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Chapter 2 · Inverse Trigonometric Functions

Example 3: sin⁡−1(2x1−x2)\sin^{-1}\left(2x\sqrt{1-x^2}\right) in terms of sin⁡−1x\sin^{-1}x and cos⁡−1x\cos^{-1}x

ExamplesProperties and substitutions · Section 2.3
The question

Show that

(i)

sin⁡−1(2x1−x2)=2sin⁡−1x,−12≤x≤12\begin{gathered} \sin^{-1}\left(2x\sqrt{1-x^2}\right) = 2\sin^{-1}x, \\ -\dfrac{1}{\sqrt2} \le x \le \dfrac{1}{\sqrt2} \end{gathered}

(ii)

sin⁡−1(2x1−x2)=2cos⁡−1x,12≤x≤1\begin{gathered} \sin^{-1}\left(2x\sqrt{1-x^2}\right) = 2\cos^{-1}x, \\ \dfrac{1}{\sqrt2} \le x \le 1 \end{gathered}
Exam answer

(i) Let x=sin⁡θx = \sin\theta⁠, where θ=sin⁡−1x\theta = \sin^{-1}x⁠.

As −12≤x≤12-\frac{1}{\sqrt2} \le x \le \frac{1}{\sqrt2}⁠, −π4≤θ≤π4-\frac{\pi}{4} \le \theta \le \frac{\pi}{4}⁠.

So cos⁡θ>0\cos\theta \gt 0 and 1−x2=cos⁡θ\sqrt{1-x^2} = \cos\theta⁠.

Using sin⁡2θ=2sin⁡θcos⁡θ\sin 2\theta = 2\sin\theta\cos\theta⁠,

LHS=sin⁡−1(2x1−x2)=sin⁡−1(2sin⁡θcos⁡θ)=sin⁡−1(sin⁡2θ)=2θ[as −π2≤2θ≤π2]\begin{aligned} \text{LHS} &= \sin^{-1}\left(2x\sqrt{1-x^2}\right) \\ &= \sin^{-1}(2\sin\theta\cos\theta) \\ &= \sin^{-1}(\sin 2\theta) \\ &= 2\theta \quad[\text{as } {-\tfrac{\pi}{2}} \le 2\theta \le \tfrac{\pi}{2}] \end{aligned}

∴ LHS=2sin⁡−1x=RHS\therefore\ \text{LHS} = 2\sin^{-1}x = \text{RHS}⁠. Hence proved.

(ii) Let x=cos⁡θx = \cos\theta⁠, where θ=cos⁡−1x\theta = \cos^{-1}x⁠.

As 12≤x≤1\frac{1}{\sqrt2} \le x \le 1⁠, 0≤θ≤π40 \le \theta \le \frac{\pi}{4}⁠.

So sin⁡θ≥0\sin\theta \ge 0 and 1−x2=sin⁡θ\sqrt{1-x^2} = \sin\theta⁠.

Using sin⁡2θ=2sin⁡θcos⁡θ\sin 2\theta = 2\sin\theta\cos\theta⁠,

LHS=sin⁡−1(2x1−x2)=sin⁡−1(2cos⁡θsin⁡θ)=sin⁡−1(sin⁡2θ)=2θ[as 0≤2θ≤π2]\begin{aligned} \text{LHS} &= \sin^{-1}\left(2x\sqrt{1-x^2}\right) \\ &= \sin^{-1}(2\cos\theta\sin\theta) \\ &= \sin^{-1}(\sin 2\theta) \\ &= 2\theta \quad[\text{as } 0 \le 2\theta \le \tfrac{\pi}{2}] \end{aligned}

∴ LHS=2cos⁡−1x=RHS\therefore\ \text{LHS} = 2\cos^{-1}x = \text{RHS}⁠. Hence proved.

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

The one idea this problem is built on

The expression 2x1−x22x\sqrt{1-x^2} is the double-angle formula 2sin⁡θcos⁡θ=sin⁡2θ2\sin\theta\cos\theta = \sin2\theta in disguise: put x=sin⁡θx = \sin\theta (or x=cos⁡θx=\cos\theta⁠) and the square root becomes the other trig function. The inside then collapses to sin⁡2θ\sin 2\theta⁠, and sin⁡−1(sin⁡2θ)=2θ\sin^{-1}(\sin2\theta) = 2\theta⁠. But that last cancellation is only allowed when 2θ2\theta lies in [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠. The intervals in the question are exactly the values of xx that make this true, which is why the answer changes from 2sin⁡−1x2\sin^{-1}x to 2cos⁡−1x2\cos^{-1}x at x=12x = \frac{1}{\sqrt2}⁠.

Given, to show, and the plan
Given
The expression sin⁡−1(2x1−x2)\sin^{-1}\left(2x\sqrt{1-x^2}\right) and two intervals of xx⁠.
To show
It equals 2sin⁡−1x2\sin^{-1}x on [−12,12]\left[-\frac{1}{\sqrt2}, \frac{1}{\sqrt2}\right]⁠, and equals 2cos⁡−1x2\cos^{-1}x on [12,1]\left[\frac{1}{\sqrt2}, 1\right]⁠.
Plan
For each part: (1) substitute an angle θ\theta and find the interval θ\theta lies in; (2) simplify the square root, choosing its sign from that interval; (3) use the double-angle formula; (4) cancel sin⁡−1(sin⁡ ⋅)\sin^{-1}(\sin\,\cdot)⁠, after checking that 2θ2\theta is in [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠. Finally, see why the formula of one part fails on the other interval.

Basics you need

1sin⁡−1(sin⁡t)=t\sin^{-1}(\sin t) = t only on the principal range

sin⁡−1(sin⁡t)=t\sin^{-1}(\sin t) = t holds when −π2≤t≤π2-\frac{\pi}{2}\le t\le\frac{\pi}{2}⁠, because sin⁡−1\sin^{-1} always returns a value in that interval. For other tt it is false: sin⁡−1(sin⁡π)=sin⁡−10=0\sin^{-1}(\sin\pi) = \sin^{-1}0 = 0⁠, not π\pi⁠. Lesson: sin⁻¹(sin x) and the folding rules

2The square root of a square

a2=∣a∣\sqrt{a^2} = |a|⁠, never simply aa⁠. It equals aa only when a≥0a \ge 0⁠. For example (−3)2=3\sqrt{(-3)^2} = 3⁠.

3Pythagorean identity and double angle

sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1⁠, so 1−sin⁡2θ=cos⁡2θ1-\sin^2\theta = \cos^2\theta and 1−cos⁡2θ=sin⁡2θ1-\cos^2\theta = \sin^2\theta⁠. Also sin⁡2θ=2sin⁡θcos⁡θ\sin2\theta = 2\sin\theta\cos\theta⁠. Basics: sin and cos on the unit circle

4Signs of sin and cos

cos⁡θ≥0\cos\theta \ge 0 for θ∈[−π2,π2]\theta\in\left[-\frac{\pi}{2}, \frac{\pi}{2}\right] (right half of the circle), and sin⁡θ≥0\sin\theta\ge0 for θ∈[0,π]\theta\in[0,\pi] (upper half). Basics: domain and range of sin and cos

5Substituting x=sin⁡θx = \sin\theta or x=cos⁡θx = \cos\theta

Every xx in [−1,1][-1,1] equals sin⁡θ\sin\theta for exactly one θ=sin⁡−1x\theta = \sin^{-1}x in [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠, and equals cos⁡θ\cos\theta for exactly one θ=cos⁡−1x\theta = \cos^{-1}x in [0,π][0,\pi]⁠. So these substitutions lose nothing. Lesson: substitutions and simplest form

Part (i): −12≤x≤12-\frac{1}{\sqrt2}\le x\le\frac{1}{\sqrt2}

  1. Substitute x=sin⁡θx = \sin\theta and locate θ\theta

    Let θ=sin⁡−1x\theta = \sin^{-1}x⁠. Then x=sin⁡θx = \sin\theta⁠, and θ\theta is in [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠. We can say more. Since sin⁡−1\sin^{-1} is increasing, applying it to

    −12≤x≤12-\frac{1}{\sqrt2} \le x \le \frac{1}{\sqrt2}

    keeps the inequalities, and sin⁡−1(±12)=±π4\sin^{-1}\left(\pm\frac{1}{\sqrt2}\right) = \pm\frac{\pi}{4}⁠. So

    −π4≤θ≤π4.-\frac{\pi}{4} \le \theta \le \frac{\pi}{4}.
    The textbook says "Let x=sin⁡θx = \sin\theta⁠. Then sin⁡−1x=θ\sin^{-1}x = \theta⁠." That second sentence is only true if θ\theta is chosen in [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠, so we define θ\theta as sin⁡−1x\sin^{-1}x⁠. Pinning θ\theta down to [−π4,π4]\left[-\frac{\pi}{4}, \frac{\pi}{4}\right] is the key fact for the whole part: Steps 2 and 4 both depend on it.
    An increasing function keeps the order of inequalities: if a≤x≤ba\le x\le b then f(a)≤f(x)≤f(b)f(a)\le f(x)\le f(b)⁠. sin⁡−1\sin^{-1} is increasing on [−1,1][-1,1] because sine is increasing on [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠. Lesson: graphs of the inverse functions
  2. Simplify the square root, with the correct sign

    1−x2=1−sin⁡2θ=cos⁡2θ=∣cos⁡θ∣=cos⁡θ.\begin{aligned} \sqrt{1-x^2} &= \sqrt{1-\sin^2\theta} = \sqrt{\cos^2\theta} \\ &= |\cos\theta| = \cos\theta. \end{aligned}

    The last equality holds because θ∈[−π4,π4]\theta\in\left[-\frac{\pi}{4}, \frac{\pi}{4}\right] is on the right half of the unit circle, where cos⁡θ≥0\cos\theta\ge0 (in fact cos⁡θ≥12\cos\theta\ge\frac{1}{\sqrt2}⁠).

    The textbook writes 1−sin⁡2θ=cos⁡θ\sqrt{1-\sin^2\theta} = \cos\theta without comment. That step needs cos⁡θ≥0\cos\theta\ge0⁠. If cos⁡θ\cos\theta were negative, the square root (which is never negative) would equal −cos⁡θ-\cos\theta instead, and every later line would change sign.
    a2=∣a∣\sqrt{a^2} = |a| (Basic 2), and 1−sin⁡2θ=cos⁡2θ1-\sin^2\theta = \cos^2\theta (Basic 3).
  3. Recognise the double-angle formula

    2x1−x2=2sin⁡θcos⁡θ=sin⁡2θ.2x\sqrt{1-x^2} = 2\sin\theta\cos\theta = \sin2\theta.

    So the expression we must simplify is

    sin⁡−1(2x1−x2)=sin⁡−1(sin⁡2θ).\sin^{-1}\left(2x\sqrt{1-x^2}\right) = \sin^{-1}(\sin 2\theta).
    This is the reason for choosing x=sin⁡θx = \sin\theta in the first place: xx becomes sin⁡θ\sin\theta⁠, 1−x2\sqrt{1-x^2} becomes cos⁡θ\cos\theta⁠, and the product 2sin⁡θcos⁡θ2\sin\theta\cos\theta is a single trig function of a single angle. It also shows that the left-hand side is always defined: sin⁡2θ\sin2\theta lies in [−1,1][-1,1]⁠, the domain of sin⁡−1\sin^{-1}⁠.
    sin⁡2θ=2sin⁡θcos⁡θ\sin2\theta = 2\sin\theta\cos\theta (Class XI, Basic 3).
  4. Cancel sin⁡−1(sin⁡ ⋅)\sin^{-1}(\sin\,\cdot)⁠, after checking 2θ2\theta

    Doubling −π4≤θ≤π4-\frac{\pi}{4}\le\theta\le\frac{\pi}{4} gives

    −π2≤2θ≤π2.-\frac{\pi}{2} \le 2\theta \le \frac{\pi}{2}.

    So 2θ2\theta is in the principal range of sin⁡−1\sin^{-1}⁠, and by Basic 1

    sin⁡−1(sin⁡2θ)=2θ=2sin⁡−1x.\sin^{-1}(\sin2\theta) = 2\theta = 2\sin^{-1}x.

    This proves sin⁡−1(2x1−x2)=2sin⁡−1x\sin^{-1}\left(2x\sqrt{1-x^2}\right) = 2\sin^{-1}x for −12≤x≤12-\frac{1}{\sqrt2}\le x\le\frac{1}{\sqrt2}⁠.

    This is the step the interval in the question exists for. sin⁡−1\sin^{-1} can only return angles between −π2-\frac{\pi}{2} and π2\frac{\pi}{2}⁠, so sin⁡−1(sin⁡2θ)\sin^{-1}(\sin2\theta) can only equal 2θ2\theta when 2θ2\theta is itself in that range. With ∣θ∣≤π4|\theta|\le\frac{\pi}{4}⁠, it is. The final substitution θ=sin⁡−1x\theta = \sin^{-1}x comes straight from Step 1.
    sin⁡−1(sin⁡t)=t\sin^{-1}(\sin t) = t for t∈[−π2,π2]t\in\left[-\frac{\pi}{2}, \frac{\pi}{2}\right] (Section 2.3). Lesson: sin⁻¹(sin x)

Part (ii): 12≤x≤1\frac{1}{\sqrt2}\le x\le 1

  1. Substitute x=cos⁡θx = \cos\theta and locate θ\theta

    Let θ=cos⁡−1x\theta = \cos^{-1}x⁠. Then x=cos⁡θx = \cos\theta and θ∈[0,π]\theta\in[0,\pi]⁠. Since cos⁡−1\cos^{-1} is decreasing, applying it to 12≤x≤1\frac{1}{\sqrt2}\le x\le1 reverses the inequalities. With cos⁡−11=0\cos^{-1}1 = 0 and cos⁡−112=π4\cos^{-1}\frac{1}{\sqrt2} = \frac{\pi}{4}⁠:

    0≤θ≤π4.0 \le \theta \le \frac{\pi}{4}.
    The textbook just says "Take x=cos⁡θx = \cos\theta⁠, then proceeding as above". We fill in what "as above" requires. We use cosine this time because the target answer is 2cos⁡−1x2\cos^{-1}x⁠, so we want θ\theta to be cos⁡−1x\cos^{-1}x⁠. As in Part (i), we define θ=cos⁡−1x\theta = \cos^{-1}x so that θ\theta is in [0,π][0,\pi] and the step "cos⁡−1x=θ\cos^{-1}x = \theta" is legitimate.
    A decreasing function reverses inequalities: larger xx gives smaller cos⁡−1x\cos^{-1}x⁠. On the unit circle, a point further right (larger cos⁡\cos⁠) on the upper half is at a smaller angle. Lesson: principal values
  2. Simplify the square root, with the correct sign

    1−x2=1−cos⁡2θ=sin⁡2θ=∣sin⁡θ∣=sin⁡θ.\begin{aligned} \sqrt{1-x^2} &= \sqrt{1-\cos^2\theta} = \sqrt{\sin^2\theta} \\ &= |\sin\theta| = \sin\theta. \end{aligned}

    The last equality holds because θ∈[0,π4]\theta\in\left[0, \frac{\pi}{4}\right] is on the upper half of the circle, where sin⁡θ≥0\sin\theta\ge0⁠.

    Same care as Part (i), Step 2. Here the sign is guaranteed by the range [0,π][0,\pi] of cos⁡−1\cos^{-1} alone: sine is never negative on the upper half of the circle.
    1−cos⁡2θ=sin⁡2θ1-\cos^2\theta = \sin^2\theta and a2=∣a∣\sqrt{a^2}=|a|⁠.
  3. Recognise the double-angle formula

    2x1−x2=2cos⁡θsin⁡θ=sin⁡2θ,2x\sqrt{1-x^2} = 2\cos\theta\sin\theta = \sin2\theta,

    so sin⁡−1(2x1−x2)=sin⁡−1(sin⁡2θ)\sin^{-1}\left(2x\sqrt{1-x^2}\right) = \sin^{-1}(\sin2\theta)⁠.

    The two factors have swapped roles compared with Part (i): now xx is the cosine and the square root is the sine. The product 2sin⁡θcos⁡θ2\sin\theta\cos\theta does not care about the order.
  4. Cancel sin⁡−1(sin⁡ ⋅)\sin^{-1}(\sin\,\cdot)⁠, after checking 2θ2\theta

    Doubling 0≤θ≤π40\le\theta\le\frac{\pi}{4} gives 0≤2θ≤π20\le2\theta\le\frac{\pi}{2}⁠, which is inside [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠. Therefore

    sin⁡−1(sin⁡2θ)=2θ=2cos⁡−1x.\sin^{-1}(\sin2\theta) = 2\theta = 2\cos^{-1}x.

    This proves sin⁡−1(2x1−x2)=2cos⁡−1x\sin^{-1}\left(2x\sqrt{1-x^2}\right) = 2\cos^{-1}x for 12≤x≤1\frac{1}{\sqrt2}\le x\le1⁠.

    Again the interval in the question is exactly what is needed. For θ=cos⁡−1x\theta = \cos^{-1}x⁠, the condition 2θ≤π22\theta\le\frac{\pi}{2} means θ≤π4\theta\le\frac{\pi}{4}⁠, which means x≥12x\ge\frac{1}{\sqrt2}⁠. For smaller xx this cancellation would be invalid.
    sin⁡−1(sin⁡t)=t\sin^{-1}(\sin t) = t for t∈[−π2,π2]t\in\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠.
  5. Why two different formulas are needed

    Try the Part (i) formula on the Part (ii) interval, at x=0.8x = 0.8⁠. Then 2x1−x2=2(0.8)(0.6)=0.962x\sqrt{1-x^2} = 2(0.8)(0.6) = 0.96⁠, and

    sin⁡−1(0.96)≈1.287002,2sin⁡−1(0.8)≈1.854590,2cos⁡−1(0.8)≈1.287002.\begin{aligned} \sin^{-1}(0.96) &\approx 1.287002, \\ 2\sin^{-1}(0.8) &\approx 1.854590, \\ 2\cos^{-1}(0.8) &\approx 1.287002. \end{aligned}

    So 2sin⁡−1x2\sin^{-1}x is wrong here and 2cos⁡−1x2\cos^{-1}x is right. The reason: for x>12x>\frac{1}{\sqrt2}⁠, θ=sin⁡−1x\theta = \sin^{-1}x is more than π4\frac{\pi}{4}⁠, so 2sin⁡−1x2\sin^{-1}x is more than π2\frac{\pi}{2}⁠, which sin⁡−1\sin^{-1} can never output. (Indeed 1.854590>π2≈1.5707961.854590 > \frac{\pi}{2}\approx1.570796⁠.)

    π π/2 −π/2 −π −1 −1/√2 0 1/√2 1 x thick blue: sin⁻¹(2x√(1 − x²)) dashed gold: 2 sin⁻¹x matches on the gold band −1/√2 ≤ x ≤ 1/√2 dashed green: 2 cos⁻¹x matches on the green band 1/√2 ≤ x ≤ 1 the blue curve never leaves [−π/2, π/2]
    Horizontal and vertical scales differ. The blue curve y=sin⁡−1(2x1−x2)y=\sin^{-1}\left(2x\sqrt{1-x^2}\right) stays in [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠. It follows 2sin⁡−1x2\sin^{-1}x (gold) on the gold band and 2cos⁡−1x2\cos^{-1}x (green) on the green band; at x=12x = \frac{1}{\sqrt2} both equal π2\frac{\pi}{2}⁠, where the curve turns down.
    The two answers agree at the shared endpoint x=12x = \frac{1}{\sqrt2}⁠: 2sin⁡−112=π2=2cos⁡−1122\sin^{-1}\frac{1}{\sqrt2} = \frac{\pi}{2} = 2\cos^{-1}\frac{1}{\sqrt2}⁠. That is a useful check that the two parts fit together. On the far left, for −1≤x<−12-1\le x<-\frac{1}{\sqrt2}⁠, neither formula holds (the curve there is −π−2sin⁡−1x-\pi - 2\sin^{-1}x⁠), which is why the question does not mention that interval.
    The values 2sin⁡−1x2\sin^{-1}x cover [−π,π][-\pi,\pi] but sin⁡−1\sin^{-1} only outputs [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠; whenever a proposed answer can leave the principal range, it cannot be right everywhere. Lesson: the folding rules
Result

(i) For −12≤x≤12-\frac{1}{\sqrt2}\le x\le\frac{1}{\sqrt2}⁠, with θ=sin⁡−1x\theta = \sin^{-1}x in [−π4,π4]\left[-\frac{\pi}{4}, \frac{\pi}{4}\right]⁠:

sin⁡−1(2x1−x2)=sin⁡−1(sin⁡2θ)=2sin⁡−1x.\begin{aligned} \sin^{-1}\left(2x\sqrt{1-x^2}\right) &= \sin^{-1}(\sin2\theta) \\ &= 2\sin^{-1}x. \end{aligned}

(ii) For 12≤x≤1\frac{1}{\sqrt2}\le x\le1⁠, with θ=cos⁡−1x\theta = \cos^{-1}x in [0,π4]\left[0, \frac{\pi}{4}\right]⁠:

sin⁡−1(2x1−x2)=sin⁡−1(sin⁡2θ)=2cos⁡−1x.\begin{aligned} \sin^{-1}\left(2x\sqrt{1-x^2}\right) &= \sin^{-1}(\sin2\theta) \\ &= 2\cos^{-1}x. \end{aligned}

Both agree with the textbook.

Check it with numbers

Part (i), x=0.5x = 0.5⁠: 2(0.5)0.75≈0.8660252(0.5)\sqrt{0.75} \approx 0.866025⁠, and sin⁡−1(0.866025)≈1.047198\sin^{-1}(0.866025)\approx1.047198⁠. Also 2sin⁡−1(0.5)=2(0.523599)2\sin^{-1}(0.5) = 2(0.523599) =1.047198= 1.047198⁠. Equal (both are π3\frac{\pi}{3}⁠).

Part (i), x=−0.6x = -0.6⁠: 2(−0.6)(0.8)=−0.962(-0.6)(0.8) = -0.96⁠, and sin⁡−1(−0.96)≈−1.287002\sin^{-1}(-0.96)\approx-1.287002⁠. Also 2sin⁡−1(−0.6)=2(−0.643501)2\sin^{-1}(-0.6) = 2(-0.643501) =−1.287002= -1.287002⁠. Equal.

Part (ii), x=0.8x = 0.8⁠: sin⁡−1(0.96)≈1.287002\sin^{-1}(0.96)\approx1.287002 and 2cos⁡−1(0.8)=2(0.643501)2\cos^{-1}(0.8) = 2(0.643501) =1.287002= 1.287002⁠. Equal.

Common mistakes
  1. Writing 1−sin⁡2θ=cos⁡θ\sqrt{1-\sin^2\theta} = \cos\theta without a reason. It is ∣cos⁡θ∣|\cos\theta|⁠. You must say why cos⁡θ≥0\cos\theta\ge0 on your interval.
  2. Cancelling sin⁡−1(sin⁡2θ)=2θ\sin^{-1}(\sin2\theta) = 2\theta automatically. It needs 2θ∈[−π2,π2]2\theta\in\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠. Forgetting this is how people "prove" Part (i) for all x∈[−1,1]x\in[-1,1]⁠, which is false (Part (ii), Step 5).
  3. Letting θ\theta be "any" angle with sin⁡θ=x\sin\theta = x⁠. Then sin⁡−1x=θ\sin^{-1}x = \theta may fail (sin⁡3π4=12\sin\frac{3\pi}{4} = \frac{1}{\sqrt2} but sin⁡−112=π4\sin^{-1}\frac{1}{\sqrt2} = \frac{\pi}{4}⁠). Define θ=sin⁡−1x\theta = \sin^{-1}x⁠.
  4. Forgetting that cos⁡−1\cos^{-1} reverses inequalities. 12≤x≤1\frac{1}{\sqrt2}\le x\le1 gives 0≤θ≤π40\le\theta\le\frac{\pi}{4}⁠, not π4≤θ≤0\frac{\pi}{4}\le\theta\le0⁠.
What to take away
  1. When you see 1−x2\sqrt{1-x^2}⁠, try x=sin⁡θx = \sin\theta or x=cos⁡θx = \cos\theta⁠. When you see 2x1−x22x\sqrt{1-x^2}⁠, expect sin⁡2θ\sin2\theta⁠.
  2. Every inverse-trig simplification has three checks: where θ\theta lies, the sign of each square root, and whether the final angle is in the principal range. The stated interval is what makes all three work.

Every fact used, and where it comes from

FactUsed inSource
sin⁡−1x=θ  ⟺  x=sin⁡θ\sin^{-1}x = \theta \iff x = \sin\theta with θ∈[−π2,π2]\theta\in\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]Part (i), Step 1Section 2.2; Section 2.3 (Lesson: substitutions)
cos⁡−1:[−1,1]→[0,π]\cos^{-1} : [-1,1]\to[0,\pi]⁠, decreasingPart (ii), Step 1Section 2.2, Fig 2.2
sin⁡−112=π4\sin^{-1}\frac{1}{\sqrt2} = \frac{\pi}{4}⁠, cos⁡−112=π4\cos^{-1}\frac{1}{\sqrt2} = \frac{\pi}{4}Step 1 of each partExample 1; special angles
a2=∣a∣\sqrt{a^2}=|a|⁠; sin⁡2θ+cos⁡2θ=1\sin^2\theta+\cos^2\theta=1Step 2 of each partAlgebra; Class XI
sin⁡2θ=2sin⁡θcos⁡θ\sin2\theta = 2\sin\theta\cos\thetaStep 3 of each partClass XI double-angle formula
sin⁡−1(sin⁡t)=t\sin^{-1}(\sin t) = t for t∈[−π2,π2]t\in\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]Step 4 of each partSection 2.3 (Lesson: sin⁻¹(sin x))
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