Ex 9.3, 11 - Find particular solution: (x3 + x2 + x + 1) dy/dx - Ex 9.3

part 2 - Ex 9.3, 11 - Ex 9.3 - Serial order wise - Chapter 9 Class 12 Differential Equations
part 3 - Ex 9.3, 11 - Ex 9.3 - Serial order wise - Chapter 9 Class 12 Differential Equations part 4 - Ex 9.3, 11 - Ex 9.3 - Serial order wise - Chapter 9 Class 12 Differential Equations part 5 - Ex 9.3, 11 - Ex 9.3 - Serial order wise - Chapter 9 Class 12 Differential Equations part 6 - Ex 9.3, 11 - Ex 9.3 - Serial order wise - Chapter 9 Class 12 Differential Equations part 7 - Ex 9.3, 11 - Ex 9.3 - Serial order wise - Chapter 9 Class 12 Differential Equations

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Ex 9.3, 11 Find a particular solution satisfying the given condition : (π‘₯^3+π‘₯^2+π‘₯+1) 𝑑𝑦/𝑑π‘₯=2π‘₯^2+π‘₯; 𝑦=1 when π‘₯=0(π‘₯^3+π‘₯^2+π‘₯+1) 𝑑𝑦/𝑑π‘₯=2π‘₯^2+π‘₯ π’…π’š = (πŸπ’™^𝟐 + 𝒙)/(𝒙^πŸ‘ + 𝒙^𝟐 + 𝒙 + 𝟏) 𝒅𝒙 Integrating both sides ∫1▒〖𝑑𝑦=∫1β–’(2π‘₯^2 + π‘₯)/(π‘₯3 + π‘₯2 + π‘₯ + 1)γ€— dx y = ∫1β–’(πŸπ’™^𝟐 + 𝒙)/( (𝒙 + 𝟏)(𝒙^𝟐 + 𝟏)) dx Rough x = βˆ’1 is a solution of x3 + x2 + x + 1 as (-1)2 + (-1)2 + (βˆ’1) + 1 = 0 Hence (x + 1) is one of its factors. So, we can write x3 + x2 + x + 1 = (x + 1) (x2 + 1) Integrating by partial fractions, using formula (πŸπ’™^𝟐 +𝒙)/((𝒙 + 𝟏)(𝒙^𝟐+𝟏)) = 𝑨/(𝒙 + 𝟏)+(𝑩𝒙 + π‘ͺ)/(𝒙^𝟐 + 𝟏) (2π‘₯^2 +π‘₯)/((π‘₯ + 1)(π‘₯^2+1)) = (𝐴(π‘₯^2+1) + (𝐡π‘₯ + 𝑐)(π‘₯ + 1))/((π‘₯ + 1)(π‘₯^2 + 1)) 2π‘₯^2 + x = A (π‘₯^2+ 1) + (Bx + C) (x + 1) Putting x = βˆ’1 2(βˆ’1)2 βˆ’ 1 = A ((βˆ’1)2 + 1) + (B(βˆ’1) + C)(βˆ’1 + 1) 2 βˆ’ 1 = A(2) + (–B + C)(0) 1 = 2A A = 𝟏/𝟐 Putting x = 0 0 = A (0 + 1) + (B(0) + C)(0 + 1) 0 = A + C(1) A = βˆ’C Since A = 𝟏/𝟐 ∴ C = (βˆ’πŸ)/𝟐 Putting x = 1 2(1) + 1 = A (12 + 1) + (B(1) + C) (1 + 1) 3 = 2A + 2B + 2C Putting A = 𝟏/𝟐, C = (βˆ’πŸ)/𝟐 3 = 2 Γ— 1/2 + 2B + 2 (βˆ’1/2 ) 3 = 2B B = πŸ‘/𝟐 Hence, (πŸπ’™^𝟐 + 𝒙)/((𝒙 + 𝟏)(𝒙^𝟐+𝟏)) = 1/(2(π‘₯ + 1)) + (3/2 π‘₯ βˆ’ 1/2)/(π‘₯^2 + 1) = 𝟏/(𝟐(𝒙 + 𝟏)) + (πŸ‘π’™ βˆ’πŸ)/(γ€–πŸ(𝒙〗^(𝟐 )+ 𝟏)) Now, our equation becomes y = ∫1β–’γ€–(2π‘₯^2 + π‘₯)/((π‘₯ + 1)(π‘₯^2 + 1)) 𝑑π‘₯γ€— y = ∫1β–’γ€–πŸ/(𝟐(𝒙 + 𝟏))+πŸ‘π’™/(𝟐(𝒙^(𝟐 )+𝟏)) βˆ’ 𝟏/𝟐(𝒙^𝟐 + 𝟏) 𝒅𝒙〗 y = ∫1β–’γ€–1/(2(π‘₯ + 1)) 𝑑π‘₯γ€—+∫1β–’γ€–3π‘₯/(2(π‘₯^(2 )+1)) 𝑑π‘₯γ€—βˆ’βˆ«1β–’γ€– 1/2(π‘₯^2 + 1) 𝑑π‘₯γ€— y = 𝟏/𝟐 log (x + 1) +∫1β–’γ€–πŸ‘π’™/(𝟐(𝒙^(𝟐 )+𝟏)) π’…π’™γ€—βˆ’ 𝟏/𝟐 tanβˆ’1 x Integrating ∫1β–’γ€–πŸ‘π’™/(𝟐(𝒙^𝟐 + 𝟏)) 𝒅𝒙〗 Put t = x2 + 1 dt = 2x dx ∴ dx = 𝑑𝑑/2π‘₯ So, ∫1β–’γ€–πŸ‘π’™/(𝟐(𝒙^𝟐 + 𝟏)) 𝒅𝒙〗 = 3/2 ∫1β–’π‘₯/𝑑×𝑑𝑑/2π‘₯ = 3/4 ∫1▒𝑑𝑑/𝑑 = πŸ‘/πŸ’ log |𝒕|+𝒄 Putting back value of t ∫1β–’γ€–3π‘₯/(2(π‘₯^2+1)) 𝑑π‘₯γ€— = 3/4 log (x2 + 1) + C Now, From (1) y = 1/2 log (x + 1) +∫1β–’γ€–3π‘₯/(2(π‘₯^(2 )+1)) 𝑑π‘₯γ€—βˆ’ 1/2 tanβˆ’1 x y = 1/2 log (x + 1) +3/4 " log (x2 + 1)"βˆ’ 1/2 tanβˆ’1 x + C Putting x = 0 and y = 1 1 = 1/2 log (0 + 1) + 3/4 log (0 + 1) βˆ’ 1/2 tanβˆ’1 0 + C 1 = 1/2 log (1) + 3/4 log (1) βˆ’ 1/2 tanβˆ’1 0 + C 1 = 0 + 0 βˆ’ 0 + C 1 = C Putting value of C in (1) y = 𝟏/𝟐 log (x + 1) + πŸ‘/πŸ’ log (x2 + 1) βˆ’ 𝟏/𝟐 tanβˆ’1 x + 1 y = 𝟐/4 log (x + 1) + 3/4 log (x2 + 1) βˆ’ 1/2 tanβˆ’1 x + 1 y = 1/4 log (x + 1)2 + 1/4 log (x2 + 1)3 βˆ’ 1/2 tanβˆ’1 x + 1 y = 1/4 [log⁑〖 (π‘₯+1)^2 γ€—+log⁑〖(π‘₯^2+1)^3 γ€— ] "βˆ’ " 1/2 " tanβˆ’1 x + 1 " As log π‘Ž + log b = log π‘Žb y = 𝟏/πŸ’ π’π’π’ˆβ‘γ€–γ€– [(𝒙+𝟏)γ€—^𝟐 (𝒙^𝟐+𝟏)^πŸ‘] γ€— "βˆ’ " 𝟏/𝟐 " tanβˆ’1 x + 1 "

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