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Additional problems, week 1-4 Example 1. Compute the solution of the pde yz

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Additional problems, week 1-4

Example 1. Compute the solution of the pde

yzx−xzy = 0.

Example 2. Compute the solution of the pde

zx+yzy = 0.

Example 3. Compute the solution of the pde

√1−x2zx+zy = 0, z(0, y) =y.

Example 4. Find the integral surfaces of the vector field (x2, y2,(x+y)z)T containing the line

(a) x=y =z, (b) x= 1, y=z, (c) x=y,z =x2.

Example 5. Compute the solution of the pde zux+yuy+xuz = 0.

Example 6. Compute the solution of the pde x2ux+y2uy+ (x+y)zuz = 0.

Example 7. Solve the pdes (a) azx+bzy =−cz, (b) xzx+ (y−1)zy =xz.

Example 8. Solve the initial value problem

xzx+ (y−1)zy =xz z(x,0) =g(x).

Example 9. Find the general solution u(x, y, z) of the equation

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Solutions for the additional problems

Solution 1. Here P =y, Q=−x and we get dy

dx = Q P dx

y =− dy x xdx=−ydy x2 =−y2+C

u(x, y) =C =x2+y2

z(x, y) =f(u(x, y)) =f(x2+y2).

Solution 2. With P = 1 and Q=y we get dx

1 = dy y x= ln|y|+C

u(x, y) =C =x−ln|y|

z(x, y) =f(u(x, y)) =f(x−ln|y|).

Solution 3. We get

√ dx

1−x2 = dy 1 arcsin(x) =y+C

u(x, y) =C = arcsin(x)−y

z(x, y) =f(u(x, y)) =f(arcsin(x)−y).

The initial condition leads to

f(arcsin(0)−y) =y f(−y) =y

z(x, y) =y−arcsin(x).

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Solution 4. The equations read dx

x2 = dy

y2 = dz (x+y)z and first we use

dx x2 = dy

y2

− 1

x =−1 y +c c1 =u1(x, y, z) = 1

x − 1 y. Next we use

dx

x2 = dz (x+y)z 1

x + y x2

dx= dz

z |y= 1

x−c 1

1

x + 1

x−c1x2

dx= dz z

ln|x|+ ln|x−c1x2| −2 ln|1−c1x|= ln|z|+c x(x−c1x2)

(1−c1x)2 =c2z x(x−x+ xy2)

(1−1 + xy)2 =c2z x3/y

(x/y)2 =c2z

xy =c2z

c2 =u2(x, y, z) = xy z .

Solution for (a): It holdsϕ(t) =ψ(t) =χ(t) and we get

1 1

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This results in

f(0, ϕ(t)) = 0 f(F1, F2) = F1

f 1

x − 1 y,xy

z

= 1 x − 1

y = 0 1

x− 1 y = 0.

Solution for (b): Here c= (1, ψ(t), ψ(t) results in u1 = 1− 1

ψ(t), u2 = 1 f(1−ψ(t)1,1) = 0 f(F1, F2) = F2−1 f

1 x − 1

y,xy z

= xy

z −1 = 0 xy

z = 1 xy =z.

Solution for (c): Here we havec= (ϕ(t), ϕ(t), ϕ(t)2)T and this results in u1 = 1

ϕ(t) − 1 ϕ(t) = 0 u2 = ϕ(t)ϕ(t)

ϕ(t)2 = 1 f(0,1) = 0

f(F1, F2) = g(F1)−F2 withg(0) = 1 g

1 x − 1

y

−xy z = 0 zg

1 x − 1

y

=xy withg(0) = 1.

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Solution 5. The solution of the pdezux+yuy +xuz = 0 can be computed as follows dx

z = dy y = dz

x . First we use

dx z = dz

x xdx=zdz

x2 2 = z2

2 −˜c

c1 =u1(x, y, z) =x2 −z2. Next we use

dx z = dy

y

√ dx x2 −c1

= dy y ln|x+p

x2−c1|= ln|y|+ ˜c x+p

x2 −c1 =c2y x+z=c2y

c2 =u2(x, y, z) = x+z y and the final solution reads

u(x, y, z) =f(u1, u2) =f(x2−z2,x+z y ).

Solution 6. From solution 4 we know

c1 =u1(x, y, z) = 1 x − 1

y, c2 =u2(x, y, z) = xy

z . Finally we get

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Solution 7. Solution for (a): In order to compute the integral curves we get dx

a = dy

b = dz

−cz. First we solve

bdx=ady bx=ay+c1

c1 =u1(x, y, z) =bx−ay.

Next we get dx

a = dz

−cz

− c

a dx= dz z

− c

ax= ln|z˜c exp

−c ax

= z c2

c2 =u2(x, y, z) =zexpc ax

. So we get the form

u2 =ze

c ax

=f(bx−ay) z =f(bx−ay)e

c ax.

Solution for (b): The integral curves are computed for dx

x = dy

y−1 = dz xz. Integral curves:

ln|x|= ln|y−1|+ ˜c x= (y−1)c1

c1 =u1(x, y, z) = x y−1

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and dx

x = dz xz dx= dz z x= ln|z| −˜c ex = z

c2

c2 =u2(x, y, z) =zex. This results in

zex =f(x/(y−1)) z =exf(x/(y−1)).

Solution 8. The general solution reads

z =exf(x/(y−1)).

With the initial condition we get

z(x,0) =exf(x/(0−1)) =exf(−x) =g(x) f(−x) =g(x)e−x ⇒f(t) =g(−t)et z(x, y) =exg

x 1−y

e

x y−1

=e

x2

y−1g(x/(1−y)). Solution 9. Integral curves:

dx

x = dy

y−1 = dz xz, c1 =u1(x, y, z) = x

y−1, c2 =u2(x, y, z) =zex.

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