Example 42 - Evaluate x dx / a2 cos2 x + b2 sin2 x - Examples - Examples

part 2 - Example 42 - Examples - Serial order wise - Chapter 7 Class 12 Integrals
part 3 - Example 42 - Examples - Serial order wise - Chapter 7 Class 12 Integrals part 4 - Example 42 - Examples - Serial order wise - Chapter 7 Class 12 Integrals part 5 - Example 42 - Examples - Serial order wise - Chapter 7 Class 12 Integrals part 6 - Example 42 - Examples - Serial order wise - Chapter 7 Class 12 Integrals part 7 - Example 42 - Examples - Serial order wise - Chapter 7 Class 12 Integrals

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Example 42 Evaluate โˆซ_0^๐œ‹โ–’(๐‘ฅ ๐‘‘๐‘ฅ)/(๐‘Ž^2 cos^2โกใ€–๐‘ฅ + ๐‘^2 ใ€— sin^2โก๐‘ฅ )Let I= โˆซ_0^๐œ‹โ–’ใ€–๐‘ฅ/(๐‘Ž^2 ๐‘๐‘œ๐‘ ^2 ๐‘ฅ + ๐‘^2 ๐‘ ๐‘–๐‘›^2 ๐‘ฅ) ๐‘‘๐‘ฅใ€— โˆด I=โˆซ_0^๐œ‹โ–’ใ€–((๐œ‹ โˆ’ ๐‘ฅ))/(๐‘Ž^2 ๐‘๐‘œ๐‘ ^2 (๐œ‹ โˆ’ ๐‘ฅ) + ๐‘^2 ๐‘ ๐‘–๐‘›^2 (๐œ‹ โˆ’ ๐‘ฅ) ) ๐‘‘๐‘ฅใ€— I=โˆซ_0^๐œ‹โ–’ใ€–(๐œ‹ โˆ’ ๐‘ฅ)/(๐‘Ž^2 [๐‘๐‘œ๐‘ (๐œ‹ โˆ’ ๐‘ฅ)]^2 + ๐‘^2 [๐‘ ๐‘–๐‘›(๐œ‹ โˆ’ ๐‘ฅ)]^2 ) ๐‘‘๐‘ฅใ€— I=โˆซ_0^๐œ‹โ–’ใ€–(๐œ‹ โˆ’ ๐‘ฅ)/(๐‘Ž^2 [โˆ’ ๐‘๐‘œ๐‘  ๐‘ฅ]^2 + ๐‘^2 [๐‘ ๐‘–๐‘› ๐‘ฅ]^2 ) ๐‘‘๐‘ฅใ€— I=โˆซ_0^๐œ‹โ–’ใ€–(๐œ‹ โˆ’ ๐‘ฅ)/(๐‘Ž^2 cos^2โก๐‘ฅ + ๐‘^2 sin^2โก๐‘ฅ ) ๐‘‘๐‘ฅใ€— Adding (1) and (2) i.e. (1) + (2) I+I=โˆซ_0^๐œ‹โ–’ใ€–๐‘ฅ/(๐‘Ž^2 cos^2โก๐‘ฅ + ๐‘^2 sin^2โก๐‘ฅ ) ๐‘‘๐‘ฅใ€—+โˆซ1โ–’(๐œ‹ โˆ’ ๐‘ฅ)/(๐‘Ž^2 cos^2โก๐‘ฅ + ๐‘^2 sin^2โก๐‘ฅ ) ๐‘‘๐‘ฅ 2I=โˆซ_0^๐œ‹โ–’(๐‘ฅ + ๐œ‹ โˆ’ ๐‘ฅ)/(๐‘Ž^2 cos^2โก๐‘ฅ + ๐‘^2 sin^2โก๐‘ฅ ) ๐‘‘๐‘ฅ 2I=โˆซ_0^๐œ‹โ–’(๐œ‹ )/(๐‘Ž^2 cos^2โก๐‘ฅ + ๐‘^2 sin^2โก๐‘ฅ ) ๐‘‘๐‘ฅ I=๐œ‹/2 โˆซ_0^๐œ‹โ–’ใ€–1/(๐‘Ž^2 cos^2โก๐‘ฅ + ๐‘^2 sin^2โก๐‘ฅ ) ๐‘‘๐‘ฅใ€— Dividing numerator and denominator by ๐‘๐‘œ๐‘ ^2 ๐‘ฅ, we get I=๐œ‹/2 โˆซ_0^๐œ‹โ–’ใ€–(1/cos^2โก๐‘ฅ )/((๐‘Ž^2 cos^2โกใ€–๐‘ฅ + ๐‘^2 sin^2โก๐‘ฅ ใ€—)/cos^2โก๐‘ฅ ) ๐‘‘๐‘ฅใ€— I=๐œ‹/2 โˆซ_0^๐œ‹โ–’ใ€–(๐‘ ๐‘’๐‘^2 ๐‘ฅ)/((๐‘Ž^2 cos^2โก๐‘ฅ)/cos^2โก๐‘ฅ + (๐‘^2 sin^2โก๐‘ฅ)/cos^2โก๐‘ฅ ) ๐‘‘๐‘ฅใ€— I=๐œ‹/2 โˆซ_0^๐œ‹โ–’ใ€–(๐‘ ๐‘’๐‘^2 ๐‘ฅ)/(๐‘Ž^2 + ๐‘^2 tan^2โก๐‘ฅ ) ๐‘‘๐‘ฅใ€— Let ๐‘“(๐‘ฅ)=sec^2โก๐‘ฅ/(๐‘Ž^2 + ๐‘^2 tan^2โก๐‘ฅ ) and a = ฯ€ Now, ๐‘“(2๐‘Žโˆ’๐‘ฅ)=sec^2โก(๐œ‹ โˆ’ ๐‘ฅ)/(๐‘Ž^2 + ๐‘^2 tan^2โก(๐œ‹ โˆ’ ๐‘ฅ) ) ๐‘“(2๐‘Žโˆ’๐‘ฅ)=[โˆ’๐‘ ๐‘’๐‘ ๐‘ฅ]^2/(๐‘Ž^2 + ๐‘^2 [โˆ’tanโก๐‘ฅ ]^2 ) ๐‘“(2๐‘Žโˆ’๐‘ฅ)=(๐‘ ๐‘’๐‘^2 ๐‘ฅ)/(๐‘Ž^2 + ๐‘^2 tan^2โก๐‘ฅ ) Therefore, ๐‘“(๐‘ฅ)=๐‘“(2๐‘Žโˆ’๐‘ฅ) Therefore, I=๐œ‹/2 โˆซ_0^๐œ‹โ–’ใ€–(๐‘ ๐‘’๐‘^2 ๐‘ฅ)/(๐‘Ž^2 + ๐‘^2 tan^2โก๐‘ฅ ) ๐‘‘๐‘ฅใ€— =๐œ‹/2 ร— 2 โˆซ_0^(๐œ‹/2)โ–’ใ€–(๐‘ ๐‘’๐‘^2 ๐‘ฅ)/(๐‘Ž^2 + ๐‘^2 tan^2โก๐‘ฅ ) ๐‘‘๐‘ฅใ€— =๐œ‹โˆซ_0^(๐œ‹/2)โ–’ใ€–(๐‘ ๐‘’๐‘^2 ๐‘ฅ)/(๐‘Ž^2 + ๐‘^2 tan^2โก๐‘ฅ ) ๐‘‘๐‘ฅใ€— Let ๐‘ tanโกใ€–๐‘ฅ=๐‘กใ€— Differentiating both sides w.r.t. ๐‘ฅ ๐‘ ๐‘ ๐‘’๐‘^2 ๐‘ฅ ๐‘‘๐‘ฅ=๐‘‘๐‘ก ๐‘‘๐‘ก=๐‘‘๐‘ก/(๐‘^2 ๐‘ ๐‘’๐‘^2 ๐‘ฅ) Putting the values of tan ๐‘ฅ and ๐‘‘๐‘ฅ , we get ๐ผ=๐œ‹โˆซ1_0^(๐œ‹/2)โ–’ใ€–(๐‘ ๐‘’๐‘^2 ๐‘ฅ)/(๐‘Ž^2 + ๐‘ก^2 ) . ๐‘‘๐‘ฅใ€— ๐ผ=๐œ‹ โˆซ1_0^โˆžโ–’ใ€–(๐‘ ๐‘’๐‘^2 ๐‘ฅ)/(๐‘Ž^2 + ๐‘ก^2 ) .๐‘‘๐‘ก/(๐‘ ๐‘ ๐‘’๐‘^2 ๐‘ฅ)ใ€— ๐ผ=๐œ‹/๐‘ โˆซ1_0^โˆžโ–’๐‘‘๐‘ก/(๐‘Ž^2 + ๐‘ก^2 ) ๐ผ= ใ€–๐œ‹/๐‘ [1/๐‘Ž tan^(โˆ’1)โก(๐‘ก/๐‘Ž) ]ใ€—_0^โˆž Putting limits, I=๐œ‹/๐‘ [1/๐‘Ž ใ€–๐‘ก๐‘Ž๐‘›ใ€—^(โˆ’1) (โˆž/๐‘Ž)โˆ’1/๐‘Ž ใ€–๐‘ก๐‘Ž๐‘›ใ€—^(โˆ’1) (0/๐‘Ž)] I =๐œ‹/๐‘ [ใ€–1/๐‘Ž tan^(โˆ’1)ใ€—โกใ€–(โˆž)โˆ’1/๐‘Ž tan^(โˆ’1)โก(0) ใ€— ] I =๐œ‹/๐‘ (1/๐‘Ž (๐œ‹/2)โˆ’0) I =๐…^๐Ÿ/๐Ÿ๐’‚๐’ƒ

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