ANSWER on Question #79036 – Math – Differential Equations
QUESTION
Find the integral surface of the PDE
( x − y ) p + ( y − x − z ) q = z (x - y)p + (y - x - z)q = z ( x − y ) p + ( y − x − z ) q = z SOLUTION
Consider a quasilinear equation
a ( x , y , z ) p + b ( x , y , z ) q = c ( x , y , z ) . a(x, y, z)p + b(x, y, z)q = c(x, y, z). a ( x , y , z ) p + b ( x , y , z ) q = c ( x , y , z ) .
By Lagrange’s method the auxiliary equations are as following:
d x a ( x , y , z ) = d y b ( x , y , z ) = d z c ( x , y , z ) . \frac{dx}{a(x, y, z)} = \frac{dy}{b(x, y, z)} = \frac{dz}{c(x, y, z)}. a ( x , y , z ) d x = b ( x , y , z ) d y = c ( x , y , z ) d z .
So, for the given quasilinear equation we come to the system in the symmetric form
d x x − y = d y y − x − z = d z z . \frac{dx}{x - y} = \frac{dy}{y - x - z} = \frac{dz}{z}. x − y d x = y − x − z d y = z d z .
One of a way to solve the system in symmetric form is to use the equal fractions property
a 1 b 1 = a 2 b 2 = ⋯ = a n b n = λ 1 a 1 + λ 2 a 2 + ⋯ + λ n a n λ 1 b 1 + λ 2 b 2 + ⋯ + λ n b n \frac{a_1}{b_1} = \frac{a_2}{b_2} = \cdots = \frac{a_n}{b_n} = \frac{\lambda_1 a_1 + \lambda_2 a_2 + \cdots + \lambda_n a_n}{\lambda_1 b_1 + \lambda_2 b_2 + \cdots + \lambda_n b_n} b 1 a 1 = b 2 a 2 = ⋯ = b n a n = λ 1 b 1 + λ 2 b 2 + ⋯ + λ n b n λ 1 a 1 + λ 2 a 2 + ⋯ + λ n a n
In our case,
Choosing λ 1 = λ 2 = λ 3 = 1 \lambda_1 = \lambda_2 = \lambda_3 = 1 λ 1 = λ 2 = λ 3 = 1 as multipliers, each fraction on (1):
d x x − y = d y y − x − z = d z z = 1 ⋅ d x + 1 ⋅ d y + 1 ⋅ d z 1 ⋅ ( x − y ) + 1 ⋅ ( y − x − z ) + 1 ⋅ z → \frac{dx}{x - y} = \frac{dy}{y - x - z} = \frac{dz}{z} = \frac{1 \cdot dx + 1 \cdot dy + 1 \cdot dz}{1 \cdot (x - y) + 1 \cdot (y - x - z) + 1 \cdot z} \rightarrow x − y d x = y − x − z d y = z d z = 1 ⋅ ( x − y ) + 1 ⋅ ( y − x − z ) + 1 ⋅ z 1 ⋅ d x + 1 ⋅ d y + 1 ⋅ d z → d x x − y = d y y − x − z = d z z = d ( x + y + z ) x − y + y − x − z + z → d x x − y = d y y − x − z = d z z = d ( x + y + z ) 0 → \frac{dx}{x - y} = \frac{dy}{y - x - z} = \frac{dz}{z} = \frac{d(x + y + z)}{x - y + y - x - z + z} \rightarrow \frac{dx}{x - y} = \frac{dy}{y - x - z} = \frac{dz}{z} = \frac{d(x + y + z)}{0} \rightarrow x − y d x = y − x − z d y = z d z = x − y + y − x − z + z d ( x + y + z ) → x − y d x = y − x − z d y = z d z = 0 d ( x + y + z ) → d ( x + y + z ) = 0 → x + y + z = C 1 d(x + y + z) = 0 \rightarrow \boxed{x + y + z = C_1} d ( x + y + z ) = 0 → x + y + z = C 1
Take the last two fractions of (1) and using (2) we get
{ d y y − x − z = d z z x + y + z = C 1 → { d y y − ( x + z ) = d z z x + z = C 1 − y → d y y − ( C 1 − y ) = d z z → d y y − C 1 + y = d z z → \left\{ \begin{array}{l} \frac {d y}{y - x - z} = \frac {d z}{z} \\ x + y + z = C _ {1} \end{array} \right. \to \left\{ \begin{array}{l} \frac {d y}{y - (x + z)} = \frac {d z}{z} \\ x + z = C _ {1} - y \end{array} \right. \to \frac {d y}{y - (C _ {1} - y)} = \frac {d z}{z} \to \frac {d y}{y - C _ {1} + y} = \frac {d z}{z} \to { y − x − z d y = z d z x + y + z = C 1 → { y − ( x + z ) d y = z d z x + z = C 1 − y → y − ( C 1 − y ) d y = z d z → y − C 1 + y d y = z d z → d y 2 y − C 1 = d z z → ∫ d y y − C 1 + y = ∫ d z z → 1 2 ⋅ ln ∣ 2 y − C 1 ∣ = ln ∣ z ∣ + ln ∣ C 2 ∣ ∣ × ( 2 ) → \frac {d y}{2 y - C _ {1}} = \frac {d z}{z} \rightarrow \int \frac {d y}{y - C _ {1} + y} = \int \frac {d z}{z} \rightarrow \frac {1}{2} \cdot \ln | 2 y - C _ {1} | = \ln | z | + \ln | C _ {2} | \Bigg | \times (2) \rightarrow 2 y − C 1 d y = z d z → ∫ y − C 1 + y d y = ∫ z d z → 2 1 ⋅ ln ∣2 y − C 1 ∣ = ln ∣ z ∣ + ln ∣ C 2 ∣ ∣ ∣ × ( 2 ) → ln ∣ 2 y − C 1 ∣ = 2 ⋅ ln ∣ z ∣ + 2 ⋅ ln ∣ C 2 ∣ ⏟ ln ∣ C 3 ∣ → ln ∣ 2 y − C 1 ∣ − ln ∣ z 2 ∣ = ln ∣ C 3 ∣ → ln ∣ 2 y − C 1 z 2 ∣ = ln ∣ C 3 ∣ → \ln | 2 y - C _ {1} | = 2 \cdot \ln | z | + \underbrace {2 \cdot \ln | C _ {2} |} _ {\ln | C _ {3} |} \rightarrow \ln | 2 y - C _ {1} | - \ln | z ^ {2} | = \ln | C _ {3} | \rightarrow \ln \left| \frac {2 y - C _ {1}}{z ^ {2}} \right| = \ln | C _ {3} | \rightarrow ln ∣2 y − C 1 ∣ = 2 ⋅ ln ∣ z ∣ + l n ∣ C 3 ∣ 2 ⋅ ln ∣ C 2 ∣ → ln ∣2 y − C 1 ∣ − ln ∣ z 2 ∣ = ln ∣ C 3 ∣ → ln ∣ ∣ z 2 2 y − C 1 ∣ ∣ = ln ∣ C 3 ∣ → ( 2 y − C 1 ) z 2 = C 3 → [ Again, we use equality (2) x + y + z = C 1 ] → ( 2 y − ( x + y + z ) ) z 2 = C 3 → \frac {(2 y - C _ {1})}{z ^ {2}} = C _ {3} \rightarrow \left[\begin{array}{c}\text{Again, we use equality (2)}\\x + y + z = C _ {1}\end{array}\right]\rightarrow\frac {(2 y - (x + y + z))}{z ^ {2}} = C _ {3} \rightarrow z 2 ( 2 y − C 1 ) = C 3 → [ Again, we use equality (2) x + y + z = C 1 ] → z 2 ( 2 y − ( x + y + z )) = C 3 → 2 y − x − y − z z 2 = C 3 → y − x − z z 2 = C 3 \frac {2 y - x - y - z}{z ^ {2}} = C _ {3} \rightarrow \boxed {\frac {y - x - z}{z ^ {2}} = C _ {3}} z 2 2 y − x − y − z = C 3 → z 2 y − x − z = C 3
We have found two integrals for the given equation
{ x + y + z = C 1 y − x − z z 2 = C 3 \left\{ \begin{array}{l} x + y + z = C _ {1} \\ \frac {y - x - z}{z ^ {2}} = C _ {3} \end{array} \right. { x + y + z = C 1 z 2 y − x − z = C 3
Therefore, any integral surface of the differential equation ( x − y ) p + ( y − x − z ) q = z (x - y)p + (y - x - z)q = z ( x − y ) p + ( y − x − z ) q = z is described by the equation
φ ( C 1 , C 3 ) = 0 → φ ( x + y + z , y − x − z z 2 ) = 0 \varphi \left(C _ {1}, C _ {3}\right) = 0 \rightarrow \boxed {\varphi \left(x + y + z, \frac {y - x - z}{z ^ {2}}\right) = 0} φ ( C 1 , C 3 ) = 0 → φ ( x + y + z , z 2 y − x − z ) = 0
where φ \varphi φ is an arbitrary function, a smooth function.
ANSWER: ( x − y ) p + ( y − x − z ) q = z → φ ( x + y + z , y − x − z z 2 ) = 0. (x - y)p + (y - x - z)q = z \to \varphi \left(x + y + z, \frac{y - x - z}{z^2}\right) = 0. ( x − y ) p + ( y − x − z ) q = z → φ ( x + y + z , z 2 y − x − z ) = 0.
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