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Chapter 2 · Inverse Trigonometric Functions

Exercise 2.2 · Q3: Simplest form of tan⁡−11+x2−1x\tan^{-1}\frac{\sqrt{1+x^2}-1}{x}

Exercise 2.2Simplest form by substitution · Section 2.3
The question

Write the following function in the simplest form:

tan⁡−11+x2−1x,x≠0.\tan^{-1}\frac{\sqrt{1+x^2}-1}{x}, \qquad x \ne 0.
Exam answer

Let y=tan⁡−11+x2−1xy = \tan^{-1}\frac{\sqrt{1+x^2}-1}{x}⁠.

Put x=tan⁡θx = \tan\theta⁠, where θ=tan⁡−1x\theta = \tan^{-1}x⁠.

Then −π2<θ<π2-\frac{\pi}{2} \lt \theta \lt \frac{\pi}{2} and θ≠0\theta \ne 0 (as x≠0x \ne 0⁠).

So sec⁡θ>0\sec\theta \gt 0 and 1+x2=sec⁡θ\sqrt{1+x^2} = \sec\theta⁠.

Using 1−cos⁡θ=2sin⁡2θ21 - \cos\theta = 2\sin^2\frac{\theta}{2} and sin⁡θ=2sin⁡θ2cos⁡θ2\sin\theta = 2\sin\frac{\theta}{2}\cos\frac{\theta}{2}⁠,

1+x2−1x=sec⁡θ−1tan⁡θ=1−cos⁡θsin⁡θ=2sin⁡2θ22sin⁡θ2cos⁡θ2=tan⁡θ2\begin{aligned} \frac{\sqrt{1+x^2}-1}{x} &= \frac{\sec\theta - 1}{\tan\theta} \\ &= \frac{1 - \cos\theta}{\sin\theta} \\ &= \frac{2\sin^2\frac{\theta}{2}}{2\sin\frac{\theta}{2}\cos\frac{\theta}{2}} \\ &= \tan\frac{\theta}{2} \end{aligned} y=tan⁡−1(tan⁡θ2)=θ2[as −π4<θ2<π4]\begin{aligned} y &= \tan^{-1}\left(\tan\frac{\theta}{2}\right) \\ &= \frac{\theta}{2} \quad[\text{as } {-\tfrac{\pi}{4}} \lt \tfrac{\theta}{2} \lt \tfrac{\pi}{4}] \end{aligned}

∴ y=12tan⁡−1x\therefore\ y = \dfrac12\tan^{-1}x⁠.

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

The one idea this problem is built on

The expression 1+x2\sqrt{1+x^2} is a signal: if x=tan⁡θx = \tan\theta⁠, then 1+x2=sec⁡2θ1 + x^2 = \sec^2\theta and the square root disappears. The fraction then turns into 1−cos⁡θsin⁡θ\frac{1-\cos\theta}{\sin\theta}⁠, which a half-angle formula turns into tan⁡θ2\tan\frac{\theta}{2}⁠. Because θ2\frac{\theta}{2} always lies in (−π4,π4)\left(-\frac{\pi}{4}, \frac{\pi}{4}\right)⁠, well inside the principal range of tan⁡−1\tan^{-1}⁠, the answer is θ2=12tan⁡−1x\frac{\theta}{2} = \frac12\tan^{-1}x for every x≠0x \ne 0⁠.

Given, to find, and the plan
Given
The function tan⁡−11+x2−1x\tan^{-1}\frac{\sqrt{1+x^2}-1}{x} for real x≠0x \ne 0⁠.
To find
A simpler expression equal to it for all such xx⁠.
Plan
(1) Put θ=tan⁡−1x\theta = \tan^{-1}x⁠. (2) Remove the square root, taking care with its sign. (3) Simplify the fraction to 1−cos⁡θsin⁡θ\frac{1-\cos\theta}{\sin\theta}⁠. (4) Derive the half-angle formulas and get tan⁡θ2\tan\frac{\theta}{2}⁠. (5) Check θ2\frac{\theta}{2} is in the principal range and conclude. (6) Cross-check by algebra.

Basics you need

1The principal branch of tan⁡−1\tan^{-1}

tan⁡−1\tan^{-1} is defined for every real number, with range (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right)⁠, an open interval. tan⁡−1(tan⁡y)=y\tan^{-1}(\tan y) = y exactly when yy is in that interval. Basics: tan, cot, sec and cosec

2a2=∣a∣\sqrt{a^2} = |a|

A square root is never negative. So sec⁡2θ=∣sec⁡θ∣\sqrt{\sec^2\theta} = |\sec\theta|⁠, which equals sec⁡θ\sec\theta only when sec⁡θ>0\sec\theta \gt 0⁠.

3Pythagorean identity for tan

Dividing sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1 by cos⁡2θ\cos^2\theta gives 1+tan⁡2θ=sec⁡2θ1 + \tan^2\theta = \sec^2\theta⁠. Basics: sin and cos on the unit circle

4Double-angle formulas

sin⁡2u=2sin⁡ucos⁡u\sin 2u = 2\sin u\cos u and cos⁡2u=1−2sin⁡2u\cos 2u = 1 - 2\sin^2 u⁠. Read "backwards" with u=θ2u = \frac{\theta}{2}⁠, they become half-angle formulas.

Solution

  1. Substitute x=tan⁡θx = \tan\theta

    Let θ=tan⁡−1x\theta = \tan^{-1}x⁠. This is defined for every real xx⁠, and

    tan⁡θ=x,θ∈(−π2,π2).\tan\theta = x, \qquad \theta \in \left(-\frac{\pi}{2}, \frac{\pi}{2}\right).

    Since x≠0x \ne 0⁠, also θ≠0\theta \ne 0⁠.

    1+x21 + x^2 under a root is the pattern 1+tan⁡2θ=sec⁡2θ1 + \tan^2\theta = \sec^2\theta⁠. Using θ=tan⁡−1x\theta = \tan^{-1}x (not any other angle with tangent xx⁠) gives us its interval, which we need in the next step and in Step 5.
    tan⁡(tan⁡−1x)=x\tan(\tan^{-1}x) = x for all real xx⁠. Lesson: substitutions and simplest form
  2. Remove the square root, with the right sign

    1+x2=1+tan⁡2θ=sec⁡2θ=∣sec⁡θ∣.\sqrt{1+x^2} = \sqrt{1+\tan^2\theta} = \sqrt{\sec^2\theta} = |\sec\theta|.

    For θ∈(−π2,π2)\theta \in \left(-\frac{\pi}{2}, \frac{\pi}{2}\right) we have cos⁡θ>0\cos\theta \gt 0⁠, so sec⁡θ>0\sec\theta \gt 0 and ∣sec⁡θ∣=sec⁡θ|\sec\theta| = \sec\theta⁠. Therefore

    1+x2−1x=sec⁡θ−1tan⁡θ.\frac{\sqrt{1+x^2}-1}{x} = \frac{\sec\theta - 1}{\tan\theta}.
    This is where the principal range first matters. If θ\theta were, say, between π2\frac{\pi}{2} and π\pi⁠, then sec⁡θ\sec\theta would be negative and sec⁡2θ\sqrt{\sec^2\theta} would be −sec⁡θ-\sec\theta⁠. Writing sec⁡θ\sec\theta there would be wrong.
    a2=∣a∣\sqrt{a^2} = |a| (Basic 2); cosine is positive in the first and fourth quadrants. Basics: sin and cos on the unit circle
  3. Write everything with sin and cos

    Multiply top and bottom by cos⁡θ\cos\theta (which is not 0):

    sec⁡θ−1tan⁡θ=1cos⁡θ−1sin⁡θcos⁡θ=1−cos⁡θsin⁡θ.\frac{\sec\theta - 1}{\tan\theta} = \frac{\frac{1}{\cos\theta} - 1}{\frac{\sin\theta}{\cos\theta}} = \frac{1 - \cos\theta}{\sin\theta}.

    The denominator sin⁡θ\sin\theta is not 0, because θ≠0\theta \ne 0 and θ∈(−π2,π2)\theta \in \left(-\frac{\pi}{2}, \frac{\pi}{2}\right)⁠.

    Clearing the small fractions leaves a form in which a standard identity is recognisable. Checking that we never divide by zero is part of the job: cos⁡θ≠0\cos\theta \ne 0 by the interval, sin⁡θ≠0\sin\theta \ne 0 because x≠0x \ne 0⁠. This is exactly why the question says x≠0x \ne 0⁠.
  4. Derive the half-angle forms and simplify

    Put u=θ2u = \frac{\theta}{2}⁠, so θ=2u\theta = 2u⁠. The double-angle formulas give

    1−cos⁡θ=1−(1−2sin⁡2u)=2sin⁡2θ2,1 - \cos\theta = 1 - (1 - 2\sin^2 u) = 2\sin^2\frac{\theta}{2}, sin⁡θ=2sin⁡θ2cos⁡θ2.\sin\theta = 2\sin\frac{\theta}{2}\cos\frac{\theta}{2}.

    Hence

    1−cos⁡θsin⁡θ=2sin⁡2θ22sin⁡θ2cos⁡θ2=sin⁡θ2cos⁡θ2=tan⁡θ2.\begin{aligned} \frac{1-\cos\theta}{\sin\theta} &= \frac{2\sin^2\frac{\theta}{2}}{2\sin\frac{\theta}{2}\cos\frac{\theta}{2}} \\ &= \frac{\sin\frac{\theta}{2}}{\cos\frac{\theta}{2}} = \tan\frac{\theta}{2}. \end{aligned}

    The cancellation is allowed: θ2∈(−π4,π4)\frac{\theta}{2} \in \left(-\frac{\pi}{4}, \frac{\pi}{4}\right) and θ2≠0\frac{\theta}{2} \ne 0⁠, so neither sin⁡θ2\sin\frac{\theta}{2} nor cos⁡θ2\cos\frac{\theta}{2} is 0.

    The "1 minus cos" in the numerator is the clue: cos⁡θ=1−2sin⁡2θ2\cos\theta = 1 - 2\sin^2\frac{\theta}{2} is the version of the double-angle formula that makes the 1 cancel. Writing sin⁡θ\sin\theta also in terms of θ2\frac{\theta}{2} lets a common factor 2sin⁡θ22\sin\frac{\theta}{2} cancel.
    cos⁡2u=1−2sin⁡2u\cos 2u = 1 - 2\sin^2 u⁠, sin⁡2u=2sin⁡ucos⁡u\sin 2u = 2\sin u\cos u (Basic 4), Class XI trigonometry.
  5. Check the principal range and conclude

    The function is now tan⁡−1(tan⁡θ2)\tan^{-1}\left(\tan\frac{\theta}{2}\right)⁠. Since −π2<θ<π2-\frac{\pi}{2} \lt \theta \lt \frac{\pi}{2}⁠,

    −π4<θ2<π4,-\frac{\pi}{4} \lt \frac{\theta}{2} \lt \frac{\pi}{4},

    which lies inside (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right)⁠. So tan⁡−1(tan⁡θ2)=θ2\tan^{-1}\left(\tan\frac{\theta}{2}\right) = \frac{\theta}{2}⁠, and

    tan⁡−11+x2−1x=θ2=12tan⁡−1x.\tan^{-1}\frac{\sqrt{1+x^2}-1}{x} = \frac{\theta}{2} = \frac12\tan^{-1}x.

    This holds for every real x≠0x \ne 0⁠. There is no further restriction, because halving an angle of (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right) can never leave that interval.

    Unlike Q1 and Q2, nothing goes wrong anywhere in the stated domain. The only excluded point is x=0x = 0⁠, where the expression is 00\frac{0}{0} and is simply undefined (the answer 12tan⁡−10=0\frac12\tan^{-1}0 = 0 is its limiting value there).
    tan⁡−1(tan⁡y)=y\tan^{-1}(\tan y) = y for y∈(−π2,π2)y\in\left(-\frac{\pi}{2}, \frac{\pi}{2}\right)⁠. Lesson: sin⁻¹(sin x) and the folding rules
  6. An algebra cross-check

    Multiply top and bottom by 1+x2+1\sqrt{1+x^2} + 1⁠:

    1+x2−1x=(1+x2)−1x(1+x2+1)=x1+x2+1.\begin{aligned} \frac{\sqrt{1+x^2}-1}{x} &= \frac{(1+x^2) - 1}{x\left(\sqrt{1+x^2}+1\right)} \\ &= \frac{x}{\sqrt{1+x^2}+1}. \end{aligned}

    The denominator is greater than ∣x∣|x|⁠, so this number lies strictly between −1-1 and 11 and has the same sign as xx⁠. So tan⁡−1\tan^{-1} of it lies in (−π4,π4)\left(-\frac{\pi}{4}, \frac{\pi}{4}\right)⁠, matching the range of 12tan⁡−1x\frac12\tan^{-1}x⁠.

    −π/4 π/4 −6 −4 −2 2 4 6 blue: (1/2) tan⁻¹x gold dashed: the given expression hole at x = 0 (0/0)
    The given expression (gold, dashed) and 12tan⁡−1x\frac12\tan^{-1}x (blue) for −6≤x≤6-6 \le x \le 6⁠: the curves lie on top of each other. Both stay between −π4-\frac{\pi}{4} and π4\frac{\pi}{4}⁠. The open circle is the excluded point x=0x = 0⁠.
    A second, independent route catches mistakes. Here it confirms the sign and the size of the answer without any trigonometry.
    Rationalising: (a−b)(a+b)=a2−b2(a-b)(a+b) = a^2 - b^2 removes a square root from a numerator.
Result

For every real x≠0x \ne 0⁠:

tan⁡−11+x2−1x=12tan⁡−1x.\tan^{-1}\frac{\sqrt{1+x^2}-1}{x} = \frac12\tan^{-1}x. (Textbook answer: 12tan⁡−1x\frac12\tan^{-1}x⁠.)

Check it with numbers

x=2x = 2⁠: 5=2.236068\sqrt5 = 2.236068⁠, so the fraction is 1.2360682=0.618034\frac{1.236068}{2} = 0.618034 and tan⁡−10.618034=0.553574\tan^{-1}0.618034 = 0.553574⁠. Also 12tan⁡−12=0.553574\frac12\tan^{-1}2 = 0.553574⁠. ✓

x=−12x = -\frac12 (a negative value): 1.25=1.118034\sqrt{1.25} = 1.118034⁠, fraction 0.118034−0.5=−0.236068\frac{0.118034}{-0.5} = -0.236068⁠, tan⁡−1(−0.236068)=−0.231824\tan^{-1}(-0.236068) = -0.231824⁠, and 12tan⁡−1(−0.5)=−0.231824\frac12\tan^{-1}(-0.5) = -0.231824⁠. ✓

Common mistakes
  1. Writing sec⁡2θ=sec⁡θ\sqrt{\sec^2\theta} = \sec\theta without a reason. It is ∣sec⁡θ∣|\sec\theta|⁠; it equals sec⁡θ\sec\theta here only because θ∈(−π2,π2)\theta \in \left(-\frac{\pi}{2}, \frac{\pi}{2}\right)⁠.
  2. Using the wrong half-angle formula. 1−cos⁡θ=2sin⁡2θ21 - \cos\theta = 2\sin^2\frac{\theta}{2}⁠, while 1+cos⁡θ=2cos⁡2θ21 + \cos\theta = 2\cos^2\frac{\theta}{2}⁠.
  3. Answering tan⁡−1x2\tan^{-1}\frac{x}{2}⁠. The half is outside the tan⁡−1\tan^{-1}⁠: 12tan⁡−1x\frac12\tan^{-1}x⁠. At x=2x = 2⁠: tan⁡−11=0.785398\tan^{-1}1 = 0.785398⁠, not 0.5535740.553574⁠.
What to take away
  1. 1+x2\sqrt{1+x^2} suggests x=tan⁡θx = \tan\theta⁠; 1−x2\sqrt{1-x^2} suggests x=sin⁡θx = \sin\theta or cos⁡θ\cos\theta⁠; x2−1\sqrt{x^2-1} suggests x=sec⁡θx = \sec\theta⁠.
  2. 1−cos⁡θsin⁡θ=tan⁡θ2\frac{1-\cos\theta}{\sin\theta} = \tan\frac{\theta}{2} is worth remembering.
  3. Halving an angle keeps it in the principal range of tan⁡−1\tan^{-1}⁠, so this identity has no hidden restriction.

Every fact used, and where it comes from

FactUsed inSource
Principal branch of tan⁡−1\tan^{-1}⁠: domain R\R⁠, range (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right)Steps 1, 5Section 2.2, table of principal value branches (Lesson: principal values)
1+tan⁡2θ=sec⁡2θ1 + \tan^2\theta = \sec^2\theta⁠; a2=∣a∣\sqrt{a^2} = |a|Step 2Class XI trigonometry; definition of square root
cos⁡2u=1−2sin⁡2u\cos 2u = 1-2\sin^2u⁠, sin⁡2u=2sin⁡ucos⁡u\sin 2u = 2\sin u\cos uStep 4Class XI trigonometry
tan⁡−1(tan⁡y)=y\tan^{-1}(\tan y) = y for y∈(−π2,π2)y\in\left(-\frac{\pi}{2}, \frac{\pi}{2}\right)Step 5Section 2.3
Answer 12tan⁡−1x\frac12\tan^{-1}xResultAnswers to Exercise 2.2, Q3
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