AMITY INTERNATIONAL SCHOOL Power Grid Complex Sec - 43, Gurgaon Class: XII Session: 2021-22 Integrals, Application of Integrals and Differential Equations Indefinite Integrations Different forms of integrations: Concepts and Formulae Integration by simple rearrangements. Use simple trigonometric and algebraic formulas or simple rearrangements to solve it for example: (i) ∫ tan π₯ tan 2π₯ tan 3π₯ dx. • Integration by simple substitutions. • Integral of the form ∫ π ′ (π₯) ππ₯ = log{π(π₯)} + πΆ π(π₯) • Integral of the form ∫{π(π₯)}π π′(π₯)ππ₯ π(π₯) • Integral of the form ∫ π′(π₯) ππ₯ • Integral of the form∫ ππππ ππ π , ∫ ππππ π dx. Where m≤ 4,use the following trigonometrical identities: (i) π ππ2 π₯ = 1−πππ 2π₯ (ii) πππ 2 π₯ = 2 3 (iii) π ππ 3π₯ = 3π ππ π₯ − 4π ππ π₯ 1+πππ 2π₯ 2 (iv) π ππ 3π₯ = 4πππ 3 π₯ − 3 πππ π₯. • Integral of the form ∫ πππ ππ πππ ππ π π, ∫ πππ ππ πππ ππ π π , ∫ πππ ππ πππ ππ π π. To evaluate this type of integrals we use the following trigonometrical identities: 2sin A cos B = sin(A + B) + sin(A − B) ; 2cos A sin B = sin(A + B) − sin(A − B) 2cos A cos B = cos(A + B) + cos(A − B) ; 2sin A sin B = cos(A − B) − cos(A + B) • Integral of the form ∫ π¬π’π§π¦ π± ππ¨π¬π§ π± dx, m, n π N. Conditions Substitutions i. If π is an odd (+)ive integer and n is even πππ π₯ = π‘ ii. If π is an odd (+)ive integer π ππ π₯ = π‘ iii. If both π, π are odd (+) ive integers either π ππ π₯ = π‘ ππ πππ π₯ = π‘. iv. If both π, π are even (+) ive integers use multiple angle formula v. If π + π is a negative even integer π‘ππ π₯ = π‘ • ∫ sinn x dx, where n is (+)ive odd integer, put cos x = t • ∫ cosn x dx, where n is (+)ive odd integer, put sin x = t • ∫ sec n x dx, where n is (+)ive even integer, put tan x = t • Integral of the forms ππ± ππ± ππ± ππ± ππ± ∫ π π¬π’π§π π± + π ππ¨π¬ π π± , ∫ π + π π¬π’π§π π± , ∫ π + π ππ¨π¬π π± , ∫ ( π π¬π’π§π± + π ππ¨π¬π± )π , ∫ π+ π π¬π’π§π π± + π ππ¨π¬π π± (i) Divide the numerator and denominator both by cos 2 x.. (ii) Replace sec2x, if any, in denominator by 1 + tan2 x. (iii) Put tan x = t so that sec 2 x dx = dt. dt This substitution reduces the integral in the form ∫ at2+bt+c. Now evaluate the integral obtained. • Integral of the forms: ππ± ππ± ππ± ππ± ∫ π π¬π’π§π± + π ππ¨π¬π± , ∫ π + π π¬π’π§π± , ∫ π + π ππ¨π¬π± , ∫ π + π π¬π’π§π± + π ππ¨π¬π± 1−tan2 x⁄2 (i) Put cos x = and sin x = 1+tan2 x⁄2 2 tanx⁄2 1+tan2 x⁄2 (ii) Replace (1+tan2 x⁄2) in the numerator by sec 2 x⁄2 x (iii) Put tan 2 = t so that 1 2 sec 2 x⁄2 dx = dt. , by this substitution the integral reduces in dt the form ∫ at2+bt+c. Now evaluate the integral obtained. • Integral of the forms: dx dx dx dx ∫ ax2+ bx + c ,∫ √ax2+ bx + c , ∫ c + bx − ax2 , ∫ √c + bx−ax2 Make the coefficient of x2 unity, if it is not, then make the denominator as a perfect square and reduce it in the form [ (x±πΌ)2 ± π½2 ], and apply the following formulas: 1 1 π₯ 1 1 π+π₯ 1 1 π₯−π ∫ π2 +π₯ 2 ππ₯ = π tan−1 ( π ) +c , ∫ π2 −π₯ 2 ππ₯ = 2π log |π−π₯| + c , ∫ π₯ 2 −π2 ππ₯ = 2π log |π₯+π| +c 1 1 ∫ √π2+π₯ 2 ππ₯ = log|π₯ + √π2 + π₯ 2 | +c , ∫ √π₯ 2−π2 ππ₯ = log|π₯ + √π₯ 2 − π2 | + c , 1 π₯ ∫ √π2−π₯ 2 ππ₯ = sin−1 ( π ) + c • Integral of the forms: ∫(px + q)√ax 2 + bx + c dx, ∫ (i) Write (px + q) as: px+q ax2 + bx + c dx, ∫ px+q √ax2 + bx +c dx. π px + q = A ππ₯(ax2+bx+c) +B = A (2ax + b) + B. (ii) Obtain the values of A and B by equating the coefficients of x and constant terms. (iii) Replace ( px + q ) by A (2ax + b) + B in the given integrals to get , ππ₯+π 2ππ₯+π 1 ∫ ππ₯ 2+ ππ₯+π dx= A ∫ ππ₯ 2+ ππ₯+πdx + B ∫ ππ₯ 2+ ππ₯+π dx. px+q 2ax+b and 1 ∫ √ax2 + bx +cdx = A ∫ √ax2 + bx +c dx + B ∫ √ax2 + bx +c dx. • ∫(px + q)√ax 2 + bx + c dx = A ∫(2ππ₯ + π) √ax 2 + bx + c dx + B ∫ √ax 2 + bx + c dx . Now integrate Integral of the forms: x2 +A x2 −A 1 ∫ x4+ kx2 + A2 dx, ∫ x4 + kx2 + A2 dx, ∫ x4 +kx2+1 dx, ∫ √tan x dx, ∫ √cot π₯ dx. A >0, k π π (i) Divide the numerator and denominator by x2. A π΄ A Introduce (1 + x2 ) or (1 − π₯ 2 ) or both in the numerator. And the denominator in the form of ( x ± x )2 β α2 π΄ A π΄ π΄ Substitute (x + π₯ ) = t when numerator is (1− x2 ). Substitute (x − π₯ ) = t when numerator is (1+ π₯ 2 ). The integral reduces in one of the following forms 1 1 ∫ π₯ 2 + π2 dx , ∫ π₯ 2 + π2 dx. Now integrate. • Integrating by parts Integral of the product of two functions = First function x Integral of second – Integral of (derivative of first x integral of second). du ∫ uv dx = u ∫ v dx – ∫( dx ∫ v dx ) dx . If two functions are of different types, take the first function to be the function which comes first in the word ‘ILATE ′ where i. ii. iii. iv. v. I L A T E for inverse trigonometric function. for the logarithmic function. for algebraic function. for trigonometric function. for exponential function. π(π±) • Partial Fraction π (π±) form: If degree of f(x) < degree of g(x) then it is a proper fraction. If degree of f(x) ≥ degree of g(x) then it is an improper fraction, divide the numerator by denominator and then simplify and integrate. S. No. Form of the rational function ππ₯ + π (π₯−π)(π₯−π) 1. ππ₯ + π (π₯ − π)2 2. 3. ,π ≠ π ππ₯ 2 + ππ₯ + π ,π ≠ π ≠ π (π₯ − π)(π₯ − π)(π₯ − π) 4. ππ₯ 2 + ππ₯ + π (π₯ − π)(π₯ − π)2 5. ππ₯ 2 + ππ₯ + π (π₯ − π)(π₯ 2 + ππ₯ + π) Form of the partial fraction π΄ (π₯−π) + (π₯−π) π΄ (π₯−π) + (π₯−π)2 π΄ (π₯−π) π΄ (π₯−π) π΅ π΅ π΅ πΆ π΅ πΆ + (π₯−π) + (π₯−π) + (π₯−π)2 + (π₯−π) π΄ (π₯−π) π΅π₯ + πΆ + π₯ 2 +ππ₯+π Where ππ + ππ + π cannot be factorized further • Some Special Integrals ∫ sin π₯+cos π₯ √sin 2π₯ dx , ∫ sin π₯− cos π₯ √sin 2π₯ dx Put the additive inverse of the numerator as t, and simplify the denominator by making the square of the substitution. As in the 1st example, put (π πππ₯ − πππ π₯) = π‘ so that (πππ π₯ + π πππ₯) ππ₯ = ππ‘ And (π πππ₯ − πππ π₯)2 = π‘ 2 π ππ2 π₯ + πππ 2 π₯ − 2π πππ₯ πππ π₯ = π‘ 2 or 2 1 − π ππ2π₯ = π‘ . Now substitute the values and integrate. Some Important Indefinite Integration Formulae: 1. ∫ π₯ π ππ₯ = π₯ π+1 π+1 + C, π ≠ −1 2. ∫ ππ₯ = π₯ + πΆ 3. ∫ cos π₯ ππ₯ = sin π₯ + πΆ 4. ∫ sin π₯ ππ₯ = − cos π₯ + πΆ 5. ∫ π ππ 2 π₯ ππ₯ = tan π₯ + πΆ 6. ∫ πππ ππ 2 π₯ππ₯ = − cot π₯ + πΆ 7. ∫ sec π₯ tan π₯ ππ₯ = sec π₯ + πΆ 8. ∫ cosec π₯ cot π₯ ππ₯ = − cosec π₯ + πΆ 1 9. ∫ ππ₯ = sin−1 π₯+ C √1− π₯ 2 1 10. ∫ ππ₯ = −cos−1 π₯+ C √1− π₯ 2 ππ₯ 11. ∫ 1+π₯2 = tan−1 π₯ + C ππ₯ 12. ∫ 1+π₯2 = − cot −1 π₯ + C 13. ∫ π π₯ ππ₯ = π π₯ + πΆ 1 14. ∫ π₯ ππ₯ = log|π₯| + πΆ 15. ∫ π π₯ ππ₯ = ππ₯ log π +C 1 16. ∫ ππ₯ = log π₯ + πΆ π₯ 17. ∫ 1 ππ₯ √π₯ = 2√π₯ + πΆ 18. ∫ π‘ππ π₯ ππ₯ = πππ |π πππ₯| + πΆ = − πππ |πππ π₯| + πΆ 19. ∫ πππ‘ π₯ ππ₯ = πππ |π πππ₯| + πΆ 20. ∫ π ππ ππ₯ = πππ |π ππ π₯ + π‘πππ₯| + πΆ 21. ∫ πππ ππ ππ₯ = πππ |πππ πππ₯ − πππ‘π₯| +πΆ 1 1 π₯ 1 1 π+π₯ 22. ∫ π2 +π₯ 2 ππ₯ = π tan−1 ( π ) +C , 23. ∫ 2 2 ππ₯ = log | | + C , π −π₯ 2π π−π₯ 1 1 π₯−π 24. ∫ π₯ 2 −π2 ππ₯ = 2π log |π₯+π| +C , 1 25. ∫ 2 2 ππ₯ = log|π₯ + √π2 + π₯ 2 | +C , √π +π₯ 1 26. ∫ 2 2 ππ₯ = log|π₯ + √π₯ 2 − π2 | + C , √π₯ −π 1 π₯ 27. ∫ 2 2 ππ₯ = sin−1 ( π ) + C. √π −π₯ π₯ π2 log|π₯ 2 + √π₯ 2 − π2 | + πΆ π₯ π2 log|π₯ 2 + √π₯ 2 + π2 | + πΆ π₯ π2 π₯ sin−1 (π) + C 2 28. ∫ √π₯ 2 − π2 ππ₯ = 2 √π₯ 2 − π2 − 29. ∫ √π₯ 2 + π2 ππ₯ = 2 √π₯ 2 + π2 + 30. ∫ √π2 − π₯ 2 ππ₯ = 2 √π2 − π₯ 2 + Definite integration π β’ Fundamental Theorem of Calculus: We have defined ∫π π(π₯)ππ₯ as the area of the region bounded by the curve π¦ = π(π₯), the ordinates π₯ = π and π₯ = π and π₯-axis. Let π₯ be a given point in [π, π]. Then π₯ ∫π π(π₯)ππ₯ represents the area of the light shaded region β’ First fundamental theorem of integral calculus: Theorem - 1 Let π be a continuous function on the closed interval [π, π] and let π΄ (π₯) be the area function. Then π΄′(π₯) = ∫ π (π₯), for all π₯ ∈ [π, π]. β’ Second fundamental theorem of integral calculus: Theorem - 2 Let f be continuous function defined on the closed interval [π, π] and πΉ be an anti π derivative of π. Then ∫π π(π₯)ππ₯dx = [πΉ(π₯)]ππ = F (b) – F(a). PROPERTIES OF DEFINITE INTEGRALS: Application Of Integrals (Graphs of Some Standard Curves) Parabolas Circles Ellipse Modulus Functions π = ππ Formula Used π₯ π+1 π π β’ ∫π π₯ π ππ₯ = [ ] π+1 π π π₯ β’ ∫π √π2 − π₯ 2 ππ₯ = [2 √π2 − π₯ 2 + π2 2 π₯ sin−1 (π)] π π β’ Equation of Straight Line passing through two points (π₯1 , π¦1 ) and (π₯2 , π¦2 )is π¦ − π¦1 = ( π¦2 − π¦1 ) (π₯ − π₯1 ) π₯2 − π₯1 β’ Area under Simple Curves β’ The area of the region bounded by the curve π¦ = π (π₯), π₯-axis and the lines π₯ = π and π₯ = π (π > π) is given by the formula: π π Area = ∫π ππ π = ∫π π(π)π π β’ The area of the region bounded by the curve π₯ = π(π¦), π¦-axis and the lines π¦ = π, π¦ = π is given by the formula: π π Area = ∫π ππ π = ∫π π(π)π π β’ The area of the region enclosed between two curves π¦ = π (π₯), π¦ = π (π₯) and the lines π₯ = π, π₯ = π is given by the formula. π Area = ∫π (π(π) − π(π))π π KEY POINTS : π π₯ π2 π₯ π • ∫π √π2 − π₯ 2 ππ₯ = [2 √π2 − π₯ 2 + • • • • Curve ππ₯ + ππ¦ = π is a straight line Curve π¦ 2 = 4ππ₯ is a parabola with vertex (0,0) and axis is x-axis. Curve π₯ 2 = 4ππ¦ is a parabola with vertex (0,0) and axis is y-axis. Curve π₯ 2 +π¦ 2 = π2 is a circle with center (0,0) and radius = π • Curve π2 + π2 = 1, π > π and π2 + π2 = 1, π > π is an ellipse with centre (0,0) • π₯2 π¦2 π¦2 2 sin−1 (π)] π π₯2 Circle and ellipse are symmetric in each quadrant. DIFFERENTIAL EQUATIONS ππ¦ β’ For a given function π, a function π such that ππ₯ = π(π₯), where π¦ = π(π₯) An equation of this form is known as a differential equation β’ Order of a differential equation: is defined as the order of the highest order derivative of the dependent variable with respect to the independent variable involved in the given differential equation. β’ Degree of a differential equation: is the degree of the highest order derivative, when differential coefficients are made free from radicals and fractions β’ NOTE: If differential equation involves following types of terms, then we say that degree of differential equation is not defined- π¬π’π§ π′ , ππ¨π¬ π′, π π¦′ , πππ π′ πππ. β’ Solution of Differential Equations• The solution which contains arbitrary constants is called the general solution (primitive) of the differential equation. • The solution free from arbitrary constants i.e., the solution obtained from the general solution by giving particular values to the arbitrary constants is called a particular solution of the differential equation. β’ NOTE: The order of a differential equation representing a family of curves is same as the number of arbitrary constants present in the equation corresponding to the family of curves β’ Methods of Solving First Order, First Degree Differential Equations β’ Equations in variable separable form: Variable separable method’ is used to solve such equation in which variables can be separated completely, i.e. terms containing π₯ should remain with ππ₯ and terms containing π¦ should remain with ππ¦. β’ Homogeneous Differential Equation: A function πΉ (π₯, π¦) is a homogeneous function of degree π if πΉ (ππ₯, ππ¦ ) = ππ πΉ (π₯, π¦) for some non-zero constant π. A differential equation which can be expressed in the form ππ¦ ππ₯ = πΉ (π₯, π¦) or ππ¦ = πΊ (π₯, π¦), where πΉ (π₯, π¦) and πΊ (π₯, π¦) are homogeneous functions of ππ₯ degree zero, β’ Steps to solve a homogeneous differential equation of the type π π π (i) π π = π(π, π) = π (π)... (1) (ii) Put π = π π ... (2) π π π π (iii) Differentiating equation (2) with respect to π₯, we get π π = π + π π π... (3) (iv) Put the value of π π ππ¦ ππ₯ from equation (3) in equation (1), we get π π π + π π π = π (π) ππ π π π = π (π) – π ... (4) π¦ Now apply Variable separable method to integrate and replace π£ by π₯ • ππ₯ If the equation is of the form ππ¦ = πΊ (π₯, π¦) We make the substitution π₯ = π£ π¦... (2) ππ₯ ππ£ Differentiating equation (2) with respect to π¦, we get ππ¦ = π£ + π¦ ππ¦...(3)proceed in the same way. ππ¦ β’ Linear differential equations: Is of the from ππ₯ + ππ¦ = π where, P and Q are constants or functions of π₯ only, is known as a first order linear differential equation. β’ Steps to solve first order linear differential equation (i) Express the given differential equation in the form π π π π (ii) Find the Integrating Factor (I.F) = π∫ π·π π . (iii) Write the solution of the given differential equation as + π·π = πΈ y (I.F) = ∫ πΈ × π°. π π π + πͺ β’ Note:- Before solving the questions, note the following concepts: (here the base of log is e.) 1 (π) πlog π₯ = π₯ (π) π− log π₯ = πlog π₯−1= π₯−1 =π₯ (c) π2 log π₯ = πlog π₯2 = π₯2 (π) πΌπ πππππππ πlog π(π₯) = π(π₯)