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Original question & working

An inverse-trigonometric identity and its endpoints · source reference

2009/YJC/Prelim/I/5(a) · Question pp. 1 · Working pp. 2

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The working and teaching notes are included in the interactive lesson.

The printed derivative includes endpoints without saying one-sided. The identity itself holds on the closed interval.

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Printed question

(i) Show that ddx(cos⁡−12x1+x2)=−21+x2\frac{d}{dx}\left(\cos^{-1}\frac{2x}{1+x^2}\right)=\frac{-2}{1+x^2} for −1≤x≤1-1\le x\le1. Explain, in your working, how you use the condition −1≤x≤1-1\le x\le1 to conclude your answer. [3]

(ii) Hence, determine the constants AA and BB satisfying the equation cos⁡−12x1+x2+Atan⁡−1x=B\cos^{-1}\frac{2x}{1+x^2}+A\tan^{-1}x=B, for −1≤x≤1-1\le x\le1. [3]

[2009/YJC/Prelim/I/5(a)]

Printed working

(i)

ddx(cos⁡−12x1+x2)=−11−(2x1+x2)2((1+x2)(2)−(2x)(2x)(1+x2)2)=−(1+x2)(1+x2)2−4x2(2+2x2−4x2(1+x2)2)=−(2−2x2)1−2x2+x4(11+x2)=−2(1−x2)(1−x2)2(11+x2).\begin{aligned} \frac{d}{dx}\left(\cos^{-1}\frac{2x}{1+x^2}\right) &=\frac{-1}{\sqrt{1-(\frac{2x}{1+x^2})^2}}\left(\frac{(1+x^2)(2)-(2x)(2x)}{(1+x^2)^2}\right)\\ &=\frac{-(1+x^2)}{\sqrt{(1+x^2)^2-4x^2}}\left(\frac{2+2x^2-4x^2}{(1+x^2)^2}\right)\\ &=\frac{-(2-2x^2)}{\sqrt{1-2x^2+x^4}}\left(\frac1{1+x^2}\right)\\ &=\frac{-2(1-x^2)}{\sqrt{(1-x^2)^2}}\left(\frac1{1+x^2}\right). \end{aligned}

Note that

(1−x2)2={1−x2,1−x2≥0,−(1−x2),1−x2<0={1−x2,−1≤x≤1,−(1−x2),x<−1 or x>1.\sqrt{(1-x^2)^2}=\begin{cases}1-x^2,&1-x^2\ge0,\\-(1-x^2),&1-x^2<0\end{cases}=\begin{cases}1-x^2,&-1\le x\le1,\\-(1-x^2),&x<-1\text{ or }x>1.\end{cases}

Since it is given that −1≤x≤1-1\le x\le1, the printed cancellation gives −2(1−x2)1−x211+x2=−21+x2\frac{-2(1-x^2)}{1-x^2}\frac1{1+x^2}=\frac{-2}{1+x^2} (shown).

(ii) Differentiating the given identity with respect to xx,

−21+x2+A1+x2=0⇒A−21+x2=0⇒A−2=0⇒A=2.\frac{-2}{1+x^2}+\frac{A}{1+x^2}=0\Rightarrow\frac{A-2}{1+x^2}=0\Rightarrow A-2=0\Rightarrow A=2.

Thus cos⁡−12x1+x2+2tan⁡−1x=B\cos^{-1}\frac{2x}{1+x^2}+2\tan^{-1}x=B. Substituting x=0x=0 (which satisfies −1≤x≤1-1\le x\le1) gives cos⁡−1(0)+2tan⁡−10=B⇒B=π2\cos^{-1}(0)+2\tan^{-1}0=B\Rightarrow B=\frac\pi2.

Endpoint qualification

The ordinary two-sided derivative computation applies on −1<x<1-1<x<1. Cancellation at x=±1x=\pm1 divides by zero; the restricted identity is continuous on the closed interval and has the stated one-sided derivatives at its endpoints. The global composite has a cusp there, so a two-sided derivative at either endpoint does not exist.

Teacher notes

From MF26: ddx(cos⁡−1x)=−11−x2\frac{d}{dx}(\cos^{-1}x)=-\frac1{\sqrt{1-x^2}}.

Apply Chain Rule: let u=2x1+x2u=\frac{2x}{1+x^2}. Then ddx(cos⁡−1u)=ddu(cos⁡−1u)dudx=−11−u2dudx=−11−(2x1+x2)2ddx(2x1+x2)\frac{d}{dx}(\cos^{-1}u)=\frac{d}{du}(\cos^{-1}u)\frac{du}{dx}=-\frac1{\sqrt{1-u^2}}\frac{du}{dx}=-\frac1{\sqrt{1-(\frac{2x}{1+x^2})^2}}\frac{d}{dx}\left(\frac{2x}{1+x^2}\right). Apply quotient rule to this last derivative.

Answer key

(ii) A=2A=2, B=π2B=\frac\pi2.