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Integrals, Application of Integrals and Differential Equations

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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 ∫
𝑓 ′ (π‘₯)
𝑑π‘₯ = log{𝑓(π‘₯)} + 𝐢
𝑓(π‘₯)
• Integral of the form ∫{𝑓(π‘₯)}𝑛 𝑓′(π‘₯)𝑑π‘₯
𝑓(π‘₯)
• Integral of the form ∫ 𝑓′(π‘₯) 𝑑π‘₯
• Integral of the form∫ π’”π’Šπ’π’Ž 𝒙𝒅𝒙 , ∫ π’„π’π’”π’Ž 𝒙 dx. Where m≤ 4,use the following trigonometrical
identities: (i) 𝑠𝑖𝑛2 π‘₯ =
1−π‘π‘œπ‘  2π‘₯
(ii) π‘π‘œπ‘  2 π‘₯ =
2
3
(iii) 𝑠𝑖𝑛 3π‘₯ = 3𝑠𝑖𝑛 π‘₯ − 4𝑠𝑖𝑛 π‘₯
1+π‘π‘œπ‘  2π‘₯
2
(iv) 𝑠𝑖𝑛 3π‘₯ = 4π‘π‘œπ‘  3 π‘₯ − 3 π‘π‘œπ‘  π‘₯.
• Integral of the form ∫ π’”π’Šπ’ π’Žπ’™ 𝒄𝒐𝒔 𝒏𝒙 𝒅𝒙, ∫ π’”π’Šπ’ π’Žπ’™ π’”π’Šπ’ 𝒏𝒙 𝒅𝒙 , ∫ 𝒄𝒐𝒔 π’Žπ’™ 𝒄𝒐𝒔 𝒏𝒙 𝒅𝒙.
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 ∫ 𝐬𝐒𝐧𝐦 𝐱 𝐜𝐨𝐬𝐧 𝐱 dx, m, n 𝝐 N.
Conditions
Substitutions
i.
If π‘š is an odd (+)ive integer and n is even
π‘π‘œπ‘  π‘₯ = 𝑑
ii.
If 𝑛 is an odd (+)ive integer
𝑠𝑖𝑛 π‘₯ = 𝑑
iii.
If both π‘š, 𝑛 are odd (+) ive integers
either 𝑠𝑖𝑛 π‘₯ = 𝑑 π‘œπ‘Ÿ π‘π‘œπ‘  π‘₯ = 𝑑.
iv.
If both π‘š, 𝑛 are even (+) ive integers
use multiple angle formula
v.
If π‘š + 𝑛 is a negative even integer
π‘‘π‘Žπ‘› π‘₯ = 𝑑
•
∫ 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
𝐝𝐱
𝐝𝐱
𝐝𝐱
𝐝𝐱
𝐝𝐱
∫ 𝐚 𝐬𝐒𝐧𝟐 𝐱 + 𝐛 𝐜𝐨𝐬 𝟐 𝐱 , ∫ 𝐚 + 𝐛 𝐬𝐒𝐧𝟐 𝐱 , ∫ 𝐚 + 𝐛 𝐜𝐨𝐬𝟐 𝐱 , ∫ ( 𝐚 𝐬𝐒𝐧𝐱 + 𝐛 𝐜𝐨𝐬𝐱 )𝟐 , ∫ 𝐚+ 𝐛 𝐬𝐒𝐧𝟐 𝐱 + 𝐜 𝐜𝐨𝐬𝟐 𝐱
(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:
𝐝𝐱
𝐝𝐱
𝐝𝐱
𝐝𝐱
∫ 𝐚 𝐬𝐒𝐧𝐱 + 𝐛 𝐜𝐨𝐬𝐱 , ∫ 𝐚 + 𝐛 𝐬𝐒𝐧𝐱 , ∫ 𝐚 + 𝐛 𝐜𝐨𝐬𝐱 , ∫ 𝐚 + 𝐛 𝐬𝐒𝐧𝐱 + 𝐜 𝐜𝐨𝐬𝐱
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±π›Ό)2 ± 𝛽2 ], and apply the following formulas:
1
1
π‘₯
1
1
π‘Ž+π‘₯
1
1
π‘₯−π‘Ž
∫ π‘Ž2 +π‘₯ 2 𝑑π‘₯ = π‘Ž tan−1 ( π‘Ž ) +c , ∫ π‘Ž2 −π‘₯ 2 𝑑π‘₯ = 2π‘Ž log |π‘Ž−π‘₯| + c , ∫ π‘₯ 2 −π‘Ž2 𝑑π‘₯ = 2π‘Ž log |π‘₯+π‘Ž| +c
1
1
∫ √π‘Ž2+π‘₯ 2 𝑑π‘₯ = log|π‘₯ + √π‘Ž2 + π‘₯ 2 | +c , ∫ √π‘₯ 2−π‘Ž2 𝑑π‘₯ = log|π‘₯ + √π‘₯ 2 − π‘Ž2 | + c ,
1
π‘₯
∫ √π‘Ž2−π‘₯ 2 𝑑π‘₯ = sin−1 ( π‘Ž ) + 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.
𝑑
px + q = A 𝑑π‘₯(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 ,
𝑝π‘₯+π‘ž
2π‘Žπ‘₯+𝑏
1
∫ π‘Žπ‘₯ 2+ 𝑏π‘₯+𝑐 dx= A ∫ π‘Žπ‘₯ 2+ 𝑏π‘₯+𝑐dx + B ∫ π‘Žπ‘₯ 2+ 𝑏π‘₯+𝑐 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 ∫(2π‘Žπ‘₯ + 𝑏) √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œ– 𝑅
(i) Divide the numerator and denominator by x2.
A
𝐴
A
Introduce (1 + x2 ) or (1 − π‘₯ 2 ) or both in the numerator. And the denominator in the form of ( x ± x )2 βˆ“ α2
𝐴
A
𝐴
𝐴
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 + π‘Ž2 dx , ∫ π‘₯ 2 + π‘Ž2 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.
𝐟(𝐱)
• Partial Fraction 𝐠(𝐱) 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
𝑝π‘₯ + π‘ž
(π‘₯−π‘Ž)(π‘₯−𝑏)
1.
𝑝π‘₯ + π‘ž
(π‘₯ − π‘Ž)2
2.
3.
,π‘Ž ≠ 𝑏
𝑝π‘₯ 2 + π‘žπ‘₯ + π‘Ÿ
,π‘Ž ≠ 𝑏 ≠ 𝑐
(π‘₯ − π‘Ž)(π‘₯ − 𝑏)(π‘₯ − 𝑐)
4.
𝑝π‘₯ 2 + π‘žπ‘₯ + π‘Ÿ
(π‘₯ − 𝑏)(π‘₯ − π‘Ž)2
5.
𝑝π‘₯ 2 + π‘žπ‘₯ + π‘Ÿ
(π‘₯ − π‘Ž)(π‘₯ 2 + 𝑏π‘₯ + 𝑐)
Form of the partial fraction
𝐴
(π‘₯−π‘Ž)
+ (π‘₯−𝑏)
𝐴
(π‘₯−π‘Ž)
+ (π‘₯−π‘Ž)2
𝐴
(π‘₯−π‘Ž)
𝐴
(π‘₯−π‘Ž)
𝐡
𝐡
𝐡
𝐢
𝐡
𝐢
+ (π‘₯−𝑏) + (π‘₯−𝑐)
+ (π‘₯−π‘Ž)2 + (π‘₯−𝑏)
𝐴
(π‘₯−π‘Ž)
𝐡π‘₯ + 𝐢
+ π‘₯ 2 +𝑏π‘₯+𝑐
Where π’™πŸ + 𝒃𝒙 + 𝒄 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 (𝑠𝑖𝑛π‘₯ − π‘π‘œπ‘ π‘₯) = 𝑑 so that (π‘π‘œπ‘ π‘₯ + 𝑠𝑖𝑛π‘₯) 𝑑π‘₯ = 𝑑𝑑
And (𝑠𝑖𝑛π‘₯ − π‘π‘œπ‘ π‘₯)2 = 𝑑 2
𝑠𝑖𝑛2 π‘₯ + π‘π‘œπ‘  2 π‘₯ − 2𝑠𝑖𝑛π‘₯ π‘π‘œπ‘ π‘₯ = 𝑑 2 or
2
1 − 𝑠𝑖𝑛2π‘₯ = 𝑑 . Now substitute the values and integrate.
Some Important Indefinite Integration Formulae:
1. ∫ π‘₯ 𝑛 𝑑π‘₯ =
π‘₯ 𝑛+1
𝑛+1
+ C, 𝑛 ≠ −1
2. ∫ 𝑑π‘₯ = π‘₯ + 𝐢
3. ∫ cos π‘₯ 𝑑π‘₯ = sin π‘₯ + 𝐢
4. ∫ sin π‘₯ 𝑑π‘₯ = − cos π‘₯ + 𝐢
5. ∫ 𝑠𝑒𝑐 2 π‘₯ 𝑑π‘₯ = tan π‘₯ + 𝐢
6. ∫ π‘π‘œπ‘ π‘’π‘ 2 π‘₯𝑑π‘₯ = − cot π‘₯ + 𝐢
7. ∫ sec π‘₯ tan π‘₯ 𝑑π‘₯ = sec π‘₯ + 𝐢
8. ∫ cosec π‘₯ cot π‘₯ 𝑑π‘₯ = − cosec π‘₯ + 𝐢
1
9. ∫
𝑑π‘₯ = sin−1 π‘₯+ C
√1− π‘₯ 2
1
10. ∫
𝑑π‘₯ = −cos−1 π‘₯+ C
√1− π‘₯ 2
𝑑π‘₯
11. ∫ 1+π‘₯2 = tan−1 π‘₯ + C
𝑑π‘₯
12. ∫ 1+π‘₯2 = − cot −1 π‘₯ + C
13. ∫ 𝑒 π‘₯ 𝑑π‘₯ = 𝑒 π‘₯ + 𝐢
1
14. ∫ π‘₯ 𝑑π‘₯ = log|π‘₯| + 𝐢
15. ∫ π‘Ž π‘₯ 𝑑π‘₯ =
π‘Žπ‘₯
log π‘Ž
+C
1
16. ∫ 𝑑π‘₯ = log π‘₯ + 𝐢
π‘₯
17. ∫
1
𝑑π‘₯
√π‘₯
= 2√π‘₯ + 𝐢
18. ∫ π‘‘π‘Žπ‘› π‘₯ 𝑑π‘₯ = π‘™π‘œπ‘” |𝑠𝑒𝑐π‘₯| + 𝐢 = − π‘™π‘œπ‘” |π‘π‘œπ‘ π‘₯| + 𝐢
19. ∫ π‘π‘œπ‘‘ π‘₯ 𝑑π‘₯ = π‘™π‘œπ‘” |𝑠𝑖𝑛π‘₯| + 𝐢
20. ∫ 𝑠𝑒𝑐 𝑑π‘₯ = π‘™π‘œπ‘” |𝑠𝑒𝑐 π‘₯ + π‘‘π‘Žπ‘›π‘₯| + 𝐢
21. ∫ π‘π‘œπ‘ π‘’π‘ 𝑑π‘₯ = π‘™π‘œπ‘” |π‘π‘œπ‘ π‘’π‘π‘₯ − π‘π‘œπ‘‘π‘₯| +𝐢
1
1
π‘₯
1
1
π‘Ž+π‘₯
22. ∫ π‘Ž2 +π‘₯ 2 𝑑π‘₯ = π‘Ž tan−1 ( π‘Ž ) +C ,
23. ∫ 2 2 𝑑π‘₯ = log | | + C ,
π‘Ž −π‘₯
2π‘Ž
π‘Ž−π‘₯
1
1
π‘₯−π‘Ž
24. ∫ π‘₯ 2 −π‘Ž2 𝑑π‘₯ = 2π‘Ž log |π‘₯+π‘Ž| +C ,
1
25. ∫ 2 2 𝑑π‘₯ = log|π‘₯ + √π‘Ž2 + π‘₯ 2 | +C ,
√π‘Ž +π‘₯
1
26. ∫ 2 2 𝑑π‘₯ = log|π‘₯ + √π‘₯ 2 − π‘Ž2 | + C ,
√π‘₯ −π‘Ž
1
π‘₯
27. ∫ 2 2 𝑑π‘₯ = sin−1 ( π‘Ž ) + C.
√π‘Ž −π‘₯
π‘₯
π‘Ž2
log|π‘₯
2
+ √π‘₯ 2 − π‘Ž2 | + 𝐢
π‘₯
π‘Ž2
log|π‘₯
2
+ √π‘₯ 2 + π‘Ž2 | + 𝐢
π‘₯
π‘Ž2
π‘₯
sin−1 (π‘Ž) + C
2
28. ∫ √π‘₯ 2 − π‘Ž2 𝑑π‘₯ = 2 √π‘₯ 2 − π‘Ž2 −
29. ∫ √π‘₯ 2 + π‘Ž2 𝑑π‘₯ = 2 √π‘₯ 2 + π‘Ž2 +
30. ∫ √π‘Ž2 − π‘₯ 2 𝑑π‘₯ = 2 √π‘Ž2 − π‘₯ 2 +
Definite integration
𝑏
➒ Fundamental Theorem of Calculus: We have defined ∫π‘Ž 𝑓(π‘₯)𝑑π‘₯ as the area of the region bounded by
the curve 𝑦 = 𝑓(π‘₯), the ordinates π‘₯ = π‘Ž and π‘₯ = 𝑏 and π‘₯-axis. Let π‘₯ be a given point in [π‘Ž, 𝑏]. Then
π‘₯
∫π‘Ž 𝑓(π‘₯)𝑑π‘₯ represents the area of the light shaded region
➒ First fundamental theorem of integral calculus:
Theorem - 1
Let 𝑓 be a continuous function on the closed interval [π‘Ž, 𝑏] and let 𝐴 (π‘₯) be the area
function. Then 𝐴′(π‘₯) = ∫ 𝑓 (π‘₯), for all π‘₯ ∈ [π‘Ž, 𝑏].
➒ Second fundamental theorem of integral calculus:
Theorem - 2
Let f be continuous function defined on the closed interval [π‘Ž, 𝑏] and 𝐹 be an anti
𝑏
derivative of 𝑓. Then ∫π‘Ž 𝑓(π‘₯)𝑑π‘₯dx = [𝐹(π‘₯)]π‘π‘Ž = F (b) – F(a).
PROPERTIES OF DEFINITE INTEGRALS:
Application Of Integrals (Graphs of Some Standard Curves)
Parabolas
Circles
Ellipse
Modulus
Functions
π’š = π’™πŸ‘
Formula Used
π‘₯ 𝑛+1
𝑏
𝑏
➒ ∫π‘Ž π‘₯ 𝑛 𝑑π‘₯ = [
]
𝑛+1
π‘Ž
𝑑
π‘₯
➒ ∫𝑐 √π‘Ž2 − π‘₯ 2 𝑑π‘₯ = [2 √π‘Ž2 − π‘₯ 2 +
π‘Ž2
2
π‘₯
sin−1 (π‘Ž)]
𝑑
𝑐
➒ Equation of Straight Line passing through two points (π‘₯1 , 𝑦1 ) and (π‘₯2 , 𝑦2 )is
𝑦 − 𝑦1 = (
𝑦2 − 𝑦1
) (π‘₯ − π‘₯1 )
π‘₯2 − π‘₯1
➒ Area under Simple Curves
➒ The area of the region bounded by the curve 𝑦 = 𝑓 (π‘₯), π‘₯-axis and the lines π‘₯ = π‘Ž and π‘₯ = 𝑏
(𝑏 > π‘Ž) is given by the formula:
𝒃
𝒃
Area = ∫𝒂 π’šπ’…π’™ = ∫𝒂 𝒇(𝒙)𝒅𝒙
➒ The area of the region bounded by the curve π‘₯ = 𝑔(𝑦), 𝑦-axis and the lines
𝑦 = 𝑐, 𝑦 = 𝑑 is given by the formula:
𝒅
𝒅
Area = ∫𝒄 π’™π’…π’š = ∫𝒄 π’ˆ(π’š)π’…π’š
➒ The area of the region enclosed between two curves 𝑦 = 𝑓 (π‘₯), 𝑦 = 𝑔 (π‘₯) and the
lines π‘₯ = π‘Ž, π‘₯ = 𝑏 is given by the formula.
𝒃
Area = ∫𝒂 (𝒇(𝒙) − π’ˆ(𝒙))𝒅𝒙
KEY POINTS :
𝑑
π‘₯
π‘Ž2
π‘₯
𝑑
•
∫𝑐 √π‘Ž2 − π‘₯ 2 𝑑π‘₯ = [2 √π‘Ž2 − π‘₯ 2 +
•
•
•
•
Curve π‘Žπ‘₯ + 𝑏𝑦 = 𝑐 is a straight line
Curve 𝑦 2 = 4π‘Žπ‘₯ is a parabola with vertex (0,0) and axis is x-axis.
Curve π‘₯ 2 = 4π‘Žπ‘¦ is a parabola with vertex (0,0) and axis is y-axis.
Curve π‘₯ 2 +𝑦 2 = π‘Ž2 is a circle with center (0,0) and radius = π‘Ž
•
Curve π‘Ž2 + 𝑏2 = 1, π‘Ž > 𝑏 and π‘Ž2 + 𝑏2 = 1, π‘Ž > 𝑏 is an ellipse with centre (0,0)
•
π‘₯2
𝑦2
𝑦2
2
sin−1 (π‘Ž)]
𝑐
π‘₯2
Circle and ellipse are symmetric in each quadrant.
DIFFERENTIAL EQUATIONS
𝑑𝑦
➒ For a given function 𝑔, a function 𝑓 such that 𝑑π‘₯ = 𝑔(π‘₯), where 𝑦 = 𝑓(π‘₯)
An equation of this form is known as a differential equation
➒ 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.
➒ Degree of a differential equation: is the degree of the highest order derivative, when differential
coefficients are made free from radicals and fractions
➒ NOTE: If differential equation involves following types of terms, then we say that degree of
differential equation is not defined- 𝐬𝐒𝐧 π’š′ , 𝐜𝐨𝐬 π’š′, 𝑒 𝑦′ , π’π’π’ˆ π’š′ 𝒆𝒕𝒄.
➒ 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.
➒ 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
➒ Methods of Solving First Order, First Degree Differential Equations
➒ 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 𝑑π‘₯ and terms
containing 𝑦 should remain with 𝑑𝑦.
➒ Homogeneous Differential Equation:
A function 𝐹 (π‘₯, 𝑦) is a homogeneous function of degree 𝑛 if 𝐹 (πœ†π‘₯, πœ†π‘¦ ) = πœ†π‘› 𝐹 (π‘₯, 𝑦)
for some non-zero constant πœ†. A differential equation which can be expressed in the form
𝑑𝑦
𝑑π‘₯
= 𝐹 (π‘₯, 𝑦) or 𝑑𝑦 = 𝐺 (π‘₯, 𝑦), where 𝐹 (π‘₯, 𝑦) and 𝐺 (π‘₯, 𝑦) are homogeneous functions of
𝑑π‘₯
degree zero,
➒ Steps to solve a homogeneous differential equation of the type
π’…π’š
π’š
(i) 𝒅𝒙 = 𝑭(𝒙, π’š) = π’ˆ (𝒙)... (1)
(ii) Put π’š = 𝒗 𝒙 ... (2)
π’…π’š
𝒅𝒗
(iii) Differentiating equation (2) with respect to π‘₯, we get 𝒅𝒙 = 𝒗 + 𝒙 𝒅𝒙... (3)
(iv) Put the value of
𝒅𝒗
𝑑𝑦
𝑑π‘₯
from equation (3) in equation (1), we get
𝒅𝒗
𝒗 + 𝒙 𝒅𝒙 = π’ˆ (𝒗) π‘œπ‘Ÿ 𝒙 𝒅𝒙 = π’ˆ (𝒗) – 𝒗 ... (4)
𝑦
Now apply Variable separable method to integrate and replace 𝑣 by π‘₯
•
𝑑π‘₯
If the equation is of the form 𝑑𝑦 = 𝐺 (π‘₯, 𝑦) We make the substitution π‘₯ = 𝑣 𝑦... (2)
𝑑π‘₯
𝑑𝑣
Differentiating equation (2) with respect to 𝑦, we get 𝑑𝑦 = 𝑣 + 𝑦 𝑑𝑦...(3)proceed in the same way.
𝑑𝑦
➒ Linear differential equations: Is of the from 𝑑π‘₯ + 𝑃𝑦 = 𝑄 where, P and Q are constants
or functions of π‘₯ only, is known as a first order linear differential equation.
➒ Steps to solve first order linear differential equation
(i) Express the given differential equation in the form
π’…π’š
𝒅𝒙
(ii) Find the Integrating Factor (I.F) = 𝒆∫ 𝑷𝒅𝒙 .
(iii) Write the solution of the given differential equation as
+ π‘·π’š = 𝑸
y (I.F) = ∫ 𝑸 × π‘°. 𝑭 𝒅𝒙 + π‘ͺ
➒ Note:- Before solving the questions, note the following concepts: (here the base of log is e.)
1
(π‘Ž) 𝑒log π‘₯ = π‘₯
(𝑏) 𝑒− log π‘₯ = 𝑒log π‘₯−1= π‘₯−1 =π‘₯
(c) 𝑒2 log π‘₯ = 𝑒log π‘₯2 = π‘₯2
(𝑑) 𝐼𝑛 π‘”π‘’π‘›π‘’π‘Ÿπ‘Žπ‘™ 𝑒log 𝑓(π‘₯) = 𝑓(π‘₯)
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