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CBSE Sample Paper 2023-24 · Section C · 3 marks

Q28: Find ∫x1−x3 dx\int\sqrt{\frac{x}{1 - x^3}}\,dx⁠, or evaluate ∫0π4log⁡(1+tan⁡x) dx\int_0^{\frac{\pi}{4}}\log(1 + \tan x)\,dx

Sample 2023-24Ch 7 · Integrals
The question

(a) Find : ∫x1−x3 dx\displaystyle\int\sqrt{\frac{x}{1 - x^3}}\,dx⁠; x∈(0,1)x \in (0, 1)⁠.

OR

(b) Evaluate: ∫0π4log⁡(1+tan⁡x) dx\displaystyle\int_0^{\frac{\pi}{4}}\log(1 + \tan x)\,dx⁠.

Exam answer

(a)

Let x32=tx^{\frac32} = t⁠, so x3=t2x^3 = t^2 and

Why?

Write the integrand as x1−x3\frac{\sqrt x}{\sqrt{1 - x^3}}⁠. Two things suggest t=x32t = x^{\frac32}⁠:

x3=(x32)2=t2x^3 = \left(x^{\frac32}\right)^2 = t^2⁠, so the bottom becomes 1−t2\sqrt{1 - t^2}⁠, a standard form.

The derivative of x32x^{\frac32} contains x12=xx^{\frac12} = \sqrt x⁠, which is exactly the top.

dt=32x12 dx⇒x dx=23 dtdt = \frac32x^{\frac12}\,dx \Rightarrow \sqrt x\,dx = \frac23\,dt
Why?

Power rule: ddxx32=32x32−1=32x12\frac{d}{dx}x^{\frac32} = \frac32x^{\frac32 - 1} = \frac32x^{\frac12}⁠.

Multiply both sides by 23\frac23 to get x dx\sqrt x\,dx on its own.

dt=32x12 dx23 dt=23⋅32x12 dx23 dt=x12 dx(23⋅32=1)23 dt=x dx\begin{aligned} dt &= \frac32x^{\frac12}\,dx \\ \frac23\,dt &= \frac23 \cdot \frac32x^{\frac12}\,dx \\ \frac23\,dt &= x^{\frac12}\,dx \quad \left(\frac23 \cdot \frac32 = 1\right) \\ \frac23\,dt &= \sqrt x\,dx \end{aligned}
∫x1−x3 dx=∫x dx1−x3=23∫dt1−t2=23sin⁡−1(t)+c\begin{aligned} \int\sqrt{\frac{x}{1 - x^3}}\,dx &= \int\frac{\sqrt x\,dx}{\sqrt{1 - x^3}} \\ &= \frac23\int\frac{dt}{\sqrt{1 - t^2}} \\ &= \frac23\sin^{-1}(t) + c \end{aligned}
Why?

Since x∈(0,1)x \in (0, 1)⁠, both xx and 1−x31 - x^3 are positive, so the root of the fraction splits into a root on top and a root below.

Now replace x dx\sqrt x\,dx by 23 dt\frac23\,dt and x3x^3 by t2t^2⁠:

∫x dx1−x3=∫23 dt1−t2=23∫dt1−t2\begin{aligned} \int\frac{\sqrt x\,dx}{\sqrt{1 - x^3}} &= \int\frac{\frac23\,dt}{\sqrt{1 - t^2}} \\ &= \frac23\int\frac{dt}{\sqrt{1 - t^2}} \end{aligned}

The standard integral used is

∫dt1−t2=sin⁡−1t+c\int\frac{dt}{\sqrt{1 - t^2}} = \sin^{-1}t + c

Finally put t=x32t = x^{\frac32} back, so the answer is in xx⁠.

=23sin⁡−1(x32)+c= \frac23\sin^{-1}\left(x^{\frac32}\right) + c⁠, where cc is an arbitrary constant of integration.

(b)

I=∫0π4log⁡(1+tan⁡x) dx…(i)I = \int_0^{\frac{\pi}{4}}\log(1 + \tan x)\,dx\quad\ldots(\text{i})
Why?

log⁡(1+tan⁡x)\log(1 + \tan x) has no standard antiderivative. The plan is to use a property that brings the same integral II back on the right side, and then solve for II⁠. That is why it is named and labelled (i).

Using ∫0af(x) dx=∫0af(a−x) dx\int_0^a f(x)\,dx = \int_0^a f(a - x)\,dx⁠,

I=∫0π4log⁡(1+tan⁡(π4−x))dx=∫0π4log⁡(1+1−tan⁡x1+tan⁡x)dx\begin{aligned} I &= \int_0^{\frac{\pi}{4}}\log\left(1 + \tan\left(\frac{\pi}{4} - x\right)\right)dx \\ &= \int_0^{\frac{\pi}{4}}\log\left(1 + \frac{1 - \tan x}{1 + \tan x}\right)dx \end{aligned}
Why?

Here a=π4a = \frac{\pi}{4}⁠, so every xx is replaced by π4−x\frac{\pi}{4} - x⁠.

Then use the formula

tan⁡(A−B)=tan⁡A−tan⁡B1+tan⁡Atan⁡B\begin{aligned} &\tan(A - B) \\ &= \frac{\tan A - \tan B}{1 + \tan A\tan B} \end{aligned}

with A=π4A = \frac{\pi}{4}⁠, tan⁡π4=1\tan\frac{\pi}{4} = 1 and B=xB = x⁠.

tan⁡(π4−x)=1−tan⁡x1+(1)tan⁡x=1−tan⁡x1+tan⁡x\begin{aligned} \tan\left(\frac{\pi}{4} - x\right) &= \frac{1 - \tan x}{1 + (1)\tan x} \\ &= \frac{1 - \tan x}{1 + \tan x} \end{aligned}
I=∫0π4log⁡(21+tan⁡x)dx=∫0π4log⁡2 dx−∫0π4log⁡(1+tan⁡x) dx=π4log⁡2−I[using (i)]\begin{aligned} I &= \int_0^{\frac{\pi}{4}}\log\left(\frac{2}{1 + \tan x}\right)dx \\ &= \int_0^{\frac{\pi}{4}}\log 2\,dx \\ &\quad - \int_0^{\frac{\pi}{4}}\log(1 + \tan x)\,dx \\ &= \frac{\pi}{4}\log 2 - I \quad[\text{using (i)}] \end{aligned}
Why?

Add the fractions inside the log over the common denominator 1+tan⁡x1 + \tan x⁠:

(1+tan⁡x)+(1−tan⁡x)1+tan⁡x=21+tan⁡x\begin{aligned} &\frac{(1 + \tan x) + (1 - \tan x)}{1 + \tan x} \\ &= \frac{2}{1 + \tan x} \end{aligned}

Then log⁡mn=log⁡m−log⁡n\log\frac{m}{n} = \log m - \log n splits the integral in two.

log⁡(21+tan⁡x)=log⁡2−log⁡(1+tan⁡x)\begin{aligned} &\log\left(\frac{2}{1 + \tan x}\right) \\ &= \log 2 - \log(1 + \tan x) \end{aligned}

log⁡2\log 2 is a constant, so its integral is log⁡2×(π4−0)\log 2 \times \left(\frac{\pi}{4} - 0\right)⁠. The second integral is II itself, by (i).

⇒2I=π4log⁡2\Rightarrow 2I = \frac{\pi}{4}\log 2
Why?

Move −I-I to the left: I+I=2II + I = 2I⁠. Then divide by 2.

I=π4log⁡2−II+I=π4log⁡2(add I)2I=π4log⁡2I=π4×2log⁡2=π8log⁡2\begin{aligned} I &= \frac{\pi}{4}\log 2 - I \\ I + I &= \frac{\pi}{4}\log 2 \quad (\text{add } I) \\ 2I &= \frac{\pi}{4}\log 2 \\ I &= \frac{\pi}{4 \times 2}\log 2 = \frac{\pi}{8}\log 2 \end{aligned}

Watch out: do not try to integrate log⁡(1+tan⁡x)\log(1 + \tan x) directly. The property does all the work.

∴ I=π8log⁡2\therefore\ I = \dfrac{\pi}{8}\log 2⁠.

Where this comes from

Chapter 7, Integrals: Integration by substitution; f(a − x) property.

Question type: (a) Substitution; (b) Limits from 0 to aa

How to spot it: click to see

(a) Type 2. Substitution: when the derivative is hiding in the question

Spot it: a function and its derivative both appear, like log⁡x\log x and 1x\frac{1}{x}⁠, or x2+1x^2 + 1 and xx⁠.

Here: Write the integrand as x1−x3\frac{\sqrt x}{\sqrt{1 - x^3}}⁠. Since x3=(x3/2)2x^3 = (x^{3/2})^2⁠, and the derivative of x3/2x^{3/2} brings out the x\sqrt x on top, put x3/2=tx^{3/2} = t⁠: the integral becomes 23∫dt1−t2\frac23\int\frac{dt}{\sqrt{1 - t^2}}⁠.

(b) Type 12. Limits from 0 to aa⁠: the f(a−x)f(a - x) trick

Spot it: replacing xx by a−xa - x swaps the parts of the question, like sin and cos when aa is π2\frac{\pi}{2}⁠.

Here: With a=π4a = \frac{\pi}{4}⁠, replacing xx by π4−x\frac{\pi}{4} - x turns 1+tan⁡x1 + \tan x into 21+tan⁡x\frac{2}{1 + \tan x}⁠. The log then splits into log⁡2\log 2 minus the original integrand, so I=π4log⁡2−II = \frac{\pi}{4}\log 2 - I⁠.

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