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Chapter 2 · Inverse Trigonometric Functions

Exercise 2.2 · Q9: tan⁡12[sin⁡−12x1+x2\tan\frac12\Big[\sin^{-1}\frac{2x}{1+x^2} +cos⁡−11−y21+y2]+\cos^{-1}\frac{1-y^2}{1+y^2}\Big]

Exercise 2.2Simplifying by substitution · Section 2.3
The question

Find the values of each of the following:

tan⁡12[sin⁡−12x1+x2+cos⁡−11−y21+y2],\tan\frac12\left[\sin^{-1}\frac{2x}{1+x^2}+\cos^{-1}\frac{1-y^2}{1+y^2}\right],

∣x∣<1|x|<1⁠, y>0y>0 and xy<1xy<1⁠.

Exam answer

Put x=tan⁡αx = \tan\alpha⁠, y=tan⁡βy = \tan\beta⁠, where α=tan⁡−1x\alpha = \tan^{-1}x⁠, β=tan⁡−1y\beta = \tan^{-1}y⁠.

As ∣x∣<1|x| < 1⁠, −π4<α<π4-\frac{\pi}{4} < \alpha < \frac{\pi}{4}⁠, so −π2<2α<π2-\frac{\pi}{2} < 2\alpha < \frac{\pi}{2}⁠.

As y>0y > 0⁠, 0<β<π20 < \beta < \frac{\pi}{2}⁠, so 0<2β<π0 < 2\beta < \pi⁠.

Using sin⁡2α=2tan⁡α1+tan⁡2α\sin 2\alpha = \frac{2\tan\alpha}{1 + \tan^2\alpha} and 2α∈[−π2,π2]2\alpha \in \left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠,

sin⁡−12x1+x2=sin⁡−12tan⁡α1+tan⁡2α=sin⁡−1(sin⁡2α)=2α\begin{aligned} &\sin^{-1}\frac{2x}{1 + x^2} \\ &= \sin^{-1}\frac{2\tan\alpha}{1 + \tan^2\alpha} \\ &= \sin^{-1}(\sin 2\alpha) = 2\alpha \end{aligned}

Using cos⁡2β=1−tan⁡2β1+tan⁡2β\cos 2\beta = \frac{1 - \tan^2\beta}{1 + \tan^2\beta} and 2β∈[0,π]2\beta \in [0, \pi]⁠,

cos⁡−11−y21+y2=cos⁡−11−tan⁡2β1+tan⁡2β=cos⁡−1(cos⁡2β)=2β\begin{aligned} &\cos^{-1}\frac{1 - y^2}{1 + y^2} \\ &= \cos^{-1}\frac{1 - \tan^2\beta}{1 + \tan^2\beta} \\ &= \cos^{-1}(\cos 2\beta) = 2\beta \end{aligned} ∴ tan⁡12[sin⁡−12x1+x2+cos⁡−11−y21+y2]=tan⁡12(2α+2β)=tan⁡(α+β)=tan⁡α+tan⁡β1−tan⁡αtan⁡β(xy<1)\begin{aligned} \therefore\ &\tan\frac12\bigg[\sin^{-1}\frac{2x}{1 + x^2} \\ &\qquad + \cos^{-1}\frac{1 - y^2}{1 + y^2}\bigg] \\ &= \tan\frac12(2\alpha + 2\beta) = \tan(\alpha + \beta) \\ &= \frac{\tan\alpha + \tan\beta}{1 - \tan\alpha\tan\beta} \quad (xy < 1) \end{aligned}

∴\therefore the required value is x+y1−xy\dfrac{x + y}{1 - xy}⁠.

Want the reason behind every step, the basics and the checks?

The one idea this problem is built on

The fractions 2t1+t2\dfrac{2t}{1+t^2} and 1−t21+t2\dfrac{1-t^2}{1+t^2} are sin⁡2ϕ\sin2\phi and cos⁡2ϕ\cos2\phi written in terms of t=tan⁡ϕt=\tan\phi⁠. So put x=tan⁡αx=\tan\alpha and y=tan⁡βy=\tan\beta⁠. The first term becomes sin⁡−1(sin⁡2α)\sin^{-1}(\sin2\alpha) and the second cos⁡−1(cos⁡2β)\cos^{-1}(\cos2\beta)⁠. Each collapses to 2α2\alpha and 2β2\beta only because the conditions put 2α2\alpha in [−π2,π2]\left[-\frac{\pi}{2},\frac{\pi}{2}\right] and 2β2\beta in [0,π][0,\pi]⁠. Half the sum is α+β\alpha+\beta⁠, and the tangent addition formula finishes it.

Given, to find, and the plan
Given
Real numbers xx⁠, yy with ∣x∣<1|x|<1⁠, y>0y>0⁠, xy<1xy<1⁠.
To find
The value of the expression in terms of xx and yy⁠.
Plan
(1) Derive sin⁡2ϕ\sin2\phi and cos⁡2ϕ\cos2\phi in terms of tan⁡ϕ\tan\phi⁠. (2) Set α=tan⁡−1x\alpha=\tan^{-1}x⁠, β=tan⁡−1y\beta=\tan^{-1}y and find their exact ranges. (3) Simplify the sin⁡−1\sin^{-1} term. (4) Simplify the cos⁡−1\cos^{-1} term. (5) Halve the sum and apply tan⁡(α+β)\tan(\alpha+\beta)⁠, checking it is defined. (6) See what each condition was for.

Basics you need

1Principal ranges

sin⁡−1\sin^{-1} in [−π2,π2]\left[-\frac{\pi}{2},\frac{\pi}{2}\right]⁠, cos⁡−1\cos^{-1} in [0,π][0,\pi]⁠, tan⁡−1\tan^{-1} in (−π2,π2)\left(-\frac{\pi}{2},\frac{\pi}{2}\right)⁠. Basics: domain and range of sin and cos

2When an inverse undoes its function

sin⁡−1(sin⁡u)=u\sin^{-1}(\sin u)=u needs u∈[−π2,π2]u\in\left[-\frac{\pi}{2},\frac{\pi}{2}\right]⁠; cos⁡−1(cos⁡u)=u\cos^{-1}(\cos u)=u needs u∈[0,π]u\in[0,\pi]⁠. Outside these, the answer is a different angle. Lesson: the folding rules

3Double-angle and addition formulas

sin⁡2ϕ=2sin⁡ϕcos⁡ϕ\sin2\phi=2\sin\phi\cos\phi⁠, cos⁡2ϕ=cos⁡2ϕ−sin⁡2ϕ\cos2\phi=\cos^2\phi-\sin^2\phi⁠, tan⁡(A+B)=tan⁡A+tan⁡B1−tan⁡Atan⁡B\tan(A+B)=\dfrac{\tan A+\tan B}{1-\tan A\tan B}⁠, and 1+tan⁡2ϕ=sec⁡2ϕ1+\tan^2\phi=\sec^2\phi⁠. (Class XI, Chapter 3.) Basics: tan, cot, sec and cosec

4Substitution

An expression built from 2t1+t2\frac{2t}{1+t^2} or 1−t21+t2\frac{1-t^2}{1+t^2} calls for t=tan⁡ϕt=\tan\phi⁠. Lesson: substitutions and simplest form

Solution

  1. sin⁡2ϕ\sin2\phi and cos⁡2ϕ\cos2\phi in terms of tan⁡ϕ\tan\phi

    For any ϕ\phi with cos⁡ϕ≠0\cos\phi\ne0⁠, we have cos⁡2ϕ=1sec⁡2ϕ=11+tan⁡2ϕ\cos^2\phi=\dfrac{1}{\sec^2\phi}=\dfrac{1}{1+\tan^2\phi}⁠. Hence

    sin⁡2ϕ=2sin⁡ϕcos⁡ϕ=2tan⁡ϕcos⁡2ϕ=2tan⁡ϕ1+tan⁡2ϕ,\begin{aligned} \sin2\phi &= 2\sin\phi\cos\phi \\ &= 2\tan\phi\cos^2\phi \\ &= \frac{2\tan\phi}{1+\tan^2\phi}, \end{aligned} cos⁡2ϕ=cos⁡2ϕ−sin⁡2ϕ=cos⁡2ϕ(1−tan⁡2ϕ)=1−tan⁡2ϕ1+tan⁡2ϕ.\begin{aligned} \cos2\phi &= \cos^2\phi-\sin^2\phi \\ &= \cos^2\phi\left(1-\tan^2\phi\right) \\ &= \frac{1-\tan^2\phi}{1+\tan^2\phi}. \end{aligned}
    These are exactly the two fractions in the question, with xx or yy in place of tan⁡ϕ\tan\phi⁠. The rewriting uses sin⁡ϕ=tan⁡ϕcos⁡ϕ\sin\phi=\tan\phi\cos\phi and then cos⁡2ϕ=11+tan⁡2ϕ\cos^2\phi=\frac{1}{1+\tan^2\phi}⁠.
    1+tan⁡2ϕ=sec⁡2ϕ1+\tan^2\phi=\sec^2\phi comes from dividing sin⁡2ϕ+cos⁡2ϕ=1\sin^2\phi+\cos^2\phi=1 by cos⁡2ϕ\cos^2\phi⁠.
  2. Set x=tan⁡αx=\tan\alpha⁠, y=tan⁡βy=\tan\beta and find the ranges

    Let α=tan⁡−1x\alpha=\tan^{-1}x and β=tan⁡−1y\beta=\tan^{-1}y⁠, so x=tan⁡αx=\tan\alpha and y=tan⁡βy=\tan\beta⁠, with both angles in (−π2,π2)\left(-\frac{\pi}{2},\frac{\pi}{2}\right)⁠. Because tan⁡−1\tan^{-1} is increasing and tan⁡−1(±1)=±π4\tan^{-1}(\pm1)=\pm\frac{\pi}{4}⁠, tan⁡−10=0\tan^{-1}0=0⁠:

    • −1<x<1-1<x<1 gives −π4<α<π4-\frac{\pi}{4}<\alpha<\frac{\pi}{4}⁠, so −π2<2α<π2-\frac{\pi}{2}<2\alpha<\frac{\pi}{2}.
    • y>0y>0 gives 0<β<π20<\beta<\frac{\pi}{2}⁠, so 0<2β<π0<2\beta<\pi.
    The substitutions are always allowed, since tan⁡−1\tan^{-1} accepts every real number. What matters is where the angles land. The two highlighted facts are exactly what Steps 3 and 4 need.
    tan⁡π4=1\tan\frac{\pi}{4}=1⁠. An increasing function preserves inequalities. Basics: special angles
  3. The sin⁡−1\sin^{-1} term is 2α2\alpha

    By Step 1 with ϕ=α\phi=\alpha⁠,

    2x1+x2=2tan⁡α1+tan⁡2α=sin⁡2α.\frac{2x}{1+x^2}=\frac{2\tan\alpha}{1+\tan^2\alpha}=\sin2\alpha.

    So sin⁡−12x1+x2=sin⁡−1(sin⁡2α)=2α\sin^{-1}\dfrac{2x}{1+x^2}=\sin^{-1}(\sin2\alpha)=2\alpha⁠, because 2α∈(−π2,π2)2\alpha\in\left(-\frac{\pi}{2},\frac{\pi}{2}\right) (Step 2) lies inside the principal range [−π2,π2]\left[-\frac{\pi}{2},\frac{\pi}{2}\right] of sin⁡−1\sin^{-1}⁠.

    This is where ∣x∣<1|x|<1 is used. If ∣x∣>1|x|>1⁠, then 2α2\alpha would be outside [−π2,π2]\left[-\frac{\pi}{2},\frac{\pi}{2}\right] and sin⁡−1(sin⁡2α)\sin^{-1}(\sin2\alpha) would not be 2α2\alpha⁠. For example, x=2x=2 gives sin⁡−145=π−2tan⁡−12\sin^{-1}\frac45=\pi-2\tan^{-1}2⁠, not 2tan⁡−122\tan^{-1}2⁠.
    sin⁡−1(sin⁡u)=u\sin^{-1}(\sin u)=u for u∈[−π2,π2]u\in\left[-\frac{\pi}{2},\frac{\pi}{2}\right] (Section 2.3). Lesson: the folding rules
  4. The cos⁡−1\cos^{-1} term is 2β2\beta

    By Step 1 with ϕ=β\phi=\beta⁠,

    1−y21+y2=1−tan⁡2β1+tan⁡2β=cos⁡2β.\frac{1-y^2}{1+y^2}=\frac{1-\tan^2\beta}{1+\tan^2\beta}=\cos2\beta.

    So cos⁡−11−y21+y2=cos⁡−1(cos⁡2β)\cos^{-1}\dfrac{1-y^2}{1+y^2}=\cos^{-1}(\cos2\beta)⁠, and this is 2β2\beta⁠, because 2β∈(0,π)2\beta\in(0,\pi) (Step 2) lies inside the principal range [0,π][0,\pi] of cos⁡−1\cos^{-1}⁠.

    π/2−π/2 0π 2α in (−π/2, π/2) 2β in (0, π) sin⁻¹(sin 2α) = 2α cos⁻¹(cos 2β) = 2β
    Left: ∣x∣<1|x|<1 keeps 2α2\alpha on the open right half of the circle, inside the range of sin⁡−1\sin^{-1}⁠. Right: y>0y>0 keeps 2β2\beta on the open upper half, inside the range of cos⁡−1\cos^{-1}⁠. Open circles mark endpoints that are not reached.
    This is where y>0y>0 is used. If y<0y<0⁠, then 2β∈(−π,0)2\beta\in(-\pi,0) and cos⁡−1(cos⁡2β)=−2β\cos^{-1}(\cos2\beta)=-2\beta⁠, which changes the final answer to x−y1+xy\frac{x-y}{1+xy}⁠. For example, x=0.5x=0.5⁠, y=−0.5y=-0.5 gives the value 10.75=43\frac{1}{0.75}=\frac43⁠, while x+y1−xy=0\frac{x+y}{1-xy}=0⁠.
    cos⁡−1(cos⁡u)=u\cos^{-1}(\cos u)=u for u∈[0,π]u\in[0,\pi] (Section 2.3, "similar results"). Lesson: the folding rules
  5. Halve the sum and use tan⁡(α+β)\tan(\alpha+\beta)

    By Steps 3 and 4,

    12[sin⁡−12x1+x2+cos⁡−11−y21+y2]=12(2α+2β)=α+β.\begin{aligned} &\frac12\left[\sin^{-1}\frac{2x}{1+x^2}+\cos^{-1}\frac{1-y^2}{1+y^2}\right] \\[1mm] &\quad=\frac12(2\alpha+2\beta)=\alpha+\beta. \end{aligned}

    Before taking its tangent, check tan⁡(α+β)\tan(\alpha+\beta) is defined, that is cos⁡(α+β)≠0\cos(\alpha+\beta)\ne0⁠. Factor out cos⁡αcos⁡β\cos\alpha\cos\beta⁠:

    cos⁡(α+β)=cos⁡αcos⁡β−sin⁡αsin⁡β=cos⁡αcos⁡β (1−tan⁡αtan⁡β)=cos⁡αcos⁡β (1−xy).\begin{aligned} \cos(\alpha+\beta) &= \cos\alpha\cos\beta-\sin\alpha\sin\beta \\ &= \cos\alpha\cos\beta\,(1-\tan\alpha\tan\beta) \\ &= \cos\alpha\cos\beta\,(1-xy). \end{aligned}

    Here cos⁡α>0\cos\alpha>0 and cos⁡β>0\cos\beta>0 (both angles are in (−π2,π2)\left(-\frac{\pi}{2},\frac{\pi}{2}\right)⁠) and 1−xy>01-xy>0 (given xy<1xy<1⁠). So cos⁡(α+β)>0\cos(\alpha+\beta)>0⁠, and the addition formula applies:

    tan⁡(α+β)=tan⁡α+tan⁡β1−tan⁡αtan⁡β=x+y1−xy.\tan(\alpha+\beta)=\frac{\tan\alpha+\tan\beta}{1-\tan\alpha\tan\beta}=\frac{x+y}{1-xy}.
    This is where xy<1xy<1 is used: it makes the denominator 1−xy1-xy non-zero, so the answer exists. (At xy=1xy=1⁠, for instance x=0.5x=0.5⁠, y=2y=2⁠, we get α+β=π2\alpha+\beta=\frac{\pi}{2} and the tangent is undefined.) In fact cos⁡(α+β)>0\cos(\alpha+\beta)>0 shows more: α+β\alpha+\beta lies in (−π4,π2)\left(-\frac{\pi}{4},\frac{\pi}{2}\right)⁠, so the bracket is also equal to 2tan⁡−1x+y1−xy2\tan^{-1}\frac{x+y}{1-xy}⁠.

    Is xy<1xy<1 more than we need? Yes. If ∣x∣<1|x|<1⁠, y>0y>0 but xy>1xy>1 (for example x=0.9x=0.9⁠, y=2y=2⁠), Steps 2 to 4 are unchanged and α+β\alpha+\beta lies in (π2,3π4)\left(\frac{\pi}{2},\frac{3\pi}{4}\right)⁠, where tangent is still defined, so the addition formula still gives x+y1−xy\frac{x+y}{1-xy} (here 2.9−0.8=−3.625\frac{2.9}{-0.8}=-3.625⁠, a negative value, as it should be in that interval). Only xy=1xy=1 has to be excluded. What xy>1xy>1 would break is the different statement that α+β\alpha+\beta equals tan⁡−1x+y1−xy\tan^{-1}\frac{x+y}{1-xy}⁠, since tan⁡−1\tan^{-1} cannot return an angle above π2\frac{\pi}{2}⁠.

    tan⁡(A+B)=tan⁡A+tan⁡B1−tan⁡Atan⁡B\tan(A+B)=\dfrac{\tan A+\tan B}{1-\tan A\tan B} (Class XI, Chapter 3). Dividing cos⁡Acos⁡B−sin⁡Asin⁡B\cos A\cos B-\sin A\sin B by cos⁡Acos⁡B\cos A\cos B is the same algebra that proves it.
Result

tan⁡12[sin⁡−12x1+x2+cos⁡−11−y21+y2]=x+y1−xy\begin{aligned} &\tan\frac12\left[\sin^{-1}\frac{2x}{1+x^2}+\cos^{-1}\frac{1-y^2}{1+y^2}\right] \\[1mm] &\quad=\frac{x+y}{1-xy} \end{aligned} for ∣x∣<1|x|<1⁠, y>0y>0⁠, xy<1xy<1⁠. (Textbook answer: x+y1−xy\frac{x+y}{1-xy}⁠.)

Check it with numbers

Take x=0.5x=0.5⁠, y=0.4y=0.4 (so xy=0.2<1xy=0.2<1⁠).

  • 2x1+x2=11.25=0.8\frac{2x}{1+x^2}=\frac{1}{1.25}=0.8⁠, and sin⁡−10.8=0.9272952180\sin^{-1}0.8=0.9272952180⁠.
  • 1−y21+y2=0.841.16\frac{1-y^2}{1+y^2}=\frac{0.84}{1.16}⁠, which is 0.72413793100.7241379310⁠; its cos⁡−1\cos^{-1} is 0.76101275420.7610127542⁠.
  • Half the sum: 0.84415398610.8441539861⁠. Its tangent: 1.12500000001.1250000000⁠.
  • Formula: 0.5+0.41−0.2=0.90.8=1.125\frac{0.5+0.4}{1-0.2}=\frac{0.9}{0.8}=1.125⁠. ✓
Common mistakes
  1. Writing sin⁡−12x1+x2=2tan⁡−1x\sin^{-1}\frac{2x}{1+x^2}=2\tan^{-1}x for every xx⁠. It holds only for ∣x∣≤1|x|\le1⁠. That is why the question says ∣x∣<1|x|<1⁠.
  2. Writing cos⁡−11−y21+y2=2tan⁡−1y\cos^{-1}\frac{1-y^2}{1+y^2}=2\tan^{-1}y for every yy⁠. It needs y≥0y\ge0⁠; for y<0y<0 it equals −2tan⁡−1y-2\tan^{-1}y⁠.
  3. Forgetting the half. The bracket is 2α+2β2\alpha+2\beta⁠; the 12\frac12 brings it back to α+β\alpha+\beta⁠.
  4. Using tan⁡(α+β)\tan(\alpha+\beta) without checking it is defined. It needs xy≠1xy\ne1⁠; the given xy<1xy<1 guarantees that.
What to take away
  1. 2t1+t2=sin⁡2ϕ\frac{2t}{1+t^2}=\sin2\phi⁠, 1−t21+t2=cos⁡2ϕ\frac{1-t^2}{1+t^2}=\cos2\phi (and 2t1−t2=tan⁡2ϕ\frac{2t}{1-t^2}=\tan2\phi⁠) when t=tan⁡ϕt=\tan\phi⁠.
  2. Each condition in the question has a job. Here: ∣x∣<1|x|<1 for the sin⁡−1\sin^{-1} step, y>0y>0 for the cos⁡−1\cos^{-1} step, xy<1xy<1 for the final tangent.
  3. Always check the principal range before writing "inverse of function equals the angle".

Every fact used, and where it comes from

FactUsed inSource
sin⁡2ϕ=2sin⁡ϕcos⁡ϕ\sin2\phi=2\sin\phi\cos\phi⁠, cos⁡2ϕ=cos⁡2ϕ−sin⁡2ϕ\cos2\phi=\cos^2\phi-\sin^2\phi⁠, 1+tan⁡2ϕ=sec⁡2ϕ1+\tan^2\phi=\sec^2\phiStep 1Class XI, Chapter 3 (Trigonometric Functions)
sin⁡2ϕ=2tan⁡ϕ1+tan⁡2ϕ\sin2\phi=\frac{2\tan\phi}{1+\tan^2\phi}⁠, cos⁡2ϕ=1−tan⁡2ϕ1+tan⁡2ϕ\cos2\phi=\frac{1-\tan^2\phi}{1+\tan^2\phi}Steps 3, 4Derived in Step 1
Principal ranges of sin⁡−1\sin^{-1}⁠, cos⁡−1\cos^{-1}⁠, tan⁡−1\tan^{-1}Steps 2 to 4Table of principal value branches, Section 2.2 (Lesson: principal values)
sin⁡−1(sin⁡u)=u\sin^{-1}(\sin u)=u on [−π2,π2]\left[-\frac{\pi}{2},\frac{\pi}{2}\right]⁠; cos⁡−1(cos⁡u)=u\cos^{-1}(\cos u)=u on [0,π][0,\pi]Steps 3, 4Section 2.3
tan⁡(A+B)=tan⁡A+tan⁡B1−tan⁡Atan⁡B\tan(A+B)=\frac{\tan A+\tan B}{1-\tan A\tan B}Step 5Class XI, Chapter 3
tan⁡π4=1\tan\frac{\pi}{4}=1⁠; tan⁡−1\tan^{-1} is increasingStep 2Special angles; graph of tan⁡−1\tan^{-1}⁠, Fig 2.5 (ii)
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