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Exercise 4.5 · Q9

Q.Solve:

(i) sin⁡−15x+sin⁡−112x=π2\sin^{-1}\dfrac5x + \sin^{-1}\dfrac{12}x = \dfrac{\pi}2
(ii) 2tan⁡−1x=cos⁡−11−a21+a2−cos⁡−11−b21+b22\tan^{-1}x = \cos^{-1}\dfrac{1-a^2}{1+a^2} - \cos^{-1}\dfrac{1-b^2}{1+b^2}, a>0, b>0a>0,\ b>0.
(iii) 2tan⁡−1(cos⁡x)=tan⁡−1(2 cosec x)2\tan^{-1}(\cos x) = \tan^{-1}(2\,\text{cosec}\,x)
(iv) cot⁡−1x−cot⁡−1(x+2)=π12\cot^{-1}x - \cot^{-1}(x+2) = \dfrac{\pi}{12}, x>0x>0.
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Each part is a distinct equation-solving technique built from the chapter's sum/double-angle identities; we solve each in turn and check the resulting value against any stated restriction.

Step 1. (i) Use the complementary-angle idea. If x=13x=13, then 513\dfrac5{13} and 1213\dfrac{12}{13} are the legs-over-hypotenuse of a 55–1212–1313 right triangle, so sin⁡−1513+sin⁡−11213=π2\sin^{-1}\dfrac5{13}+\sin^{-1}\dfrac{12}{13}=\dfrac{\pi}2 exactly (since (513)2+(1213)2=1\left(\dfrac5{13}\right)^2+\left(\dfrac{12}{13}\right)^2=1 means the two angles are complementary).

Step 2. (i) Confirm by direct algebra. Let θ=sin⁡−15x\theta=\sin^{-1}\dfrac5x. The equation forces cos⁡θ=sin⁡(π2−θ)=12x\cos\theta=\sin\left(\dfrac{\pi}2-\theta\right)=\dfrac{12}x, so 1−25x2=12x⇒1−25x2=144x2⇒x2=169⇒x=±13\sqrt{1-\dfrac{25}{x^2}}=\dfrac{12}x\Rightarrow1-\dfrac{25}{x^2}=\dfrac{144}{x^2}\Rightarrow x^2=169\Rightarrow x=\pm13. Only x=13x=13 keeps both arguments positive so the sum of two positive arcsines can equal +π2+\dfrac{\pi}2 (at x=−13x=-13 the sum would be −π2-\dfrac{\pi}2). So x=13x=13.

Step 3. (ii) Apply the double-angle cosine-inverse identity. For t≥0t\ge0, cos⁡−11−t21+t2=2tan⁡−1t\cos^{-1}\dfrac{1-t^2}{1+t^2}=2\tan^{-1}t. With a,b>0a,b>0: cos⁡−11−a21+a2=2tan⁡−1a\cos^{-1}\dfrac{1-a^2}{1+a^2}=2\tan^{-1}a and cos⁡−11−b21+b2=2tan⁡−1b\cos^{-1}\dfrac{1-b^2}{1+b^2}=2\tan^{-1}b.

Step 4. (ii) Substitute and simplify. 2tan⁡−1x=2tan⁡−1a−2tan⁡−1b⇒tan⁡−1x=tan⁡−1a−tan⁡−1b=tan⁡−1a−b1+ab2\tan^{-1}x=2\tan^{-1}a-2\tan^{-1}b\Rightarrow\tan^{-1}x=\tan^{-1}a-\tan^{-1}b=\tan^{-1}\dfrac{a-b}{1+ab} (valid since a,b>0⇒ab>−1a,b>0\Rightarrow ab>-1). Hence x=a−b1+abx=\dfrac{a-b}{1+ab}.

Step 5. (iii) Apply the double-angle tangent identity to the left side. With t=cos⁡xt=\cos x (so ∣t∣<1|t|<1 generically), 2tan⁡−1(cos⁡x)=tan⁡−12cos⁡x1−cos⁡2x=tan⁡−12cos⁡xsin⁡2x2\tan^{-1}(\cos x)=\tan^{-1}\dfrac{2\cos x}{1-\cos^2x}=\tan^{-1}\dfrac{2\cos x}{\sin^2x}.

Step 6. (iii) Equate the arguments. 2cos⁡xsin⁡2x=2 cosec x=2sin⁡x⇒cos⁡xsin⁡2x=1sin⁡x⇒cos⁡x=sin⁡x⇒tan⁡x=1\dfrac{2\cos x}{\sin^2x}=2\,\text{cosec}\,x=\dfrac2{\sin x}\Rightarrow\dfrac{\cos x}{\sin^2x}=\dfrac1{\sin x}\Rightarrow\cos x=\sin x\Rightarrow\tan x=1. …

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