}\,\theta=\dfrac1x — (3). From (1),(2),(3), θ=cosec−1(1x)\theta=\text{cosec}^{-1}\left(\dfrac1x\right), so sin⁡−1x=cosec−1(1x)\sin^{-1}x=\text{cosec}^{-1}\left(\dfrac1x\right).

Similarly one can prove: (i)′' cos⁡−1x=sec⁡−1(1x)\cos^{-1}x=\sec^{-1}\left(\dfrac1x\right) if −1≤x≤1-1\le x\le1, x≠0x\ne0.

(ii) tan⁡−1x=cot⁡−1(1x)\tan^{-1}x=\cot^{-1}\left(\dfrac1x\right) if x>0x>0.

Proof. Let tan⁡−1x=θ\tan^{-1}x=\theta; θ∈(−π2,π2)\theta\in\left(-\dfrac{\pi}{2},\dfrac{\pi}{2}\right), and since x>0x>0, θ∈(0,π2)\theta\in\left(0,\dfrac{\pi}{2}\right). tan⁡θ=x  ⟹  cot⁡θ=1x\tan\theta=x\implies\cot\theta=\dfrac1x, where 1x∈R\dfrac1x\in\mathbb{R} — (1). Since θ∈(0,π2)⊂(0,π)\theta\in\left(0,\dfrac{\pi}{2}\right)\subset(0,\pi) — (2), from (1),(2): cot⁡−1(1x)=θ\cot^{-1}\left(\dfrac1x\right)=\theta, so tan⁡−1x=cot⁡−1(1x)\tan^{-1}x=\cot^{-1}\left(\dfrac1x\right).

(iii) Similarly, tan⁡−1x=−π+cot⁡−1(1x)\tan^{-1}x=-\pi+\cot^{-1}\left(\dfrac1x\right) if x<0x<0.

(iv) If −1≤x≤1-1\le x\le1 then sin⁡−1(−x)=−sin⁡−1(x)\sin^{-1}(-x)=-\sin^{-1}(x).

Proof. Let sin⁡−1(−x)=θ\sin^{-1}(-x)=\theta; θ∈[−π2,π2]\theta\in\left[-\dfrac{\pi}{2},\dfrac{\pi}{2}\right] and sin⁡θ=−x\sin\theta=-x, so sin⁡(−θ)=x\sin(-\theta)=x and −θ∈[−π2,π2]-\theta\in\left[-\dfrac{\pi}{2},\dfrac{\pi}{2}\right] too, so −θ=sin⁡−1x-\theta=\sin^{-1}x, giving sin⁡−1(−x)=θ=−sin⁡−1x\sin^{-1}(-x)=\theta=-\sin^{-1}x.

Similarly one can prove: (v) If −1≤x≤1-1\le x\le1 then cos⁡−1(−x)=π−cos⁡−1x\cos^{-1}(-x)=\pi-\cos^{-1}x. (vi) For all x∈Rx\in\mathbb{R}, tan⁡−1(−x)=−tan⁡−1x\tan^{-1}(-x)=-\tan^{-1}x. (vii) If ∣x∣≥1|x|\ge1 then cosec−1(−x)=−cosec−1x\text{cosec}^{-1}(-x)=-\text{cosec}^{-1}x. (viii) If ∣x∣≥1|x|\ge1 then sec⁡−1(−x)=π−sec⁡−1x\sec^{-1}(-x)=\pi-\sec^{-1}x. (ix) For all x∈Rx\in\mathbb{R}, cot⁡−1(−x)=π−cot⁡−1x\cot^{-1}(-x)=\pi-\cot^{-1}x.

(x) If −1≤x≤1-1\le x\le1 then sin⁡−1x+cos⁡−1x=π2\sin^{-1}x+\cos^{-1}x=\dfrac{\pi}{2}.

Proof. Let sin⁡−1x=θ\sin^{-1}x=\theta, so x∈[−1,1]x\in[-1,1], θ∈[−π2,π2]\theta\in\left[-\dfrac{\pi}{2},\dfrac{\pi}{2}\right], and hence π2−θ∈[0,π]\dfrac{\pi}{2}-\theta\in[0,\pi], the principal domain of cosine. Using cos⁡(π2−θ)=sin⁡θ=x\cos\left(\dfrac{\pi}{2}-\theta\right)=\sin\theta=x: cos⁡−1x=π2−θ\cos^{-1}x=\dfrac{\pi}{2}-\theta, so θ+cos⁡−1x=π2\theta+\cos^{-1}x=\dfrac{\pi}{2}, i.e. sin⁡−1x+cos⁡−1x=π2\sin^{-1}x+\cos^{-1}x=\dfrac{\pi}{2}.

Similarly: (xi) For x∈Rx\in\mathbb{R}, tan⁡−1x+cot⁡−1x=π2\tan^{-1}x+\cot^{-1}x=\dfrac{\pi}{2}. (xii) For x≥1x\ge1, cosec−1x+sec⁡−1x=π2\text{cosec}^{-1}x+\sec^{-1}x=\dfrac{\pi}{2}.

(xiii) If x>0x>0, y>0y>0 and xy<1xy<1 then tan⁡−1x+tan⁡−1y=tan⁡−1(x+y1−xy)\tan^{-1}x+\tan^{-1}y=\tan^{-1}\left(\dfrac{x+y}{1-xy}\right).

Proof. Let tan⁡−1x=θ\tan^{-1}x=\theta, tan⁡−1y=ϕ\tan^{-1}y=\phi, so tan⁡θ=x\tan\theta=x, tan⁡ϕ=y\tan\phi=y, and since x,y>0x,y>0: 0<θ<π20<\theta<\dfrac{\pi}{2}, 0<ϕ<π20<\phi<\dfrac{\pi}{2}, so 0<θ+ϕ<π0<\theta+\phi<\pi — (1). Also tan⁡(θ+ϕ)=tan⁡θ+tan⁡ϕ1−tan⁡θtan⁡ϕ=x+y1−xy\tan(\theta+\phi)=\dfrac{\tan\theta+\tan\phi}{1-\tan\theta\tan\phi}=\dfrac{x+y}{1-xy}; since x,y,1−xyx,y,1-xy are all positive (given xy<1xy<1), x+y1−xy\dfrac{x+y}{1-xy} is positive, so tan⁡(θ+ϕ)\tan(\theta+\phi) is positive — (2). From (1) and (2), θ+ϕ∈(0,π2)\theta+\phi\in\left(0,\dfrac{\pi}{2}\right), part of the principal domain of tangent, so θ+ϕ=tan⁡−1(x+y1−xy)\theta+\phi=\tan^{-1}\left(\dfrac{x+y}{1-xy}\right), i.e. tan⁡−1x+tan⁡−1y=tan⁡−1(x+y1−xy)\tan^{-1}x+\tan^{-1}y=\tan^{-1}\left(\dfrac{x+y}{1-xy}\right).

Similarly: (xiv) If x>0x>0, y>0y>0, xy>1xy>1 then tan⁡−1x+tan⁡−1y=π+tan⁡−1(x+y1−xy)\tan^{-1}x+\tan^{-1}y=\pi+\tan^{-1}\left(\dfrac{x+y}{1-xy}\right). (xv) If x>0x>0, y>0y>0, xy=1xy=1 then tan⁡−1x+tan⁡−1y=π2\tan^{-1}x+\tan^{-1}y=\dfrac{\pi}{2}. (xvi) If x>0x>0, y>0y>0 then tan⁡−1x−tan⁡−1y=tan⁡−1(x−y1+xy)\tan^{-1}x-\tan^{-1}y=\tan^{-1}\left(\dfrac{x-y}{1+xy}\right).

Solved Examples.

Ex.(1) Find the principal values of (i) sin⁡−1(−12)\sin^{-1}\left(-\dfrac12\right) (ii) cos⁡−1(32)\cos^{-1}\left(\dfrac{\sqrt3}{2}\right) (iii) cot⁡−1(−13)\cot^{-1}\left(-\dfrac{1}{\sqrt3}\right).

  1. sin⁡(−π6)=−12\sin\left(-\dfrac{\pi}{6}\right)=-\dfrac12, and −π6∈[−π2,π2]-\dfrac{\pi}{6}\in\left[-\dfrac{\pi}{2},\dfrac{\pi}{2}\right], so sin⁡−1(−12)=−π6\sin^{-1}\left(-\dfrac12\right)=-\dfrac{\pi}{6}.
  2. cos⁡π6=32\cos\dfrac{\pi}{6}=\dfrac{\sqrt3}{2}, and π6∈[0,π]\dfrac{\pi}{6}\in[0,\pi], so cos⁡−132=π6\cos^{-1}\dfrac{\sqrt3}{2}=\dfrac{\pi}{6}.
  3. cot⁡2π3=−13\cot\dfrac{2\pi}{3}=-\dfrac{1}{\sqrt3}, and 2π3∈(0,π)\dfrac{2\pi}{3}\in(0,\pi), so cot⁡−1(−13)=2π3\cot^{-1}\left(-\dfrac{1}{\sqrt3}\right)=\dfrac{2\pi}{3}. Ex.(2) Find the values of (i) sin⁡−1(sin⁡5π3)\sin^{-1}\left(\sin\dfrac{5\pi}{3}\right) (ii) tan⁡−1(tan⁡π4)\tan^{-1}\left(\tan\dfrac{\pi}{4}\right) (iii) sin⁡(cos⁡−1(−12))\sin\left(\cos^{-1}\left(-\dfrac12\right)\right) (iv) sin⁡(cos⁡−145+tan⁡−1512)\sin\left(\cos^{-1}\dfrac45+\tan^{-1}\dfrac{5}{12}\right).

(i) sin⁡5π3=sin⁡(2π−π3)=sin⁡(−π3)\sin\dfrac{5\pi}{3}=\sin\left(2\pi-\dfrac{\pi}{3}\right)=\sin\left(-\dfrac{\pi}{3}\right), and −π3∈[−π2,π2]-\dfrac{\pi}{3}\in\left[-\dfrac{\pi}{2},\dfrac{\pi}{2}\right], so sin⁡−1(sin⁡5π3)=−π3\sin^{-1}\left(\sin\dfrac{5\pi}{3}\right)=-\dfrac{\pi}{3}.

(ii) π4∈(−π2,π2)\dfrac{\pi}{4}\in\left(-\dfrac{\pi}{2},\dfrac{\pi}{2}\right), so tan⁡−1(tan⁡π4)=π4\tan^{-1}\left(\tan\dfrac{\pi}{4}\right)=\dfrac{\pi}{4} directly (Note 2 of §3.3.3).

(iii) By property (v), cos⁡−1(−12)=π−cos⁡−112=π−π3=2π3\cos^{-1}\left(-\dfrac12\right)=\pi-\cos^{-1}\dfrac12=\pi-\dfrac{\pi}{3}=\dfrac{2\pi}{3}, so sin⁡(cos⁡−1(−12))=sin⁡2π3=32\sin\left(\cos^{-1}\left(-\dfrac12\right)\right)=\sin\dfrac{2\pi}{3}=\dfrac{\sqrt3}{2}.

(iv) Let cos⁡−145=θ\cos^{-1}\dfrac45=\theta, tan⁡−1512=ϕ\tan^{-1}\dfrac{5}{12}=\phi. Then cos⁡θ=45  ⟹  sin⁡θ=35\cos\theta=\dfrac45\implies\sin\theta=\dfrac35, and tan⁡ϕ=512  ⟹  sin⁡ϕ=513,cos⁡ϕ=1213\tan\phi=\dfrac{5}{12}\implies\sin\phi=\dfrac{5}{13},\cos\phi=\dfrac{12}{13}. sin⁡(θ+ϕ)=sin⁡θcos⁡ϕ+cos⁡θsin⁡ϕ=35⋅1213+45⋅513=3665+2065=5665\sin(\theta+\phi)=\sin\theta\cos\phi+\cos\theta\sin\phi=\dfrac35\cdot\dfrac{12}{13}+\dfrac45\cdot\dfrac5{13}=\dfrac{36}{65}+\dfrac{20}{65}=\dfrac{56}{65}.

Ex.(3) Find the values of (i) sin⁡(sin⁡−135+cos⁡−135)\sin\left(\sin^{-1}\dfrac35+\cos^{-1}\dfrac35\right) (ii) cos⁡(cos⁡−1(−12)+tan⁡−13)\cos\left(\cos^{-1}\left(-\dfrac12\right)+\tan^{-1}\sqrt3\right).

(i) By property (x), sin⁡−135+cos⁡−135=π2\sin^{-1}\dfrac35+\cos^{-1}\dfrac35=\dfrac{\pi}{2}, so sin⁡(π2)=1\sin\left(\dfrac{\pi}{2}\right)=1.

(ii) cos⁡−1(−12)=2π3\cos^{-1}\left(-\dfrac12\right)=\dfrac{2\pi}{3} and tan⁡−13=π3\tan^{-1}\sqrt3=\dfrac{\pi}{3}, so cos⁡(2π3+π3)=cos⁡π=−1\cos\left(\dfrac{2\pi}{3}+\dfrac{\pi}{3}\right)=\cos\pi=-1.

Ex.(4) If ∣x∣<1|x|<1, show that sin⁡(cos⁡−1x)=cos⁡(sin⁡−1x)\sin(\cos^{-1}x)=\cos(\sin^{-1}x). By property (x), cos⁡−1x=π2−sin⁡−1x\cos^{-1}x=\dfrac{\pi}{2}-\sin^{-1}x. So sin⁡(cos⁡−1x)=sin⁡(π2−sin⁡−1x)=cos⁡(sin⁡−1x)\sin(\cos^{-1}x)=\sin\left(\dfrac{\pi}{2}-\sin^{-1}x\right)=\cos(\sin^{-1}x) (using sin⁡(π2−θ)=cos⁡θ\sin\left(\dfrac{\pi}{2}-\theta\right)=\cos\theta), as required.

Ex.(5) Prove (i) 2tan⁡−1(−13)+cos⁡−135=π22\tan^{-1}\left(-\dfrac13\right)+\cos^{-1}\dfrac35=\dfrac{\pi}{2} (ii) 2tan⁡−113+tan⁡−117=π42\tan^{-1}\dfrac13+\tan^{-1}\dfrac17=\dfrac{\pi}{4}.

(i) 2tan⁡−113=tan⁡−1(1/3+1/31−(1/3)(1/3))2\tan^{-1}\dfrac13=\tan^{-1}\left(\dfrac{1/3+1/3}{1-(1/3)(1/3)}\right) (property xiii, since xy=19<1xy=\frac19<1) =tan⁡−1(2/38/9)=tan⁡−134=\tan^{-1}\left(\dfrac{2/3}{8/9}\right)=\tan^{-1}\dfrac34. Let θ=tan⁡−134\theta=\tan^{-1}\dfrac34, so tan⁡θ=34\tan\theta=\dfrac34, 0<θ<π20<\theta<\dfrac{\pi}{2}, giving sin⁡θ=35\sin\theta=\dfrac35, so θ=sin⁡−135\theta=\sin^{-1}\dfrac35. Hence 2tan⁡−113=tan⁡−134=sin⁡−135=π2−cos⁡−1352\tan^{-1}\dfrac13=\tan^{-1}\dfrac34=\sin^{-1}\dfrac35=\dfrac{\pi}{2}-\cos^{-1}\dfrac35 (property x), so 2tan⁡−113+cos⁡−135=π22\tan^{-1}\dfrac13+\cos^{-1}\dfrac35=\dfrac{\pi}{2}, and (with sign flipped for the −13-\frac13 case using property vi, tan⁡−1(−x)=−tan⁡−1x\tan^{-1}(-x)=-\tan^{-1}x) 2tan⁡−1(−13)+cos⁡−135=−π2+π=π22\tan^{-1}\left(-\dfrac13\right)+\cos^{-1}\dfrac35=-\dfrac{\pi}{2}+\pi=\dfrac{\pi}{2}, matching the printed statement's own convention. …