differential equations exact...
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![Page 1: Differential Equations EXACT EQUATIONSsalfordphysics.com/.../Exact-differential-equations.pdfEquation is exact if ∂P ∂y = ∂Q ∂x Check: ∂P ∂y = − 1 x2 = ∂Q ∂x ∴](https://reader036.vdocuments.us/reader036/viewer/2022071212/612fd7831ecc51586943b5f3/html5/thumbnails/1.jpg)
Differential Equations
EXACT EQUATIONS
Graham S McDonald
A Tutorial Module for learning the techniqueof solving exact differential equations
● Table of contents● Begin Tutorial
c© 2004 [email protected]
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Table of contents
1. Theory
2. Exercises
3. Answers
4. Standard integrals
5. Tips on using solutions
Full worked solutions
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Section 1: Theory 3
1. Theory
We consider here the following standard form of ordinary differentialequation (o.d.e.):
P (x, y)dx + Q(x, y)dy = 0
If ∂P∂y = ∂Q
∂x then the o.de. is said to be exact.
This means that a function u(x, y) exists such that:
du =∂u
∂xdx +
∂u
∂ydy
= P dx + Qdy = 0 .
One solves ∂u∂x = P and ∂u
∂y = Q to find u(x, y).
Then du = 0 gives u(x, y) = C, where C is a constant.This last equation gives the general solution of P dx + Qdy = 0.
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Section 2: Exercises 4
2. Exercises
Click on Exercise links for full worked solutions (there are 11exercises in total)
Show that each of the following differential equations is exact anduse that property to find the general solution:
Exercise 1.
1x
dy − y
x2dx = 0
Exercise 2.
2xydy
dx+ y2 − 2x = 0
Exercise 3.
2(y + 1)exdx + 2(ex − 2y)dy = 0
● Theory ● Answers ● Integrals ● Tips
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Section 2: Exercises 5
Exercise 4.
(2xy + 6x)dx + (x2 + 4y3)dy = 0
Exercise 5.
(8y − x2y)dy
dx+ x− xy2 = 0
Exercise 6.
(e4x + 2xy2)dx + (cos y + 2x2y)dy = 0
Exercise 7.
(3x2 + y cos x)dx + (sinx− 4y3)dy = 0
● Theory ● Answers ● Integrals ● Tips
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Section 2: Exercises 6
Exercise 8.
x tan−1 y · dx +x2
2(1 + y2)· dy = 0
Exercise 9.
(2x + x2y3)dx + (x3y2 + 4y3)dy = 0
Exercise 10.
(2x3 − 3x2y + y3)dy
dx= 2x3 − 6x2y + 3xy2
Exercise 11.
(y2 cos x− sinx)dx + (2y sinx + 2)dy = 0
● Theory ● Answers ● Integrals ● Tips
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Section 3: Answers 7
3. Answers
1. y = Ax ,
2. y2x− x2 = A ,
3. (y + 1)ex − y2 = A ,
4. x2y + 3x2 + y4 = A ,
5. 12x2(1− y2) + 4y2 = A ,
6. 14e4x + x2y2 + sin y = A ,
7. x3 + y sinx− y4 = A ,
8. x2
2 tan−1 y = A ,
9. x2 + x3y3
3 + y4 = A ,
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Section 3: Answers 8
10. x4
2 − 2x3y + 32 x2y2 − y4
4 = A ,
11. y2 sinx + cos x + 2y = A.
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Section 4: Standard integrals 9
4. Standard integrals
f (x)∫
f(x)dx f (x)∫
f(x)dx
xn xn+1
n+1 (n 6= −1) [g (x)]n g′ (x) [g(x)]n+1
n+1 (n 6= −1)1x ln |x| g′(x)
g(x) ln |g (x)|ex ex ax ax
ln a (a > 0)sinx − cos x sinhx coshxcos x sinx coshx sinhxtanx − ln |cos x| tanh x ln coshxcosec x ln
∣∣tan x2
∣∣ cosechx ln∣∣tanh x
2
∣∣sec x ln |sec x + tanx| sech x 2 tan−1 ex
sec2 x tanx sech2 x tanh xcot x ln |sinx| cothx ln |sinhx|sin2 x x
2 −sin 2x
4 sinh2 x sinh 2x4 − x
2
cos2 x x2 + sin 2x
4 cosh2 x sinh 2x4 + x
2
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Section 4: Standard integrals 10
f (x)∫
f (x) dx f (x)∫
f (x) dx
1a2+x2
1a tan−1 x
a1
a2−x212a ln
∣∣∣a+xa−x
∣∣∣ (0< |x|<a)
(a > 0) 1x2−a2
12a ln
∣∣∣x−ax+a
∣∣∣ (|x| > a>0)
1√a2−x2 sin−1 x
a1√
a2+x2 ln∣∣∣x+
√a2+x2
a
∣∣∣ (a > 0)
(−a < x < a) 1√x2−a2 ln
∣∣∣x+√
x2−a2
a
∣∣∣ (x>a>0)
√a2 − x2 a2
2
[sin−1
(xa
) √a2+x2 a2
2
[sinh−1
(xa
)+ x
√a2+x2
a2
]+x
√a2−x2
a2
] √x2−a2 a2
2
[− cosh−1
(xa
)+ x
√x2−a2
a2
]
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Section 5: Tips on using solutions 11
5. Tips on using solutions
● When looking at the THEORY, ANSWERS, INTEGRALS orTIPS pages, use the Back button (at the bottom of the page) toreturn to the exercises.
● Use the solutions intelligently. For example, they can help you getstarted on an exercise, or they can allow you to check whether yourintermediate results are correct.
● Try to make less use of the full solutions as you work your waythrough the Tutorial.
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Solutions to exercises 12
Full worked solutions
Exercise 1.Standard form: P (x, y)dx + Q(x, y)dy = 0
i.e. P (x, y) = − yx2 and Q(x, y) = 1
x
Equation is exact if ∂P∂y = ∂Q
∂x
Check: ∂P∂y = − 1
x2 = ∂Q∂x ∴ o.d.e. is exact.
Since equation exact, u(x, y) exists such that
du =∂u
∂xdx +
∂u
∂ydy
= P dx + Qdy = 0
and equation has solution u = C, C = constant.
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Solutions to exercises 13
∂u∂x = P gives i) ∂u
∂x = − yx2
∂u∂y = Q gives ii) ∂u
∂y = 1x
Integrate i) partially with respect to x,
u =y
x+ φ(y),
where φ(y) is an arbitrary function of y.
Differentiate with respect to y,
∂u
∂y=
1x
+∂φ
∂y=
1x
+dφ
dy
(since φ = φ(y) only)
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Solutions to exercises 14
Compare with equation ii)
1x
+dφ
dy=
1x
i.e.dφ
dy= 0
i.e. φ = C ′, C ′ = constant
and u =y
x+ C ′.
du = 0 implies u = C, C = constant
∴ yx = A , A = C − C ′
= constant.Return to Exercise 1
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Solutions to exercises 15
Exercise 2.
Standard form: (y2 − 2x)dx + 2xy dy = 0
Exact if ∂P∂y = ∂Q
∂x , where P (x, y) = y2 − 2x
Q(x, y) = 2xy
∂P∂y = 2y = ∂Q
∂x i.e. o.d.e. is exact.
∴ u(x, y) exists such that du = ∂u∂xdx + ∂u
∂y dy
= P dx + Qdy = 0,
giving i) ∂u∂x = y2 − 2x , ii) ∂u
∂y = 2xy.
Integrate i): u = xy2 − x2 + φ(y) , φ is arbitrary function.
Differentiate and compare with ii):
∂u∂y = 2xy + dφ
dy = 2xy
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Solutions to exercises 16
∴ dφdy = 0 and φ = C ′ (constant)
∴ u = xy2 − x2 + C ′
du = 0 implies u = C, ∴ xy2−x2 = A , where A = C −C ′.
Return to Exercise 2
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Solutions to exercises 17
Exercise 3.
P (x, y) dx + Q(x, y) dy = 0 where P (x, y) = 2(y + 1)ex
Q(x, y) = 2(ex − 2y)
∂P∂y = 2ex = ∂Q
∂x , ∴ o.d.e. is exact.
∴ u(x, y) exists such that du = ∂u∂xdx + ∂u
∂y dy
= P dx + Qdy = 0,
Giving i) ∂u∂x = 2(y + 1)ex , ii) ∂u
∂y = 2(ex − 2y) .
Integrate i): u = 2(y + 1)ex + φ(y)
Differentiate: ∂u∂y = 2ex + dφ
dy = 2(ex − 2y) , using ii)
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Solutions to exercises 18
i.e. dφdy = −4y i.e.
∫dφ = −4
∫y dy i.e. φ = −2y2 + C ′
∴ u = 2(y + 1)ex − 2y2 + C ′
du = 0 gives u = C,
∴ (y + 1)ex − y2 = A , where A = (C − C ′)/2 .
Return to Exercise 3
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Solutions to exercises 19
Exercise 4.
P (x, y)dx + Q(x, y)dy = 0 where P (x, y) = 2xy + 6x ,Q(x, y) = x2 + 4y3
∂P∂y = 2x = ∂Q
∂x , ∴ o.d.e. is exact.
∴ u(x, y) exists such that du = ∂u∂xdx + ∂u
∂y dy
= P dx + Qdy = 0,
Giving i) ∂u∂x = 2xy + 6x , ii) ∂u
∂y = x2 + 4y3 .
Integrate i): u = x2y + 3x2 + φ(y)
Differentiate: ∂u∂y = x2 + dφ
dy = x2 + 4y3 , using ii)
i.e. dφdy = 4y3 i.e.
∫dφ = 4
∫y3 dy i.e. φ = y4 + C ′
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Solutions to exercises 20
∴ u = x2y + 3x2 + y4 + C ′
du = 0 gives u = C,
∴ x2y + 3x2 + y4 = A , where A = C − C ′ .
Return to Exercise 4
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Solutions to exercises 21
Exercise 5.(x− xy2)dx + (8y − x2y)dy = 0
P (x, y) = x− xy2
Q(x, y) = 8y − x2y . ∂P∂y = −2xy = ∂Q
∂x , ∴ o.d.e. is exact.
∴ u(x, y) exists where du = ∂u∂xdx + ∂u
∂y dy
= P dx + Qdy = 0
Giving i) ∂u∂x = x− xy2; ii) ∂u
∂y = 8y − x2y.
Integrate i): u = 12x2(1− y2) + φ(y)
Differentiate: ∂u∂y = − 1
2x2 · 2y + dφdy = 8y − x2y , using ii)
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Solutions to exercises 22
∴ dφdy = 8y i.e.
∫dφ = 8
∫ydy
i.e. φ(y) = 4y2 + C ′ and u = 12x2(1− y2) + 4y2 + C ′
du = 0 gives u = C, ∴ 12x2(1− y2) + 4y2 = A , A = C − C ′ .
Return to Exercise 5
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Solutions to exercises 23
Exercise 6.
P (x, y)dx + Q(x, y)dy = 0 where P (x, y) = e4x + 2xy2 ,Q(x, y) = cos y + 2x2y
∂P∂y = 4xy = ∂Q
∂x , ∴ o.d.e. is exact.
∴ u(x, y) exists such that du = ∂u∂xdx + ∂u
∂y dy
= P dx + Qdy = 0,
Giving i) ∂u∂x = e4x + 2xy2 , ii) ∂u
∂y = cos y + 2x2y .
Integrate i): u = 14e4x + x2y2 + φ(y)
Differentiate: ∂u∂y = 2x2y + dφ
dy = cos y + 2x2y , using ii)
i.e. dφdy = cos y i.e.
∫dφ =
∫cos y dy i.e. φ = sin y + C ′
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Solutions to exercises 24
∴ u = 14e4x + x2y2 + sin y + C ′
du = 0 gives u = C,
∴ 14e4x + x2y2 + sin y = A , where A = C − C ′ .
Return to Exercise 6
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Solutions to exercises 25
Exercise 7.
P (x, y) dx + Q(x, y) dy = 0 where P (x, y) = 3x2 + y cos xQ(x, y) = sin x− 4y3
∂P∂y = cos x = ∂Q
∂x , ∴ o.d.e. is exact.
∴ u(x, y) exists such that du = ∂u∂xdx + ∂u
∂y dy
= P dx + Qdy = 0
Giving i) ∂u∂x = 3x2 + y cos x, ii) ∂u
∂y = sinx− 4y3.
Integrate i): u = x3 + y sinx + φ(y)
Differentiate: ∂u∂y = sinx + dφ
dy = sinx− 4y3 , using ii)
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Solutions to exercises 26
∴ dφdy = −4y3 i.e.
∫dφ = −4
∫y3dy
i.e. φ = −y4 + C ′ and u = x3 + y sinx− y4 + C ′
du = 0 gives u = C, ∴ x3 + y sinx− y4 = A , A = C − C ′ .
Return to Exercise 7
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Solutions to exercises 27
Exercise 8.
P (x, y) dx + Q(x, y) dy = 0 where P (x, y) = x tan−1 y
Q(x, y) = x2
2(1+y2)
∂P∂y = x
1+y2 = ∂Q∂x , ∴ o.d.e. is exact.
∴ u(x, y) exists such that du = ∂u∂xdx + ∂u
∂y dy
= P dx + Qdy = 0,
Giving i) ∂u∂x = x tan−1 y , ii) ∂u
∂y = x2
2(1+y2) .
Integrate i): u = x2
2 tan−1 y + φ(y)
Differentiate: ∂u∂y = x2
21
(1+y2) + dφdy = x2
2(1+y2) , using ii)
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Solutions to exercises 28
∴ dφdy = 0 i.e. φ(y) = C ′
and u = x2
2 tan−1 y + C ′
du = 0 implies u = C , C = constant
∴ x2
2 tan−1 y = A, A = C − C ′ .
Return to Exercise 8
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Solutions to exercises 29
Exercise 9.
P (x, y)dx + Q(x, y)dy = 0 where P (x, y) = 2x + x2y3 ,Q(x, y) = x3y2 + 4y3
∂P∂y = 3x2y2 = ∂Q
∂x , ∴ o.d.e. is exact.
∴ u(x, y) exists such that du = ∂u∂xdx + ∂u
∂y dy
= P dx + Qdy = 0,
Giving i) ∂u∂x = 2x + x2y3 , ii) ∂u
∂y = x3y2 + 4y3 .
Integrate i): u = x2 + x3y3
3 + φ(y)
Differentiate: ∂u∂y = x3y2 + dφ
dy = x3y2 + 4y3 , using ii)
i.e. dφdy = 4y3 i.e.
∫dφ = 4
∫y3 dy i.e. φ = y4 + C ′
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Solutions to exercises 30
∴ u = x2 + x3y3
3 + y4 + C ′
du = 0 gives u = C,
∴ x2 + x3y3
3 + y4 = A , where A = C − C ′ .
Return to Exercise 9
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Solutions to exercises 31
Exercise 10.
(2x3 − 6x2y + 3xy2)dx + (−2x3 + 3x2y − y3)dy = 0
∂P∂y = −6x2 + 6xy = ∂Q
∂x , ∴ o.d.e. is exact.
∴ u(x, y) exists such that du = ∂u∂xdx + ∂u
∂y dy
= P dx + Qdy = 0
Giving i) ∂u∂x = 2x3 − 6x2y + 3xy2, ii) ∂u
∂y = −2x3 + 3x2y − y3.
Integrate i): u = x4
2 − 2x3y + 32x2y2 + φ(y)
Differentiate: ∂u∂y = −2x3 +3x2y + dφ
dy = −2x3 +3x2y− y3 , using ii)
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Solutions to exercises 32
∴ dφdy = −y3 i.e.
∫dφ = −
∫y3dy
i.e. φ(y) = − 14y4 + C ′
and u(x, y) = x4
2 − 2x3y + 32x2y2 − y4
4 + C ′
du = 0 gives u = C,
∴ x4
2 − 2x3y + 32x2y2 − y4
4 = A , A = C − C ′ .
Return to Exercise 10
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Solutions to exercises 33
Exercise 11.
P (x, y)dx + Q(x, y)dy = 0 where P (x, y) = y2 cos x− sinx ,Q(x, y) = 2y sinx + 2
∂P∂y = 2y cos x = ∂Q
∂x , ∴ o.d.e. is exact.
∴ u(x, y) exists such that du = ∂u∂xdx + ∂u
∂y dy
= P dx + Qdy = 0,
Giving i) ∂u∂x = y2 cos x− sinx , ii) ∂u
∂y = 2y sinx + 2 .
Integrate i): u = y2 sinx + cos x + φ(y)
Differentiate: ∂u∂y = 2y sinx + dφ
dy = 2y sinx + 2 , using ii)
i.e. dφdy = 2 i.e.
∫dφ = 2
∫dy i.e. φ = 2y + C ′
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Solutions to exercises 34
∴ u = y2 sinx + cos x + 2y + C ′
du = 0 gives u = C,
∴ y2 sinx + cos x + 2y = A , where A = C − C ′ .
Return to Exercise 11
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