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Trigonometry -- Diagnostic Tests

flowchart TD
A[Diag Trigonometry] --> B[Key Concepts]
A --> C[Core Principles]
A --> D[Practical Applications]
B --> E[Fundamental definitions]
C --> F[Design patterns]
D --> G[Real-world usage]

Trigonometry is like a bridge between angles and lengths, sine, cosine, and tangent are the tools that connect them.

Tests edge cases, boundary conditions, and common misconceptions for trigonometry.

Question:

In triangle ABCABC, a=8a = 8, b=10b = 10 And A=35°A = 35°.

(a) Find the two possible values of angle BB Giving your answers to 1 decimal place.

(b) For each value of BB Find the corresponding value of angle CC and the length of side cc.

(c) Explain why a student who applies the cosine rule to find BB directly (without first finding cc) would fail to discover the ambiguous case.

[Difficulty: hard. Tests the ambiguous case of the sine rule where two valid triangles exist, and why alternative methods miss the second solution.]

Solution:

(a) By the sine rule:

sin⁡Bb=sin⁡Aa\frac{\sin B}{b} = \frac{\sin A}{a} sin⁡B=bsin⁡Aa=10sin⁡35°8=10×0.57368=0.7170\sin B = \frac{b \sin A}{a} = \frac{10 \sin 35°}{8} = \frac{10 \times 0.5736}{8} = 0.7170

Since sin⁡B=0.7170\sin B = 0.7170 and BB is an angle in a triangle (0°<B<180°0° \lt B \lt 180°), there are two solutions:

B1=arcsin⁡(0.7170)=45.8°B_1 = \arcsin(0.7170) = 45.8° B2=180°−45.8°=134.2°B_2 = 180° - 45.8° = 134.2°

Both are valid: B1+A=80.8°<180°B_1 + A = 80.8° \lt 180° and B2+A=169.2°<180°B_2 + A = 169.2° \lt 180°.

(b) For B1=45.8°B_1 = 45.8°:

C1=180°−35°−45.8°=99.2°C_1 = 180° - 35° - 45.8° = 99.2° c1=asin⁡C1sin⁡A=8sin⁡99.2°sin⁡35°=8×0.98630.5736=13.76c_1 = \frac{a \sin C_1}{\sin A} = \frac{8 \sin 99.2°}{\sin 35°} = \frac{8 \times 0.9863}{0.5736} = 13.76

For B2=134.2°B_2 = 134.2°:

C2=180°−35°−134.2°=10.8°C_2 = 180° - 35° - 134.2° = 10.8° c2=8sin⁡10.8°sin⁡35°=8×0.18740.5736=2.61c_2 = \frac{8 \sin 10.8°}{\sin 35°} = \frac{8 \times 0.1874}{0.5736} = 2.61

(c) The cosine rule for finding BB is cos⁡B=a2+c2−b22ac\cos B = \frac{a^2 + c^2 - b^2}{2ac}. This requires knowing cc Which is not given. The cosine rule is not directly applicable with the SSA (two sides and a non-included angle) configuration.

More fundamentally, cos⁡\cos is injective on (0°,180°)(0°, 180°) (it is strictly decreasing), so the cosine rule can only ever yield one value for BB. The ambiguity is an inherent property of the sine rule, because sin⁡\sin is symmetric about 90°90° on (0°,180°)(0°, 180°): sin⁡θ=sin⁡(180°−θ)\sin\theta = \sin(180° - \theta).


UT-2: Cancelling sin⁡θ\sin\theta When sin⁡θ=0\sin\theta = 0

Section titled “UT-2: Cancelling sin⁡θ\sin\thetasinθ When sin⁡θ=0\sin\theta = 0sinθ=0”

Question:

(a) Solve the equation sin⁡θ=2sin⁡θcos⁡θ\sin\theta = 2\sin\theta\cos\theta for θ∈[0°,360°)\theta \in [0°, 360°).

(b) A student”s working is shown below. Identify the error, state which solutions are lost, and explain why.

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

Dividing both sides by sin⁡θ\sin\theta:

1=2cos⁡θ1 = 2\cos\theta

cos⁡θ=12\cos\theta = \frac{1}{2}

θ=60°\theta = 60° or θ=300°\theta = 300°

(c) Find all solutions of tan⁡2x=tan⁡x\tan 2x = \tan x for x∈[0,π)x \in [0, \pi) Taking care not to lose solutions.

[Difficulty: hard. Tests the common error of dividing by a trigonometric expression that may equal zero, which systematically discards valid solutions.]

Solution:

(a) sin⁡θ=2sin⁡θcos⁡θ\sin\theta = 2\sin\theta\cos\theta

sin⁡θ−2sin⁡θcos⁡θ=0\sin\theta - 2\sin\theta\cos\theta = 0 sin⁡θ(1−2cos⁡θ)=0\sin\theta(1 - 2\cos\theta) = 0

Case 1: sin⁡θ=0  ⟹  θ=0°,180°,360°\sin\theta = 0 \implies \theta = 0°, 180°, 360°

Case 2: 1−2cos⁡θ=0  ⟹  cos⁡θ=12  ⟹  θ=60°,300°1 - 2\cos\theta = 0 \implies \cos\theta = \frac{1}{2} \implies \theta = 60°, 300°

All solutions: θ=0°,60°,180°,300°,360°\theta = 0°, 60°, 180°, 300°, 360°.

(b) The error is dividing both sides by sin⁡θ\sin\theta. This is only valid when sin⁡θ≠0\sin\theta \neq 0. By dividing, the student implicitly assumes sin⁡θ≠0\sin\theta \neq 0 Which discards the solutions θ=0°,180°,360°\theta = 0°, 180°, 360°. The correct approach is to factorise, not to divide.

(c) tan⁡2x=tan⁡x\tan 2x = \tan x for x∈[0,π)x \in [0, \pi).

First, establish the domain. Both tan⁡x\tan x and tan⁡2x\tan 2x must be defined:

  • tan⁡x\tan x undefined at x=π2x = \frac{\pi}{2}
  • tan⁡2x\tan 2x undefined at 2x=π22x = \frac{\pi}{2} and 2x=3π22x = \frac{3\pi}{2} I.e. x=π4x = \frac{\pi}{4} and x=3π4x = \frac{3\pi}{4}

So the domain excludes x=π4,π2,3π4x = \frac{\pi}{4}, \frac{\pi}{2}, \frac{3\pi}{4}.

Using the double angle formula tan⁡2x=2tan⁡x1−tan⁡2x\tan 2x = \frac{2\tan x}{1 - \tan^2 x}:

2tan⁡x1−tan⁡2x=tan⁡x\frac{2\tan x}{1 - \tan^2 x} = \tan x

Do NOT divide by tan⁡x\tan x. Bring everything to one side:

2tan⁡x−tan⁡x(1−tan⁡2x)1−tan⁡2x=0\frac{2\tan x - \tan x(1 - \tan^2 x)}{1 - \tan^2 x} = 0 tan⁡x+tan⁡3x1−tan⁡2x=0\frac{\tan x + \tan^3 x}{1 - \tan^2 x} = 0 tan⁡x(1+tan⁡2x)1−tan⁡2x=0\frac{\tan x(1 + \tan^2 x)}{1 - \tan^2 x} = 0

Since 1+tan⁡2x=sec⁡2x≥11 + \tan^2 x = \sec^2 x \geq 1 for all xx where tan⁡x\tan x is defined, the numerator is zero when tan⁡x=0\tan x = 0:

tan⁡x=0  ⟹  x=0\tan x = 0 \implies x = 0

(The solution x=πx = \pi is excluded by the interval [0,π)[0, \pi).)

Verify: tan⁡0=0\tan 0 = 0 and tan⁡0=0\tan 0 = 0. Confirmed.

Solution: x=0x = 0 only.


UT-3: Solving cos⁡(3x)=12\cos(3x) = \frac{1}{2} with Full Periodicity

Section titled “UT-3: Solving cos⁡(3x)=12\cos(3x) = \frac{1}{2}cos(3x)=21​ with Full Periodicity”

Question:

(a) Solve cos⁡(3x)=12\cos(3x) = \frac{1}{2} for x∈[0,2π)x \in [0, 2\pi). A common error produces only 2 or 4 solutions. Find all solutions.

(b) A student argues: ”cos⁡(3x)=12\cos(3x) = \frac{1}{2} means 3x=π33x = \frac{\pi}{3} or 3x=5π33x = \frac{5\pi}{3} Giving x=π9x = \frac{\pi}{9} or x=5π9x = \frac{5\pi}{9}.” Explain the error in this reasoning and state how many solutions the student is missing.

(c) The curve y=cos⁡(3x)y = \cos(3x) intersects the line y=12y = \frac{1}{2} at NN distinct points in the interval [0,2π)[0, 2\pi). Find NN and the sum of all xx-coordinates of the intersection points.

[Difficulty: hard. Tests understanding that multiplying the argument of a trigonometric function by a constant changes the period, requiring systematic enumeration of all solutions within the given interval.]

Solution:

(a) cos⁡(3x)=12\cos(3x) = \frac{1}{2}.

Let θ=3x\theta = 3x. Since x∈[0,2π)x \in [0, 2\pi) We have θ∈[0,6π)\theta \in [0, 6\pi).

cos⁡θ=12\cos\theta = \frac{1}{2} gives θ=π3+2nπ\theta = \frac{\pi}{3} + 2n\pi or θ=5π3+2nπ\theta = \frac{5\pi}{3} + 2n\pi for n∈Zn \in \mathbb{Z}.

Systematically listing all θ∈[0,6π)\theta \in [0, 6\pi):

nnθ=π3+2nπ\theta = \frac{\pi}{3} + 2n\piθ=5π3+2nπ\theta = \frac{5\pi}{3} + 2n\pi
0π3\frac{\pi}{3}5π3\frac{5\pi}{3}
17π3\frac{7\pi}{3}11π3\frac{11\pi}{3}
213π3\frac{13\pi}{3}17π3\frac{17\pi}{3}

All six values are in [0,6π)[0, 6\pi) since 17π3=523π<6π\frac{17\pi}{3} = 5\frac{2}{3}\pi \lt 6\pi.

Dividing by 3:

x=π9,5π9,7π9,11π9,13π9,17π9x = \frac{\pi}{9},\quad \frac{5\pi}{9},\quad \frac{7\pi}{9},\quad \frac{11\pi}{9},\quad \frac{13\pi}{9},\quad \frac{17\pi}{9}

(b) The student correctly identifies the principal solutions for 3x3x but fails to account for the fact that the period of cos⁡(3x)\cos(3x) is 2π3\frac{2\pi}{3} Not 2π2\pi. When xx ranges over [0,2π)[0, 2\pi) The argument 3x3x ranges over [0,6π)[0, 6\pi) Which spans three full periods of cosine. The student finds solutions from only the first period, missing the four solutions from the second and third periods. The student is missing 4 out of 6 solutions.

(c) N=6N = 6 (from part (a)).

The sum of all xx-coordinates:

S=π9+5π9+7π9+11π9+13π9+17π9=60π9=20π3S = \frac{\pi}{9} + \frac{5\pi}{9} + \frac{7\pi}{9} + \frac{11\pi}{9} + \frac{13\pi}{9} + \frac{17\pi}{9} = \frac{60\pi}{9} = \frac{20\pi}{3}

Tests synthesis of trigonometry with other topics. Requires combining concepts from multiple units.

Section titled “IT-1: Related Rates with Trigonometric Functions (with Differentiation)”

Question:

A ladder of length 5 metres is leaning against a vertical wall. The foot of the ladder is pulled away from the wall horizontally at a constant rate of 0.50.5 m/s.

(a) Find the rate at which the top of the ladder is sliding down the wall when the foot of the ladder is 3 metres from the wall.

(b) Find the angle θ\theta between the ladder and the ground at the instant when the top of the ladder is sliding down at the same speed as the foot is being pulled away.

(c) Show that θ\theta is always decreasing, and find the rate of change of θ\theta in rad/s when θ=π4\theta = \frac{\pi}{4}.

[Difficulty: hard. Combines implicit differentiation with trigonometric relationships in a kinematics context.]

Solution:

(a) Let xx be the distance from the foot of the ladder to the wall, and yy be the height of the top of the ladder above the ground.

By Pythagoras’ theorem: x2+y2=25x^2 + y^2 = 25.

Differentiating implicitly with respect to tt:

2xdxdt+2ydydt=0  ⟹  xdxdt+ydydt=02x\frac{dx}{dt} + 2y\frac{dy}{dt} = 0 \implies x\frac{dx}{dt} + y\frac{dy}{dt} = 0

Given dxdt=0.5\frac{dx}{dt} = 0.5. When x=3x = 3: y=25−9=4y = \sqrt{25 - 9} = 4.

3(0.5)+4dydt=0  ⟹  dydt=−38 m/s3(0.5) + 4\frac{dy}{dt} = 0 \implies \frac{dy}{dt} = -\frac{3}{8} \text{ m/s}

The negative sign confirms the top is sliding down.

(b) We need ∣dydt∣=∣dxdt∣=0.5\left\lvert\frac{dy}{dt}\right\rvert = \left\lvert\frac{dx}{dt}\right\rvert = 0.5.

From xdxdt+ydydt=0x\frac{dx}{dt} + y\frac{dy}{dt} = 0: dydt=−xydxdt\frac{dy}{dt} = -\frac{x}{y}\frac{dx}{dt}.

∣−xy⋅0.5∣=0.5  ⟹  xy=1  ⟹  x=y\left\lvert-\frac{x}{y} \cdot 0.5\right\rvert = 0.5 \implies \frac{x}{y} = 1 \implies x = y

Since x2+y2=25x^2 + y^2 = 25 and x=yx = y: 2x2=252x^2 = 25 So x=52x = \frac{5}{\sqrt{2}}.

cos⁡θ=x5=12\cos\theta = \frac{x}{5} = \frac{1}{\sqrt{2}} Giving θ=π4\theta = \frac{\pi}{4}.

(c) cos⁡θ=x5\cos\theta = \frac{x}{5}.

Differentiating with respect to tt:

−sin⁡θ⋅dθdt=15dxdt-\sin\theta \cdot \frac{d\theta}{dt} = \frac{1}{5}\frac{dx}{dt} dθdt=−15sin⁡θ⋅dxdt=−0.55sin⁡θ=−110sin⁡θ\frac{d\theta}{dt} = -\frac{1}{5\sin\theta} \cdot \frac{dx}{dt} = -\frac{0.5}{5\sin\theta} = -\frac{1}{10\sin\theta}

Since sin⁡θ>0\sin\theta \gt 0 for 0<θ<π0 \lt \theta \lt \pi We have dθdt<0\frac{d\theta}{dt} \lt 0 Confirming θ\theta is always decreasing.

When θ=π4\theta = \frac{\pi}{4}: sin⁡π4=12\sin\frac{\pi}{4} = \frac{1}{\sqrt{2}}.

dθdt=−110⋅12=−210 rad/s\frac{d\theta}{dt} = -\frac{1}{10 \cdot \frac{1}{\sqrt{2}}} = -\frac{\sqrt{2}}{10} \text{ rad/s}

IT-2: Area Enclosed by a Parametric Trigonometric Curve (with Coordinate Geometry)

Section titled “IT-2: Area Enclosed by a Parametric Trigonometric Curve (with Coordinate Geometry)”

Question:

A curve is defined parametrically by:

x=a(cos⁡t+cos⁡2t),y=a(sin⁡t+sin⁡2t)x = a(\cos t + \cos 2t), \quad y = a(\sin t + \sin 2t)

For 0≤t≤2π0 \leq t \leq 2\pi Where a>0a \gt 0.

(a) Show that the curve is closed.

(b) Find the total area enclosed by the curve, giving your answer in terms of aa.

(c) Find the coordinates of all points on the curve where the tangent is horizontal, giving exact answers in terms of aa.

[Difficulty: hard. Combines parametric differentiation, trigonometric identities, and definite integration for area under a parametric curve.]

Solution:

(a) At t=0t = 0: x=a(1+1)=2ax = a(1 + 1) = 2a, y=a(0+0)=0y = a(0 + 0) = 0.

At t=2πt = 2\pi: x=a(cos⁡2π+cos⁡4π)=a(1+1)=2ax = a(\cos 2\pi + \cos 4\pi) = a(1+1) = 2a, y=a(sin⁡2π+sin⁡4π)=0y = a(\sin 2\pi + \sin 4\pi) = 0.

The curve starts and ends at (2a,0)(2a, 0) So it is closed.

(b) The area enclosed by a parametric curve (x(t),y(t))(x(t), y(t)) traced once anticlockwise is:

A=∣∫02πydxdt dt∣A = \left\lvert\int_0^{2\pi} y\frac{dx}{dt}\, dt\right\rvert dxdt=a(−sin⁡t−2sin⁡2t)\frac{dx}{dt} = a(-\sin t - 2\sin 2t) ydxdt=a(sin⁡t+sin⁡2t)⋅a(−sin⁡t−2sin⁡2t)=−a2(sin⁡t+sin⁡2t)(sin⁡t+2sin⁡2t)y\frac{dx}{dt} = a(\sin t + \sin 2t) \cdot a(-\sin t - 2\sin 2t) = -a^2(\sin t + \sin 2t)(\sin t + 2\sin 2t)

Expanding:

=−a2[sin⁡2t+3sin⁡tsin⁡2t+2sin⁡22t]= -a^2[\sin^2 t + 3\sin t\sin 2t + 2\sin^2 2t]

Integrate each term separately over [0,2π][0, 2\pi]:

∫02πsin⁡2t dt=∫02π1−cos⁡2t2 dt=[t2−sin⁡2t4]02π=π\int_0^{2\pi}\sin^2 t\, dt = \int_0^{2\pi}\frac{1 - \cos 2t}{2}\, dt = \left[\frac{t}{2} - \frac{\sin 2t}{4}\right]_0^{2\pi} = \pi ∫02πsin⁡tsin⁡2t dt=∫02π2sin⁡2tcos⁡t dt=2[sin⁡3t3]02π=0\int_0^{2\pi}\sin t\sin 2t\, dt = \int_0^{2\pi}2\sin^2 t\cos t\, dt = 2\left[\frac{\sin^3 t}{3}\right]_0^{2\pi} = 0 ∫02πsin⁡22t dt=∫02π1−cos⁡4t2 dt=[t2−sin⁡4t8]02π=π\int_0^{2\pi}\sin^2 2t\, dt = \int_0^{2\pi}\frac{1 - \cos 4t}{2}\, dt = \left[\frac{t}{2} - \frac{\sin 4t}{8}\right]_0^{2\pi} = \pi

Therefore:

∫02πydxdt dt=−a2[π+3(0)+2π]=−3πa2\int_0^{2\pi} y\frac{dx}{dt}\, dt = -a^2[\pi + 3(0) + 2\pi] = -3\pi a^2 A=∣−3πa2∣=3πa2A = \lvert -3\pi a^2 \rvert = 3\pi a^2

(c) The tangent is horizontal when dydt=0\frac{dy}{dt} = 0 and dxdt≠0\frac{dx}{dt} \neq 0.

dydt=a(cos⁡t+2cos⁡2t)=0\frac{dy}{dt} = a(\cos t + 2\cos 2t) = 0 cos⁡t+2cos⁡2t=0\cos t + 2\cos 2t = 0

Using cos⁡2t=2cos⁡2t−1\cos 2t = 2\cos^2 t - 1:

cos⁡t+2(2cos⁡2t−1)=0  ⟹  4cos⁡2t+cos⁡t−2=0\cos t + 2(2\cos^2 t - 1) = 0 \implies 4\cos^2 t + \cos t - 2 = 0

Let u=cos⁡tu = \cos t:

u=−1±1+328=−1±338u = \frac{-1 \pm \sqrt{1 + 32}}{8} = \frac{-1 \pm \sqrt{33}}{8}

Both roots lie in [−1,1][-1, 1]: u1=33−18≈0.593u_1 = \frac{\sqrt{33}-1}{8} \approx 0.593 and u2=−33+18≈−0.843u_2 = -\frac{\sqrt{33}+1}{8} \approx -0.843.

Each gives two values of tt in [0,2π)[0, 2\pi) Producing four horizontal tangent points.

For u1=33−18u_1 = \frac{\sqrt{33}-1}{8}: t=±arccos⁡(33−18)t = \pm\arccos\left(\frac{\sqrt{33}-1}{8}\right). Substituting into xx and yy:

x=a(33−18)+a(2(33−18)2−1)x = a\left(\frac{\sqrt{33}-1}{8}\right) + a\left(2\left(\frac{\sqrt{33}-1}{8}\right)^2 - 1\right) =a(33−18+34−23332−1)=a⋅433−4+34−233−3232=a(33−1)16= a\left(\frac{\sqrt{33}-1}{8} + \frac{34-2\sqrt{33}}{32} - 1\right) = a \cdot \frac{4\sqrt{33}-4+34-2\sqrt{33}-32}{32} = \frac{a(\sqrt{33}-1)}{16}

By symmetry, the four horizontal tangent points are:

(a(33−1)16,±a1630+233)\left(\frac{a(\sqrt{33}-1)}{16},\quad \pm\frac{a}{16}\sqrt{30+2\sqrt{33}}\right) (−a(33+1)16,±a1630−233)\left(\frac{-a(\sqrt{33}+1)}{16},\quad \pm\frac{a}{16}\sqrt{30-2\sqrt{33}}\right)

IT-3: Inverse Trigonometric Composition and Domain Restrictions (with Functions)

Section titled “IT-3: Inverse Trigonometric Composition and Domain Restrictions (with Functions)”

Question:

The function ff is defined by f(x)=cos⁡xf(x) = \cos x on the domain [0,π2]\left[0, \frac{\pi}{2}\right].

(a) State the range of ff and explain why f−1f^{-1} exists on this domain.

(b) Let g(x)=arccos⁡xg(x) = \arccos x (principal inverse cosine, domain [−1,1][-1, 1] Range [0,π][0, \pi]). Find g(f(x))g(f(x)) and f(g(x))f(g(x)) Stating the domain of each composition.

(c) A student claims f−1(f(π))=πf^{-1}(f(\pi)) = \pi. Explain why this is incorrect.

(d) The function hh is defined by h(x)=arcsin⁡(cos⁡x)h(x) = \arcsin(\cos x) for x∈Rx \in \mathbb{R}. Express h(x)h(x) as a piecewise function and find all xx for which h(x)=xh(x) = x.

[Difficulty: hard. Tests the interplay between trigonometric functions and their inverses, requiring careful attention to domain and range restrictions.]

Solution:

(a) On [0,π2]\left[0, \frac{\pi}{2}\right], f′(x)=−sin⁡x<0f'(x) = -\sin x \lt 0 for 0<x<π20 \lt x \lt \frac{\pi}{2} So ff is strictly decreasing and therefore injective.

f(0)=1f(0) = 1 and f ⁣(π2)=0f\!\left(\frac{\pi}{2}\right) = 0 So the range is [0,1][0, 1].

Since ff is injective, f−1f^{-1} exists. Its domain is [0,1][0, 1] and its range is [0,π2]\left[0, \frac{\pi}{2}\right].

(b) g(f(x))=arccos⁡(cos⁡x)g(f(x)) = \arccos(\cos x): defined when cos⁡x∈[−1,1]\cos x \in [-1, 1] Which is always true. Domain: [0,π2]\left[0, \frac{\pi}{2}\right].

For x∈[0,π2]x \in \left[0, \frac{\pi}{2}\right]: since x∈[0,π]x \in [0, \pi] (the range of arccos⁡\arccos), we have arccos⁡(cos⁡x)=x\arccos(\cos x) = x. So g(f(x))=xg(f(x)) = x.

f(g(x))=cos⁡(arccos⁡x)f(g(x)) = \cos(\arccos x): defined when arccos⁡x∈[0,π2]\arccos x \in \left[0, \frac{\pi}{2}\right] I.e. x∈[0,1]x \in [0, 1].

For x∈[0,1]x \in [0, 1]: cos⁡(arccos⁡x)=x\cos(\arccos x) = x. So f(g(x))=xf(g(x)) = x.

The domains differ: g∘fg \circ f has domain [0,π2]\left[0, \frac{\pi}{2}\right] while f∘gf \circ g has domain [0,1][0, 1].

(c) π\pi is not in the domain of ff (which is [0,π2]\left[0, \frac{\pi}{2}\right]), so f(π)f(\pi) is undefined. The expression f−1(f(π))f^{-1}(f(\pi)) is therefore meaningless.

Even if ff were extended to R\mathbb{R} Then f(π)=−1f(\pi) = -1 But −1-1 is not in the domain of f−1f^{-1} (which is [0,1][0, 1] The range of ff on its original domain). So f−1(−1)f^{-1}(-1) would also be undefined.

(d) h(x)=arcsin⁡(cos⁡x)h(x) = \arcsin(\cos x). Using cos⁡x=sin⁡ ⁣(π2−x)\cos x = \sin\!\left(\frac{\pi}{2} - x\right):

h(x)=arcsin⁡ ⁣(sin⁡ ⁣(π2−x))h(x) = \arcsin\!\left(\sin\!\left(\frac{\pi}{2} - x\right)\right)

Since arcsin⁡(sin⁡θ)=θ\arcsin(\sin\theta) = \theta only when θ∈[−π2,π2]\theta \in \left[-\frac{\pi}{2}, \frac{\pi}{2}\right]:

When −π2≤π2−x≤π2-\frac{\pi}{2} \leq \frac{\pi}{2} - x \leq \frac{\pi}{2} I.e. 0≤x≤π0 \leq x \leq \pi: h(x)=π2−xh(x) = \frac{\pi}{2} - x.

When π≤x≤2π\pi \leq x \leq 2\pi: cos⁡x=cos⁡(2π−x)\cos x = \cos(2\pi - x) and 2π−x∈[0,π]2\pi - x \in [0, \pi] So h(x)=π2−(2π−x)=x−3π2h(x) = \frac{\pi}{2} - (2\pi - x) = x - \frac{3\pi}{2}.

By periodicity (period 2π2\pi):

h(x)={π2−x+2nπif 2nπ≤x≤(2n+1)πx−3π2+2nπif (2n+1)π≤x≤(2n+2)πh(x) = \begin{cases} \frac{\pi}{2} - x + 2n\pi & \text{if } 2n\pi \leq x \leq (2n+1)\pi \\ x - \frac{3\pi}{2} + 2n\pi & \text{if } (2n+1)\pi \leq x \leq (2n+2)\pi \end{cases}

For n∈Zn \in \mathbb{Z}.

To find h(x)=xh(x) = x: on [0,π][0, \pi], π2−x=x  ⟹  x=π4\frac{\pi}{2} - x = x \implies x = \frac{\pi}{4}.

On [π,2π][\pi, 2\pi]: x−3π2=x  ⟹  0=3π2x - \frac{3\pi}{2} = x \implies 0 = \frac{3\pi}{2} Impossible.

By periodicity: x=π4+2nπx = \frac{\pi}{4} + 2n\pi for n∈Zn \in \mathbb{Z}.