Chapter 7 Class 12 Integrals
Serial order wise

The given integral ∫ f(x) dx can be transformed into another form by changing the independent variable x to t by substituting x=g(t)

 

Consider   I = ∫ f(x) dx

Put    x = g(t) so that dx/dt = g′(t)

We write  dx = g′ (t)dt

Thus  I = ∫ f(x) dx= ∫ f(g(t))  g′(t) dt

 

This change of variable formula is one of the important tools available to us in the name of integration by substitution.

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Question 1

∫ sin⁡ (tan -1 x)/(1 + x 2 ) dx is equal to:

(a) -sin⁡(tan -1 ⁡x + C 

(b) -cos⁡(tan -1 ⁡x + C

(c) tan⁡x + C 

(d) None of these

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Question 2

∫ tan⁡x  dx is equal to:

(a) sec⁡x + C    

(b) cot⁡x + C  

(c) log⁡|x| + C    

(d) None of these

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Question 3

∫ 2x/1 + x 2   dx is equal to:

(a) 1 + x 2 + C  

(b) log⁡ |1 + x 2 | + C

(c) log ⁡|2/1 + x 2 | + C 

(d) None of these

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Question 4

∫ sin⁡ (ax+b)  cos⁡ (ax+b)  dx is equal to:

(a) cos 2   x (ax + b) + C  

(b) sin 2 ⁡(ax + b)

(c) (-1)/4a  cos⁡2  (ax + b) + C 

(d) None of these

This question is inspired from Ex 7.2, 5 - Chapter 7 Class 12 - Integrals

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Question 5

∫ 1/x + x log⁡x  dx is equal to:

(a) |1 + log⁡x | + C 

(b) log⁡|1 + log⁡x| + C

(c) log⁡x + C 

(d) None of these

This question is inspired from Ex 7.2, 3 - Chapter 7 Class 12 - Integrals

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Transcript

Question 3 The given integral ∫1▒〖𝑓(π‘₯)γ€— 𝑑π‘₯ can be transformed into another form by changing the independent variable π‘₯ to 𝑑 by substituting π‘₯=𝑔(𝑑) Consider I = ∫1▒〖𝑓(π‘₯)γ€— 𝑑π‘₯ Put π‘₯ = 𝑔(𝑑) so that 𝑑π‘₯/𝑑𝑑=𝑔′(𝑑) We write 𝑑π‘₯=𝑔^β€² (𝑑)𝑑𝑑 Thus I = ∫1▒〖𝑓(π‘₯)γ€— 𝑑π‘₯= ∫1▒〖𝑓(𝑔(𝑑)) 𝑔^β€² (𝑑) 𝑑𝑑〗 This change of variable formula is one of the important tools available to us in the name of integration by substitution. For example: ∫1β–’γ€–2π‘₯ sin⁑〖(π‘₯^2+1)γ€— 𝑑π‘₯γ€— Put π‘₯^2+1=𝑑 2π‘₯𝑑π‘₯=𝑑𝑑 Thus, ∫1β–’γ€–sin⁑〖(𝑑) 𝑑𝑑〗=βˆ’cos⁑(𝑑)+𝐢〗 = βˆ’cos⁑〖(π‘₯^2+1)+𝐢〗 Based on the above information, answer any four of the following questions. Question 1 ∫1β–’γ€–sin⁑〖(tan^(βˆ’1)⁑π‘₯)γ€—/(1 + π‘₯^2 ) 𝑑π‘₯γ€— is equal to: (a) βˆ’sin⁑(tan^(βˆ’1)⁑π‘₯ )+𝐢 (b) βˆ’cos⁑(tan^(βˆ’1)⁑π‘₯ )+𝐢 (c) tan⁑π‘₯+𝐢 (d) None of these ∫1β–’γ€–sin⁑〖(tan^(βˆ’1)⁑π‘₯)γ€—/(1 + π‘₯^2 ) 𝑑π‘₯γ€— Let γ€–π­πšπ§γ€—^(βˆ’πŸ)⁑𝒙=𝒕 Differentiating both sides 𝑀.π‘Ÿ.𝑑.π‘₯ 𝟏/(𝟏 + 𝒙^𝟐 )= 𝒅𝒕/𝒅𝒙 𝑑π‘₯/(1 + π‘₯^2 )=𝑑𝑑 Now, Integrating the function ∫1β–’γ€–π’”π’Šπ’β‘γ€–(〖𝒕𝒂𝒏〗^(βˆ’πŸ)⁑𝒙)γ€—/(𝟏 + 𝒙^𝟐 ) 𝒅𝒙〗 Putting tan^(βˆ’1)⁑π‘₯=𝑑 & 𝑑π‘₯/(1 + π‘₯^2 )=𝑑𝑑 = ∫1▒〖𝐬𝐒𝐧⁑𝒕 . 𝒅𝒕〗 = βˆ’cos⁑𝑑+𝐢 Putting back t = tan^(βˆ’1)⁑π‘₯ = βˆ’πœπ¨π¬β‘γ€–(𝒕𝒂𝒏^(βˆ’πŸ) 𝒙)γ€—+π‘ͺ So, the correct answer is (b) Question 2 ∫1β–’γ€–tan⁑π‘₯ 𝑑π‘₯γ€— is equal to: (a) sec⁑π‘₯+𝐢 (b) cot⁑π‘₯+𝐢 (c) log⁑〖|π‘₯|γ€—+𝐢 (d) None of these ∫1β–’γ€–tan⁑π‘₯ 𝑑π‘₯γ€—=∫1β–’γ€–sin⁑π‘₯/cos⁑π‘₯ 𝑑π‘₯γ€— Let 𝒄𝒐𝒔⁑𝒙=𝒕 Differentiating both sides 𝑀.π‘Ÿ.𝑑.π‘₯ βˆ’π’”π’Šπ’ 𝒙= 𝒅𝒕/𝒅𝒙 sin x 𝑑π‘₯=βˆ’π‘‘π‘‘ Now, ∫1β–’(π’”π’Šπ’ 𝒙)/(𝒄𝒐𝒔 𝒙) 𝒅𝒙 Putting π‘π‘œπ‘ β‘π‘₯=𝑑 & sin⁑π‘₯ 𝑑π‘₯=𝑑𝑑 = ∫1β–’γ€–πŸ/𝒕 . (βˆ’π’…π’•)γ€— = βˆ’βˆ«1▒𝒅𝒕/𝒕 = βˆ’log⁑〖|𝑑|γ€—+𝐢 Putting back t = cos⁑π‘₯ = βˆ’π₯π¨π’ˆ |𝒄𝒐𝒔 𝒙|+π‘ͺ = lo𝑔 |π‘π‘œπ‘  π‘₯|^(βˆ’1)+𝐢 = lo𝑔 1/(|π‘π‘œπ‘  π‘₯|)+𝐢 = π₯π¨π’ˆ |𝒔𝒆𝒄 𝒙|+π‘ͺ So, the correct answer is (d) Question 3 ∫1β–’γ€–2π‘₯/(1 + π‘₯^2 ) 𝑑π‘₯γ€— is equal to: (a) 1+π‘₯^2+𝐢 (b) log⁑〖|1+π‘₯^2 |+𝐢〗 (c) log⁑|2/(1 + π‘₯^2 )|+𝐢 (d) None of these ∫1β–’γ€–2π‘₯/(1 + π‘₯^2 ) 𝑑π‘₯γ€— Let 𝟏+𝒙^𝟐=𝒕 Differentiating both sides 𝑀.π‘Ÿ.𝑑.π‘₯ πŸπ’™= 𝒅𝒕/𝒅𝒙 2π‘₯ 𝑑π‘₯=𝑑𝑑 Now, Integrating the function ∫1β–’γ€–πŸπ’™/(𝟏 + 𝒙^𝟐 ) 𝒅𝒙〗 Putting 1+π‘₯^2=𝑑 & 2π‘₯𝑑π‘₯=𝑑𝑑 = ∫1β–’γ€–πŸ/𝒕 . 𝒅𝒕〗 = log⁑〖|𝑑|γ€—+𝐢 Putting back t = 1+π‘₯^2 = π₯π’π’ˆ|𝟏+𝒙^𝟐 |+π‘ͺ So, the correct answer is (b) Question 4 ∫1β–’γ€–sin⁑〖(π‘Žπ‘₯+𝑏)γ€— cos⁑〖(π‘Žπ‘₯+𝑏)γ€— 𝑑π‘₯γ€— is equal to: (a) cos^2 π‘₯ (π‘Žπ‘₯+𝑏)+𝐢 (b) sin^2⁑〖(π‘Žπ‘₯+𝑏)γ€— (c) (βˆ’1)/4π‘Ž cos⁑2 (π‘Žπ‘₯+𝑏)+𝐢 (d) None of these Taking the given function π’”π’Šπ’β‘(𝒂𝒙 + 𝒃) 𝒄𝒐𝒔⁑(𝒂𝒙 + 𝒃) = 1/2 sin⁑(2(π‘Žπ‘₯+𝑏)) = 𝟏/𝟐 π’”π’Šπ’β‘(πŸπ’‚π’™+πŸπ’ƒ) Let (πŸπ’‚π’™+πŸπ’ƒ)=𝒕 Differentiating both sides 𝑀.π‘Ÿ.𝑑.π‘₯ 2π‘Ž+0=𝑑𝑑/𝑑π‘₯ 2π‘Ž=𝑑𝑑/𝑑π‘₯ 2π‘Ž.𝑑π‘₯=𝑑𝑑 𝒅𝒙=𝒅𝒕/πŸπ’‚ Integrating the function ∫1β–’γ€–" " sin⁑(π‘Žπ‘₯+𝑏) cos⁑(π‘Žπ‘₯+𝑏)" " γ€—.𝑑π‘₯ = 1/2 ∫1β–’γ€–sin⁑(2π‘Žπ‘₯+2𝑏)γ€— .𝑑π‘₯ Putting 𝑑=2π‘Žπ‘₯+2𝑏 & 𝑑π‘₯=𝑑𝑑/2π‘Ž = 𝟏/𝟐 ∫1β–’γ€–π’”π’Šπ’ 𝒕〗 .𝒅𝒕/πŸπ’‚ = 1/4π‘Ž ∫1β–’γ€–sin⁑(𝑑)γ€— .𝑑𝑑 = 1/4π‘Ž [βˆ’cos⁑𝑑+𝐢1] = βˆ’ 1/4π‘Ž . cos⁑𝑑 + 𝐢1/4π‘Ž = βˆ’ 𝟏/πŸ’π’‚ . 𝒄𝒐𝒔⁑𝒕 + π‘ͺ Putting back 𝑑=2π‘Žπ‘₯+2𝑏 = βˆ’ 1/4π‘Ž . cos⁑〖(2π‘Žπ‘₯+2𝑏)γ€— + 𝐢 = βˆ’ 𝟏/πŸ’π’‚ . π’„π’π’”β‘γ€–πŸ(𝒂𝒙+𝒃)γ€—+π‘ͺ So, the correct answer is (c) Question 5 ∫1β–’γ€–1/(π‘₯ + π‘₯ log⁑π‘₯ ) 𝑑π‘₯γ€— is equal to: (a) |1+log⁑π‘₯ |+𝐢 (b) log⁑〖|1+log⁑π‘₯ |+𝐢〗 (c) log⁑π‘₯+𝐢 (d) None of these ∫1β–’γ€–1/(π‘₯ + π‘₯ log⁑π‘₯ ) 𝑑π‘₯γ€— = ∫1β–’γ€–1/(π‘₯(1 + log⁑π‘₯)) 𝑑π‘₯γ€— Let 1 + log 𝒙= 𝒕 Differentiate 𝑀.π‘Ÿ.𝑑.π‘₯ 0 + 𝑑𝑑/𝑑π‘₯= 1/π‘₯ 0 + 𝑑𝑑/𝑑π‘₯= 1/π‘₯ 𝒅𝒕.𝒙=𝒅𝒙 Now, ∫1β–’1/(π‘₯ + π‘₯ log⁑π‘₯ ) .𝑑π‘₯ =∫1β–’1/(π‘₯ (1 + log⁑π‘₯ ) ) .𝑑π‘₯" " Putting 1+log⁑π‘₯ & 𝑑π‘₯=π‘₯ 𝑑𝑑 = ∫1β–’1/(π‘₯(𝑑)) 𝑑𝑑.π‘₯ = ∫1β–’1/𝑑 𝑑𝑑 = π‘™π‘œπ‘”|𝑑|+𝐢 Putting back 𝑑 =1+π‘™π‘œπ‘”β‘π‘₯ = π’π’π’ˆ|𝟏+π₯𝐨𝐠⁑𝒙 |+π‘ͺ So, the correct answer is (b)

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Davneet Singh has done his B.Tech from Indian Institute of Technology, Kanpur. He has been teaching from the past 14 years. He provides courses for Maths, Science and Computer Science at Teachoo