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More from Inverse Trigonometric Functions

Match Trigonometric and Inverse Trigonometric Expressions with Evaluated Values

Match the mathematical expressions in List-I with their corresponding values in List-II and select the correct option using the codes given below:

List – IList – IIP. (1y2(cos⁡(tan⁡−1y)+ysin⁡(tan⁡−1y)cot⁡(sin⁡−1y)+tan⁡(sin⁡−1y))2+y4)1/2 evaluates to1. 1253Q. If cos⁡x+cos⁡y+cos⁡z=0=sin⁡x+sin⁡y+sin⁡z, then a possible value of cos⁡(x−y2) is2. 2R. If cos⁡(π4−x)cos⁡2x+sin⁡xsin⁡2xsec⁡x=cos⁡xsin⁡2xsec⁡x+cos⁡(π4+x)cos⁡2x,3. 12 then a possible value of sec⁡x isS. If cot⁡(sin⁡−11−x2)=sin⁡(tan⁡−1(x6)),  x≠0, then a possible value of x is4. 1\begin{array}{ll} \textbf{List -- I} & \textbf{List -- II} \\[6pt] \text{P. } \left( \dfrac{1}{y^2} \left( \dfrac{\cos(\tan^{-1} y) + y \sin(\tan^{-1} y)}{\cot(\sin^{-1} y) + \tan(\sin^{-1} y)} \right)^2 + y^4 \right)^{1/2} \text{ evaluates to} & \text{1. } \dfrac{1}{2}\sqrt{\dfrac{5}{3}} \\[16pt] \text{Q. If } \cos x + \cos y + \cos z = 0 = \sin x + \sin y + \sin z, \text{ then a possible value of } \cos\left(\dfrac{x-y}{2}\right) \text{ is} & \text{2. } \sqrt{2} \\[12pt] \text{R. If } \cos\left(\dfrac{\pi}{4}-x\right)\cos 2x + \sin x \sin 2x \sec x = \cos x \sin 2x \sec x + \cos\left(\dfrac{\pi}{4}+x\right)\cos 2x, & \text{3. } \dfrac{1}{2} \\[4pt] \quad\text{ then a possible value of } \sec x \text{ is} & \\[12pt] \text{S. If } \cot\left(\sin^{-1}\sqrt{1-x^2}\right) = \sin\left(\tan^{-1}(x\sqrt{6})\right), \; x \neq 0, \text{ then a possible value of } x \text{ is} & \text{4. } 1 \end{array}

Options

A

P →\rightarrow 4, Q →\rightarrow 3, R →\rightarrow 1, S →\rightarrow 2

B

P →\rightarrow 4, Q →\rightarrow 3, R →\rightarrow 2, S →\rightarrow 1

Correct
C

P →\rightarrow 3, Q →\rightarrow 4, R →\rightarrow 2, S →\rightarrow 1

D

P →\rightarrow 3, Q →\rightarrow 4, R →\rightarrow 1, S →\rightarrow 2

Step-by-Step Solution

To match each expression in List-I with its correct value in List-II, we evaluate each part step-by-step:


Evaluation of P:

The given expression is: E=(1y2(cos⁡(tan⁡−1y)+ysin⁡(tan⁡−1y)cot⁡(sin⁡−1y)+tan⁡(sin⁡−1y))2+y4)1/2E = \left( \dfrac{1}{y^2} \left( \dfrac{\cos(\tan^{-1} y) + y \sin(\tan^{-1} y)}{\cot(\sin^{-1} y) + \tan(\sin^{-1} y)} \right)^2 + y^4 \right)^{1/2}

  1. Numerator: Let θ=tan⁡−1y\theta = \tan^{-1} y, which implies: cos⁡θ=11+y2andsin⁡θ=y1+y2\cos\theta = \frac{1}{\sqrt{1+y^2}} \quad \text{and} \quad \sin\theta = \frac{y}{\sqrt{1+y^2}} cos⁡(tan⁡−1y)+ysin⁡(tan⁡−1y)=11+y2+y(y1+y2)=1+y21+y2=1+y2\cos(\tan^{-1} y) + y \sin(\tan^{-1} y) = \frac{1}{\sqrt{1+y^2}} + y\left(\frac{y}{\sqrt{1+y^2}}\right) = \frac{1+y^2}{\sqrt{1+y^2}} = \sqrt{1+y^2}

  2. Denominator: Let ϕ=sin⁡−1y\phi = \sin^{-1} y, then: cot⁡(sin⁡−1y)+tan⁡(sin⁡−1y)=cot⁡ϕ+tan⁡ϕ=cos⁡ϕsin⁡ϕ+sin⁡ϕcos⁡ϕ=cos⁡2ϕ+sin⁡2ϕsin⁡ϕcos⁡ϕ=1y1−y2\cot(\sin^{-1} y) + \tan(\sin^{-1} y) = \cot\phi + \tan\phi = \frac{\cos\phi}{\sin\phi} + \frac{\sin\phi}{\cos\phi} = \frac{\cos^2\phi + \sin^2\phi}{\sin\phi\cos\phi} = \frac{1}{y\sqrt{1-y^2}}

  3. Substituting the numerator and denominator into the quotient: cos⁡(tan⁡−1y)+ysin⁡(tan⁡−1y)cot⁡(sin⁡−1y)+tan⁡(sin⁡−1y)=1+y2⋅(y1−y2)=y1−y4\dfrac{\cos(\tan^{-1} y) + y \sin(\tan^{-1} y)}{\cot(\sin^{-1} y) + \tan(\sin^{-1} y)} = \sqrt{1+y^2} \cdot \left(y\sqrt{1-y^2}\right) = y\sqrt{1-y^4}

  4. Substituting back into the original expression: E=(1y2(y1−y4)2+y4)1/2=(1y2⋅y2(1−y4)+y4)1/2=(1−y4+y4)1/2=1=1E = \left( \frac{1}{y^2}\left(y\sqrt{1-y^4}\right)^2 + y^4 \right)^{1/2} = \left( \frac{1}{y^2}\cdot y^2(1-y^4) + y^4 \right)^{1/2} = \left( 1 - y^4 + y^4 \right)^{1/2} = \sqrt{1} = 1

Thus, P→4\text{P} \rightarrow 4.


Evaluation of Q:

Given that: cos⁡x+cos⁡y+cos⁡z=0  ⟹  cos⁡x+cos⁡y=−cos⁡z\cos x + \cos y + \cos z = 0 \implies \cos x + \cos y = -\cos z sin⁡x+sin⁡y+sin⁡z=0  ⟹  sin⁡x+sin⁡y=−sin⁡z\sin x + \sin y + \sin z = 0 \implies \sin x + \sin y = -\sin z

Squaring both equations and adding them: (cos⁡x+cos⁡y)2+(sin⁡x+sin⁡y)2=(−cos⁡z)2+(−sin⁡z)2(\cos x + \cos y)^2 + (\sin x + \sin y)^2 = (-\cos z)^2 + (-\sin z)^2 cos⁡2x+cos⁡2y+2cos⁡xcos⁡y+sin⁡2x+sin⁡2y+2sin⁡xsin⁡y=cos⁡2z+sin⁡2z\cos^2 x + \cos^2 y + 2\cos x\cos y + \sin^2 x + \sin^2 y + 2\sin x\sin y = \cos^2 z + \sin^2 z (1)+(1)+2(cos⁡xcos⁡y+sin⁡xsin⁡y)=1(1) + (1) + 2(\cos x\cos y + \sin x\sin y) = 1 2+2cos⁡(x−y)=12 + 2\cos(x-y) = 1 2(1+cos⁡(x−y))=12(1 + \cos(x-y)) = 1

Using the half-angle formula 1+cos⁡(x−y)=2cos⁡2(x−y2)1 + \cos(x-y) = 2\cos^2\left(\dfrac{x-y}{2}\right): 4cos⁡2(x−y2)=1  ⟹  cos⁡2(x−y2)=14  ⟹  cos⁡(x−y2)=±124\cos^2\left(\dfrac{x-y}{2}\right) = 1 \implies \cos^2\left(\dfrac{x-y}{2}\right) = \dfrac{1}{4} \implies \cos\left(\dfrac{x-y}{2}\right) = \pm\dfrac{1}{2}

Thus, a possible value is 12\dfrac{1}{2}, so Q→3\text{Q} \rightarrow 3.


Evaluation of R:

The given equation is: cos⁡(π4−x)cos⁡2x+sin⁡xsin⁡2xsec⁡x=cos⁡xsin⁡2xsec⁡x+cos⁡(π4+x)cos⁡2x\cos\left(\frac{\pi}{4}-x\right)\cos 2x + \sin x \sin 2x \sec x = \cos x \sin 2x \sec x + \cos\left(\frac{\pi}{4}+x\right)\cos 2x

Rearranging the terms: [cos⁡(π4−x)−cos⁡(π4+x)]cos⁡2x=(cos⁡x−sin⁡x)sin⁡2xsec⁡x\left[ \cos\left(\frac{\pi}{4}-x\right) - \cos\left(\frac{\pi}{4}+x\right) \right]\cos 2x = (\cos x - \sin x)\sin 2x \sec x

Using the identity cos⁡(A−B)−cos⁡(A+B)=2sin⁡Asin⁡B\cos(A-B) - \cos(A+B) = 2\sin A\sin B: 2sin⁡(π4)sin⁡xcos⁡2x=(cos⁡x−sin⁡x)(2sin⁡xcos⁡x)(1cos⁡x)2\sin\left(\frac{\pi}{4}\right)\sin x \cos 2x = (\cos x - \sin x)(2\sin x \cos x)\left(\frac{1}{\cos x}\right) 2sin⁡xcos⁡2x=2sin⁡x(cos⁡x−sin⁡x)\sqrt{2}\sin x \cos 2x = 2\sin x(\cos x - \sin x)

Assuming sin⁡x≠0\sin x \neq 0: 2cos⁡2x=2(cos⁡x−sin⁡x)\sqrt{2}\cos 2x = 2(\cos x - \sin x)

Using cos⁡2x=cos⁡2x−sin⁡2x=(cos⁡x−sin⁡x)(cos⁡x+sin⁡x)\cos 2x = \cos^2 x - \sin^2 x = (\cos x - \sin x)(\cos x + \sin x): 2(cos⁡x−sin⁡x)(cos⁡x+sin⁡x)−2(cos⁡x−sin⁡x)=0\sqrt{2}(\cos x - \sin x)(\cos x + \sin x) - 2(\cos x - \sin x) = 0 (cos⁡x−sin⁡x)[2(cos⁡x+sin⁡x)−2]=0(\cos x - \sin x)\left[\sqrt{2}(\cos x + \sin x) - 2\right] = 0

  • If cos⁡x−sin⁡x=0\cos x - \sin x = 0: tan⁡x=1  ⟹  sec⁡2x=1+tan⁡2x=2  ⟹  sec⁡x=±2\tan x = 1 \implies \sec^2 x = 1 + \tan^2 x = 2 \implies \sec x = \pm\sqrt{2}

  • If 2(cos⁡x+sin⁡x)=2  ⟹  cos⁡x+sin⁡x=2\sqrt{2}(\cos x + \sin x) = 2 \implies \cos x + \sin x = \sqrt{2}: cos⁡(x−π4)=1  ⟹  x=2nπ+π4  ⟹  sec⁡x=2\cos\left(x - \frac{\pi}{4}\right) = 1 \implies x = 2n\pi + \frac{\pi}{4} \implies \sec x = \sqrt{2}

Thus, a possible value of sec⁡x\sec x is 2\sqrt{2}, so R→2\text{R} \rightarrow 2.


Evaluation of S:

The given equation is: cot⁡(sin⁡−11−x2)=sin⁡(tan⁡−1(x6)),x≠0\cot\left(\sin^{-1}\sqrt{1-x^2}\right) = \sin\left(\tan^{-1}(x\sqrt{6})\right), \quad x \neq 0

  1. For the LHS, let α=sin⁡−11−x2\alpha = \sin^{-1}\sqrt{1-x^2} where sin⁡α=1−x2\sin\alpha = \sqrt{1-x^2}. Then: cos⁡α=1−sin⁡2α=1−(1−x2)=∣x∣=x(for x>0)\cos\alpha = \sqrt{1 - \sin^2\alpha} = \sqrt{1 - (1-x^2)} = |x| = x \quad (\text{for } x > 0) cot⁡α=cos⁡αsin⁡α=x1−x2\cot\alpha = \frac{\cos\alpha}{\sin\alpha} = \frac{x}{\sqrt{1-x^2}}

  2. For the RHS, let β=tan⁡−1(x6)\beta = \tan^{-1}(x\sqrt{6}) where tan⁡β=x6\tan\beta = x\sqrt{6}. Then: sin⁡β=tan⁡β1+tan⁡2β=x61+6x2\sin\beta = \frac{\tan\beta}{\sqrt{1+\tan^2\beta}} = \frac{x\sqrt{6}}{\sqrt{1 + 6x^2}}

Equating LHS and RHS: x1−x2=x61+6x2\frac{x}{\sqrt{1-x^2}} = \frac{x\sqrt{6}}{\sqrt{1+6x^2}}

Since x≠0x \neq 0, divide both sides by xx: 11−x2=61+6x2\frac{1}{\sqrt{1-x^2}} = \frac{\sqrt{6}}{\sqrt{1+6x^2}}

Squaring both sides: 11−x2=61+6x2\frac{1}{1-x^2} = \frac{6}{1+6x^2} 1+6x2=6(1−x2)1 + 6x^2 = 6(1-x^2) 1+6x2=6−6x21 + 6x^2 = 6 - 6x^2 12x2=5  ⟹  x2=51212x^2 = 5 \implies x^2 = \frac{5}{12} x=512=1253x = \sqrt{\frac{5}{12}} = \frac{1}{2}\sqrt{\frac{5}{3}}

Thus, S→1\text{S} \rightarrow 1.


Conclusion:

The correct matching is: P→4,Q→3,R→2,S→1\text{P} \rightarrow 4, \quad \text{Q} \rightarrow 3, \quad \text{R} \rightarrow 2, \quad \text{S} \rightarrow 1

Therefore, the correct option is B.