Answer on Question #51034 – Math – Differential Calculus
Question:
a) Find f ( y ) f(y) f ( y ) so that equation f ( y ) d x − z x d y − x y ln y d z = 0 f(y)dx - zxdy - xy\ln ydz = 0 f ( y ) d x − z x d y − x y ln y d z = 0 is integrable. Also obtain the corresponding integral using Natani's method.
b) Find the differential equation of the family of surfaces Φ ( z ( x + y ) 2 , x 2 − y 2 ) = 0 \Phi (z(x + y)^2,x^2 -y^2) = 0 Φ ( z ( x + y ) 2 , x 2 − y 2 ) = 0
Solution:
a) Equation f ( y ) d x − z x d y − x y ln y d z = 0 f(y)dx - zxdy - xy\ln ydz = 0 f ( y ) d x − z x d y − x y ln y d z = 0 is integrable, if
X ⋅ rot X = 0 X \cdot \operatorname {rot} X = 0 X ⋅ rot X = 0 X = ( f ( y ) , − z x , − x y ln y ) X = (f (y), - z x, - x y \ln y) X = ( f ( y ) , − z x , − x y ln y )
Let's calculate rot X \operatorname{rot} X rot X
rot X = ∇ × X = ∣ i j k ∂ ∂ x ∂ ∂ y ∂ ∂ z f ( y ) − z x − x y ln y ∣ = i ( ∂ ∂ y ( − x y ln y ) − ∂ ∂ z ( − x z ) ) − j ( ∂ ∂ x ( − x y ln y ) − ∂ ∂ z f ( y ) ) + k ( ∂ ∂ x ( − z x ) − ∂ ∂ y f ( y ) ) = ( − x ln y ) i + ( y ln y ) j + ( − z − f ′ ( y ) ) k \begin{array}{l}
\operatorname {rot} X = \nabla \times X = \left| \begin{array}{c c c}
\mathbf {i} & \mathbf {j} & \mathbf {k} \\
\frac {\partial}{\partial x} & \frac {\partial}{\partial y} & \frac {\partial}{\partial z} \\
f (y) & - z x & - x y \ln y
\end{array} \right| \\
= \boldsymbol {i} \left(\frac {\partial}{\partial y} (- x y \ln y) - \frac {\partial}{\partial z} (- x z)\right) - \boldsymbol {j} \left(\frac {\partial}{\partial x} (- x y \ln y) - \frac {\partial}{\partial z} f (y)\right) \\
+ \boldsymbol {k} \left(\frac {\partial}{\partial x} (- z x) - \frac {\partial}{\partial y} f (y)\right) = (- x \ln y) \boldsymbol {i} + (y \ln y) \boldsymbol {j} + (- z - f ^ {\prime} (y)) \boldsymbol {k} \\
\end{array} rot X = ∇ × X = ∣ ∣ i ∂ x ∂ f ( y ) j ∂ y ∂ − z x k ∂ z ∂ − x y ln y ∣ ∣ = i ( ∂ y ∂ ( − x y ln y ) − ∂ z ∂ ( − x z ) ) − j ( ∂ x ∂ ( − x y ln y ) − ∂ z ∂ f ( y ) ) + k ( ∂ x ∂ ( − z x ) − ∂ y ∂ f ( y ) ) = ( − x ln y ) i + ( y ln y ) j + ( − z − f ′ ( y )) k
Then
X ⋅ rot X = − x ln y ⋅ f ( y ) + x y ln y f ′ ( y ) = 0 X \cdot \operatorname {rot} X = - x \ln y \cdot f (y) + x y \ln y f ^ {\prime} (y) = 0 X ⋅ rot X = − x ln y ⋅ f ( y ) + x y ln y f ′ ( y ) = 0
Thus x ln y ⋅ ( y f ′ ( y ) − f ( y ) ) = 0 x\ln y\cdot (yf'(y) - f(y)) = 0 x ln y ⋅ ( y f ′ ( y ) − f ( y )) = 0 , hence y f ′ ( y ) − f ( y ) = 0 yf^{\prime}(y) - f(y) = 0 y f ′ ( y ) − f ( y ) = 0
The solution of the last equation is determined by
d f f = d y y → ln ∣ f ( y ) ∣ = ln ∣ y ∣ + ln ∣ A ∣ → f ( y ) = A ⋅ y \frac {d f}{f} = \frac {d y}{y} \rightarrow \ln | f (y) | = \ln | y | + \ln | A | \rightarrow f (y) = A \cdot y f df = y d y → ln ∣ f ( y ) ∣ = ln ∣ y ∣ + ln ∣ A ∣ → f ( y ) = A ⋅ y
where A A A is a real constant. Finally, equation takes the form
A y d x − z x d y − x y ln y d z = 0 A y d x - z x d y - x y \ln y d z = 0 A y d x − z x d y − x y ln y d z = 0
Using Natani's method we firstly put z = const z = \text{const} z = const and solve the obtained equation
A y d x = z x d y → A d x x = z d y y → A ln x = z ln y + F ( z ) A y d x = z x d y \rightarrow A \frac {d x}{x} = z \frac {d y}{y} \rightarrow A \ln x = z \ln y + F (z) A y d x = z x d y → A x d x = z y d y → A ln x = z ln y + F ( z )
Now we let x = 1 x = 1 x = 1 . Then equation takes the form
− z d y − y ln y d z = 0 - z d y - y \ln y d z = 0 − z d y − y ln y d z = 0
and
\begin{array}{l}
F(z) = -z \cdot \ln y.
Thus,
z d y + y ln y d z = 0 → d y y ln y + d z z = 0 → ln ∣ ln y ∣ = − ln ∣ z ∣ + ln ∣ C ∣ → ln y = C z z \, dy + y \ln y \, dz = 0 \quad \rightarrow \frac{dy}{y \ln y} + \frac{dz}{z} = 0 \quad \rightarrow \ln |\ln y| = -\ln |z| + \ln |C| \quad \rightarrow \\
\ln y = \frac{C}{z} z d y + y ln y d z = 0 → y ln y d y + z d z = 0 → ln ∣ ln y ∣ = − ln ∣ z ∣ + ln ∣ C ∣ → ln y = z C
Therefore,
F ( z ) = − z ln y = − z ⋅ C z = − C = K F(z) = -z \ln y = -z \cdot \frac{C}{z} = -C = K F ( z ) = − z ln y = − z ⋅ z C = − C = K
(inother constant).
Finally,
A ln x = z ln y + K A \ln x = z \ln y + K A ln x = z ln y + K
where K K K is an arbitrary real constant.
b) The general solution of first-order differential equation
Φ ( z ( x + y ) 2 , x 2 − y 2 ) = 0 \Phi(z(x + y)^2, x^2 - y^2) = 0 Φ ( z ( x + y ) 2 , x 2 − y 2 ) = 0
implies that
z ( x + y ) 2 = c 1 = const z(x + y)^2 = c_1 = \text{const} z ( x + y ) 2 = c 1 = const x 2 − y 2 = c 2 = const x^2 - y^2 = c_2 = \text{const} x 2 − y 2 = c 2 = const
After differentiating these both equations we get
d z = − 2 z ⋅ d x + d y x + y dz = -2z \cdot \frac{dx + dy}{x + y} d z = − 2 z ⋅ x + y d x + d y x d x = y d y x \, dx = y \, dy x d x = y d y
First-order differential equation
a ⋅ ∂ z ∂ x + b ⋅ ∂ z ∂ y = c a \cdot \frac{\partial z}{\partial x} + b \cdot \frac{\partial z}{\partial y} = c a ⋅ ∂ x ∂ z + b ⋅ ∂ y ∂ z = c
is equivalent to
d x a = d y b = d z c \frac{dx}{a} = \frac{dy}{b} = \frac{dz}{c} a d x = b d y = c d z
From x d x = y d y x \, dx = y \, dy x d x = y d y and previous equation, we get
d x y = d y x → a = y , b = x \frac{dx}{y} = \frac{dy}{x} \quad \rightarrow \quad a = y, \quad b = x y d x = x d y → a = y , b = x
Putting d x = y x d y dx = \frac{y}{x} \, dy d x = x y d y into d z = − 2 z ⋅ d x + d y x + y dz = -2z \cdot \frac{dx + dy}{x + y} d z = − 2 z ⋅ x + y d x + d y , we get
d z = − 2 z ⋅ d y x dz = -2z \cdot \frac{dy}{x} d z = − 2 z ⋅ x d y
Thus
d z c = − 2 z c ⋅ d y x = d y b = d y x → c = − 2 z \frac{dz}{c} = -\frac{2z}{c} \cdot \frac{dy}{x} = \frac{dy}{b} = \frac{dy}{x} \rightarrow c = -2z c d z = − c 2 z ⋅ x d y = b d y = x d y → c = − 2 z
Finally,
d x y = d y x = d z − 2 z \frac{dx}{y} = \frac{dy}{x} = \frac{dz}{-2z} y d x = x d y = − 2 z d z
or
y ⋅ ∂ z ∂ x + x ⋅ ∂ z ∂ y = − 2 z y \cdot \frac{\partial z}{\partial x} + x \cdot \frac{\partial z}{\partial y} = -2z y ⋅ ∂ x ∂ z + x ⋅ ∂ y ∂ z = − 2 z
Answer: y ⋅ ∂ z ∂ x + x ⋅ ∂ z ∂ y = − 2 z y \cdot \frac{\partial z}{\partial x} + x \cdot \frac{\partial z}{\partial y} = -2z y ⋅ ∂ x ∂ z + x ⋅ ∂ y ∂ z = − 2 z
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