Chapter 7 Class 12 Integrals
Concept wise

Ex 7.10, 16 - Evaluate definite integral log (1 + cos x) dx - Ex 7.10

part 2 - Ex 7.10, 16 - Ex 7.10 - Serial order wise - Chapter 7 Class 12 Integrals
part 3 - Ex 7.10, 16 - Ex 7.10 - Serial order wise - Chapter 7 Class 12 Integrals part 4 - Ex 7.10, 16 - Ex 7.10 - Serial order wise - Chapter 7 Class 12 Integrals part 5 - Ex 7.10, 16 - Ex 7.10 - Serial order wise - Chapter 7 Class 12 Integrals part 6 - Ex 7.10, 16 - Ex 7.10 - Serial order wise - Chapter 7 Class 12 Integrals part 7 - Ex 7.10, 16 - Ex 7.10 - Serial order wise - Chapter 7 Class 12 Integrals part 8 - Ex 7.10, 16 - Ex 7.10 - Serial order wise - Chapter 7 Class 12 Integrals part 9 - Ex 7.10, 16 - Ex 7.10 - Serial order wise - Chapter 7 Class 12 Integrals

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Ex 7.10, 16 By using the properties of definite integrals, evaluate the integrals : ∫_0^πœ‹β–’log⁑(1+cos⁑π‘₯ ) 𝑑π‘₯ Let I=∫_𝟎^π…β–’π’π’π’ˆβ‘(𝟏+𝒄𝒐𝒔⁑𝒙 ) 𝒅𝒙 ∴ I=∫_0^πœ‹β–’log⁑(1+π‘π‘œπ‘ (πœ‹βˆ’π‘₯)) 𝑑π‘₯ 𝐈=∫_𝟎^𝝅▒π₯𝐨𝐠⁑(πŸβˆ’π’„π’π’”β‘π’™ ) 𝑑π‘₯ Adding (1) and (2) i.e. (1) + (2) I+I=∫_0^πœ‹β–’π‘™π‘œπ‘”(1+cos⁑π‘₯ )𝑑π‘₯+∫_0^πœ‹β–’π‘™π‘œπ‘”(1βˆ’cos⁑π‘₯ )𝑑π‘₯ 𝟐𝐈=∫_𝟎^𝝅▒[π’π’π’ˆ(𝟏+𝒄𝒐𝒔⁑𝒙 )+π’π’π’ˆ(πŸβˆ’π’„π’π’”β‘π’™ )]𝒅𝒙 "Using log(a) + log(b)" = "log(a.b)") 2I=∫_0^πœ‹β–’π’π’π’ˆ[(𝟏+𝒄𝒐𝒔⁑𝒙 )(πŸβˆ’π’„π’π’”β‘π’™ )]𝒅𝒙 2I=∫_0^πœ‹β–’π‘™π‘œπ‘”[1βˆ’cos^2⁑π‘₯ ]𝑑π‘₯ 2I=∫_0^πœ‹β–’π‘™π‘œπ‘”(〖𝑠𝑖𝑛〗^2⁑π‘₯ )𝑑π‘₯ Using log 𝒂^𝒃=𝒃 π’π’π’ˆβ‘π’‚ 2I=∫_0^πœ‹β–’γ€–2 π‘™π‘œπ‘”(𝑠𝑖𝑛⁑π‘₯ )𝑑π‘₯γ€— 2I=2∫_0^πœ‹β–’π‘™π‘œπ‘”(𝑠𝑖𝑛⁑π‘₯ )𝑑π‘₯ 𝐈=∫_𝟎^π…β–’π’π’π’ˆ(π’”π’Šπ’β‘π’™ )𝒅𝒙 Here, 𝒇(𝒙)=log⁑sin⁑π‘₯ f(π…βˆ’π’™)=π‘™π‘œπ‘”[𝑠𝑖𝑛(πœ‹βˆ’π‘₯)]𝑑π‘₯ =π‘™π‘œπ‘”(sin⁑π‘₯ )𝑑π‘₯ =𝒇(𝒙) Therefore, I=∫_𝟎^π…β–’π’π’π’ˆ(𝐬𝐒𝐧⁑𝒙 )𝒅𝒙=𝟐∫_𝟎^(𝝅/𝟐)β–’π’π’π’ˆ(π’”π’Šπ’β‘π’™ )𝒅𝒙 Let I1=∫_0^(πœ‹/2 )β–’π‘™π‘œπ‘”(𝑠𝑖𝑛π‘₯) 𝑑π‘₯ Solving 𝐈𝟏 I1=∫_0^(πœ‹/2 )β–’π‘™π‘œπ‘”(𝑠𝑖𝑛π‘₯) 𝑑π‘₯ ∴ I1=∫_𝟎^(𝝅/𝟐)β–’π’”π’Šπ’(𝝅/πŸβˆ’π’™)𝒅𝒙 I1= ∫_𝟎^(𝝅/𝟐)β–’π’π’π’ˆ(𝒄𝒐𝒔⁑𝒙 )𝒅𝒙 Adding (2) and (3) i.e. (2) + (3) 𝐈𝟏 + 𝐈𝟏 =∫_𝟎^(𝝅/𝟐)β–’γ€–π’π’π’ˆ(π’”π’Šπ’β‘π’™ )𝒅𝒙+∫_𝟎^(𝝅/𝟐)β–’π’π’π’ˆ(πœπ¨π¬β‘π’™ )𝒅𝒙〗 "Using" π’π’π’ˆβ‘π’‚ + π’π’π’ˆβ‘π’ƒ = π’π’π’ˆβ‘(𝒂.𝒃) 2I1 =∫_𝟎^(𝝅/𝟐)β–’γ€–π₯𝐨𝐠⁑[𝐬𝐒𝐧⁑〖𝒙 πœπ¨π¬β‘π’™ γ€— ] 𝒅𝒙〗 2I1 = ∫_𝟎^(𝝅/𝟐)β–’γ€–π’π’π’ˆβ‘[πŸπ’”π’Šπ’β‘γ€–π’™ 𝒄𝒐𝒔⁑𝒙 γ€—/𝟐] 𝒅𝒙〗 "Using " π’π’π’ˆ(𝒂/𝒃) = log⁑(π‘Ž) – log⁑(𝑏)) 2I1 = ∫_0^(πœ‹/2)β–’[log[2sin⁑〖π‘₯ cos⁑π‘₯ γ€— ]βˆ’π‘™π‘œπ‘”(2)]𝑑π‘₯ "Using" π’”π’Šπ’β‘πŸπ’™=2 sin⁑〖π‘₯ cos⁑π‘₯ γ€— 2I1 = ∫_0^(πœ‹/2)β–’[log[sin⁑2π‘₯ ]βˆ’π‘™π‘œπ‘”2]𝑑π‘₯ 2I1 = ∫_𝟎^(𝝅/𝟐)β–’π₯𝐨𝐠[π’”π’Šπ’β‘πŸπ’™ ]π’…π’™βˆ’βˆ«_0^(πœ‹/2)β–’log(2)𝑑π‘₯ Solving 𝐈𝟐 𝐈𝟐=∫_𝟎^(𝝅/𝟐)β–’γ€–π₯𝐨𝐠 π’”π’Šπ’β‘πŸπ’™ 𝒅𝒙〗 Let 2π‘₯=𝑑 Differentiating both sides w.r.t.π‘₯ 2=𝑑𝑑/𝑑π‘₯ 𝑑π‘₯=𝑑𝑑/2 ∴ Putting the values of t and 𝑑𝑑 and changing the limits, I2 =∫_0^(πœ‹/2)β–’log(sin⁑2π‘₯ )𝑑π‘₯ I2 = ∫_0^πœ‹β–’γ€–log(sin⁑𝑑 ) 𝑑𝑑/2γ€— 𝐈𝟐 = 𝟏/𝟐 ∫_𝟎^𝝅▒π₯𝐨𝐠(π’”π’Šπ’β‘π’• )𝒅𝒕 Here, 𝑓(𝑑)=log⁑𝑠𝑖𝑛𝑑 𝑓(2π‘Žβˆ’π‘‘)=𝑓(2πœ‹βˆ’π‘‘)=log⁑𝑠𝑖𝑛(2πœ‹βˆ’π‘‘)=log⁑sin⁑𝑑 As, 𝒇(𝒕)=𝒇(πŸπ’‚βˆ’π’•) ∴ 𝐈𝟐 = 1/2 ∫_0^πœ‹β–’log⁑sin⁑〖𝑑 𝑑𝑑〗 =𝟏/𝟐 Γ— 𝟐∫_𝟎^(𝝅/𝟐)β–’π’π’π’ˆβ‘π’”π’Šπ’β‘γ€–π’•. 𝒅𝒕〗 =∫_0^(πœ‹/2)β–’log⁑sin⁑〖𝑑. 𝑑𝑑〗 =∫_0^(πœ‹/2)β–’log⁑sin⁑〖π‘₯ 𝑑π‘₯γ€— Putting the value of I2 in equation (3), we get 2I1 =∫_𝟎^(𝝅/𝟐)β–’π₯𝐨𝐠[π’”π’Šπ’β‘πŸπ’™ ]⁑𝒅𝒙 βˆ’βˆ«_0^(πœ‹/2)β–’log(2)⁑𝑑π‘₯ 2I1 = ∫_𝟎^(𝝅/𝟐)β–’π₯𝐨𝐠(π’”π’Šπ’β‘π’™ )⁑𝒅𝒙 βˆ’log(2) ∫_𝟎^(𝝅/𝟐)β–’γ€–πŸ.〗⁑𝒅𝒙 2I1 = I1 βˆ’ log(2) [π‘₯]_0^(πœ‹/2) 2I1βˆ’I1=βˆ’log⁑2 [πœ‹/2βˆ’0] 𝐈𝟏=βˆ’π’π’π’ˆβ‘πŸ [𝝅/𝟐] Hence, 𝐈=2 I1= 2 Γ— (βˆ’πœ‹)/2 log⁑2 =βˆ’π… π’π’π’ˆβ‘πŸ

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