Answer on Question #68974 – Math – Differential Equations
Question
Solve the following differential equation
i)
x 2 p + y 2 q = ( x + y ) z x ^ {2} p + y ^ {2} q = (x + y) z x 2 p + y 2 q = ( x + y ) z Solution
Let
p = ∂ z ∂ x ; q = ∂ z ∂ y . p = \frac {\partial z}{\partial x}; \quad q = \frac {\partial z}{\partial y}. p = ∂ x ∂ z ; q = ∂ y ∂ z .
We can present this quasilinear partial differential equation of the first order
x 2 ∂ z ∂ x + y 2 ∂ z ∂ y = ( x + y ) z x ^ {2} \frac {\partial z}{\partial x} + y ^ {2} \frac {\partial z}{\partial y} = (x + y) z x 2 ∂ x ∂ z + y 2 ∂ y ∂ z = ( x + y ) z
as
V ( x , y , z ) = 0 , V (x, y, z) = 0, V ( x , y , z ) = 0 ,
where
∂ z ∂ x = − ∂ V ∂ x ∂ V ∂ z , \frac {\partial z}{\partial x} = - \frac {\frac {\partial V}{\partial x}}{\frac {\partial V}{\partial z}}, ∂ x ∂ z = − ∂ z ∂ V ∂ x ∂ V , ∂ z ∂ y = − ∂ V ∂ y ∂ V ∂ z . \frac {\partial z}{\partial y} = - \frac {\frac {\partial V}{\partial y}}{\frac {\partial V}{\partial z}}. ∂ y ∂ z = − ∂ z ∂ V ∂ y ∂ V .
Then
x 2 ⋅ ( − ∂ V ∂ x ∂ V ∂ z ) + y 2 ⋅ ( − ∂ V ∂ y ∂ V ∂ z ) = ( x + y ) z , x ^ {2} \cdot \left(- \frac {\frac {\partial V}{\partial x}}{\frac {\partial V}{\partial z}}\right) + y ^ {2} \cdot \left(- \frac {\frac {\partial V}{\partial y}}{\frac {\partial V}{\partial z}}\right) = (x + y) z, x 2 ⋅ ( − ∂ z ∂ V ∂ x ∂ V ) + y 2 ⋅ ( − ∂ z ∂ V ∂ y ∂ V ) = ( x + y ) z , − x 2 ∂ V ∂ x − y 2 ∂ V ∂ y − ( x + y ) z ∂ V ∂ z = 0 , - x ^ {2} \frac {\partial V}{\partial x} - y ^ {2} \frac {\partial V}{\partial y} - (x + y) z \frac {\partial V}{\partial z} = 0, − x 2 ∂ x ∂ V − y 2 ∂ y ∂ V − ( x + y ) z ∂ z ∂ V = 0 , x 2 ∂ V ∂ x + y 2 ∂ V ∂ y + ( x + y ) z ∂ V ∂ z = 0. x ^ {2} \frac {\partial V}{\partial x} + y ^ {2} \frac {\partial V}{\partial y} + (x + y) z \frac {\partial V}{\partial z} = 0. x 2 ∂ x ∂ V + y 2 ∂ y ∂ V + ( x + y ) z ∂ z ∂ V = 0.
The associated system of equations is
d x x 2 = d y y 2 = d z ( x + y ) z \frac {d x}{x ^ {2}} = \frac {d y}{y ^ {2}} = \frac {d z}{(x + y) z} x 2 d x = y 2 d y = ( x + y ) z d z
If d x x 2 = d y y 2 \frac{dx}{x^2} = \frac{dy}{y^2} x 2 d x = y 2 d y , then − 1 x = − 1 y + C 1 -\frac{1}{x} = -\frac{1}{y} + C_1 − x 1 = − y 1 + C 1 and u ( x , y ) = C 1 = 1 y − 1 x u(x,y) = C_1 = \frac{1}{y} - \frac{1}{x} u ( x , y ) = C 1 = y 1 − x 1 , hence y = 1 C 1 + 1 x y = \frac{1}{C_1 + \frac{1}{x}} y = C 1 + x 1 1 ,
y = x C 1 x + 1 y = \frac {x}{C _ {1} x + 1} y = C 1 x + 1 x
If
d x x 2 = d z ( x + y ) z , \frac {d x}{x ^ {2}} = \frac {d z}{(x + y) z}, x 2 d x = ( x + y ) z d z ,
substituting for y y y from (4) into (3) one gets
d x x 2 = d z ( x + x C 1 x + 1 ) z , \frac {d x}{x ^ {2}} = \frac {d z}{(x + \frac {x}{C _ {1} x + 1}) z}, x 2 d x = ( x + C 1 x + 1 x ) z d z , d x x = d z ( 1 + 1 C 1 x + 1 ) z , \frac {d x}{x} = \frac {d z}{\left(1 + \frac {1}{C _ {1} x + 1}\right) z}, x d x = ( 1 + C 1 x + 1 1 ) z d z , d x x = ( C 1 x + 1 ) C 1 x + 2 ⋅ d z z , \frac {d x}{x} = \frac {(C _ {1} x + 1)}{C _ {1} x + 2} \cdot \frac {d z}{z}, x d x = C 1 x + 2 ( C 1 x + 1 ) ⋅ z d z , C 1 x + 2 x ( C 1 x + 1 ) d x = d z z , \frac {C _ {1} x + 2}{x \left(C _ {1} x + 1\right)} d x = \frac {d z}{z}, x ( C 1 x + 1 ) C 1 x + 2 d x = z d z , ∫ C 1 x + 2 x ( C 1 x + 1 ) d x = ∫ d z z , \int \frac {C _ {1} x + 2}{x \left(C _ {1} x + 1\right)} d x = \int \frac {d z}{z}, ∫ x ( C 1 x + 1 ) C 1 x + 2 d x = ∫ z d z , ∫ ( 2 x − C 1 C 1 x + 1 ) d x = ln ∣ z ∣ + ln ∣ C 2 ∣ , \int \left(\frac {2}{x} - \frac {C _ {1}}{C _ {1} x + 1}\right) d x = \ln | z | + \ln | C _ {2} |, ∫ ( x 2 − C 1 x + 1 C 1 ) d x = ln ∣ z ∣ + ln ∣ C 2 ∣ , 2 ln ∣ x ∣ − ln ∣ C 1 x + 1 ∣ = ln ∣ C 2 z ∣ , 2 \ln | x | - \ln | C _ {1} x + 1 | = \ln | C _ {2} z |, 2 ln ∣ x ∣ − ln ∣ C 1 x + 1∣ = ln ∣ C 2 z ∣ , x 2 C 1 x + 1 = C 2 z , \frac {x ^ {2}}{C _ {1} x + 1} = C _ {2} z, C 1 x + 1 x 2 = C 2 z , C 2 = x 2 z ( C 1 x + 1 ) , C _ {2} = \frac {x ^ {2}}{z (C _ {1} x + 1)}, C 2 = z ( C 1 x + 1 ) x 2 , C 2 = x 2 z ( ( 1 y − 1 x ) x + 1 ) C _ {2} = \frac {x ^ {2}}{z \left(\left(\frac {1}{y} - \frac {1}{x}\right) x + 1\right)} C 2 = z ( ( y 1 − x 1 ) x + 1 ) x 2 C 2 = x 2 z y 2 , C _ {2} = \frac {x ^ {2}}{z _ {y} ^ {2}}, C 2 = z y 2 x 2 , v ( x , y ) = C 2 = x y z . v (x, y) = C _ {2} = \frac {x y}{z}. v ( x , y ) = C 2 = z x y .
The general integral is given by
F ( u , v ) = 0 , F (u, v) = 0, F ( u , v ) = 0 , F ( 1 y − 1 x , x y z ) = 0 , F \left(\frac {1}{y} - \frac {1}{x}, \frac {x y}{z}\right) = 0, F ( y 1 − x 1 , z x y ) = 0 , F ( x − y x y , x y z ) = 0 , F \left(\frac {x - y}{x y}, \frac {x y}{z}\right) = 0, F ( x y x − y , z x y ) = 0 ,
where F F F is an arbitrary function.
For example, if we take
F ( u , v ) = − C u v − 1 = − C ⋅ x − y x y ⋅ x y z − 1 = C ⋅ y − x z − 1 = 0 , F (u, v) = - C u v - 1 = - C \cdot \frac {x - y}{x y} \cdot \frac {x y}{z} - 1 = C \cdot \frac {y - x}{z} - 1 = 0, F ( u , v ) = − C uv − 1 = − C ⋅ x y x − y ⋅ z x y − 1 = C ⋅ z y − x − 1 = 0 ,
then z = C ( y − x ) z = C(y - x) z = C ( y − x ) is one of solutions of (1).
Function z = 0 z = 0 z = 0 is also a solution of equation (1) because ∂ z ∂ x = 0 \frac{\partial z}{\partial x} = 0 ∂ x ∂ z = 0 , ∂ z ∂ y = 0 \frac{\partial z}{\partial y} = 0 ∂ y ∂ z = 0 .
If x = 0 x = 0 x = 0 , then y 2 ∂ z ∂ y = y z y^{2}\frac{\partial z}{\partial y} = yz y 2 ∂ y ∂ z = yz , d z z = d y y \frac{dz}{z} = \frac{dy}{y} z d z = y d y , z y = C 1 \frac{z}{y} = C_{1} y z = C 1 and a solution of (1) is
( x , y , z ) = ( 0 , y , C 1 y ) = s ( 0 , 1 , C 1 ) . (x, y, z) = (0, y, C _ {1} y) = s (0, 1, C _ {1}). ( x , y , z ) = ( 0 , y , C 1 y ) = s ( 0 , 1 , C 1 ) .
If y = 0 y = 0 y = 0 , then x 2 ∂ z ∂ x = x z x^{2}\frac{\partial z}{\partial x} = xz x 2 ∂ x ∂ z = x z , d z z = d x x \frac{dz}{z} = \frac{dx}{x} z d z = x d x , z x = C 2 \frac{z}{x} = C_{2} x z = C 2 and a solution of (1) is
( x , y , z ) = ( x , 0 , C 2 x ) = t ( 1 , 0 , C 2 ) . (x, y, z) = (x, 0, C _ {2} x) = t (1, 0, C _ {2}). ( x , y , z ) = ( x , 0 , C 2 x ) = t ( 1 , 0 , C 2 ) .
If y = − x y = -x y = − x , then z z z is arbitrary and a solution of (1) is ( x , y , z ) = ( x , − x , z ) = ( s , − s , t ) (x, y, z) = (x, -x, z) = (s, -s, t) ( x , y , z ) = ( x , − x , z ) = ( s , − s , t ) .
Answer: F ( x − y x y , x y z ) = 0 ; z = C 1 y , x = 0 ; z = C 2 x , y = 0 ; y = − x . F\left(\frac{x - y}{xy}, \frac{xy}{z}\right) = 0; z = C_1y, x = 0; z = C_2x, y = 0; y = -x. F ( x y x − y , z x y ) = 0 ; z = C 1 y , x = 0 ; z = C 2 x , y = 0 ; y = − x .
Question
Solve the following differential equation
ii)
p − q + 3 x = 0 \sqrt {p} - \sqrt {q} + 3 x = 0 p − q + 3 x = 0 Solution
F ( x , y , z , p , q ) = p − q + 3 x , F (x, y, z, p, q) = \sqrt {p} - \sqrt {q} + 3 x, F ( x , y , z , p , q ) = p − q + 3 x , ∂ F ∂ x = 3 , ∂ F ∂ y = 0 , ∂ F ∂ z = 0 , ∂ F ∂ p = 1 2 p , ∂ F ∂ q = − 1 2 q . \frac {\partial F}{\partial x} = 3, \frac {\partial F}{\partial y} = 0, \frac {\partial F}{\partial z} = 0, \frac {\partial F}{\partial p} = \frac {1}{2 \sqrt {p}}, \frac {\partial F}{\partial q} = - \frac {1}{2 \sqrt {q}}. ∂ x ∂ F = 3 , ∂ y ∂ F = 0 , ∂ z ∂ F = 0 , ∂ p ∂ F = 2 p 1 , ∂ q ∂ F = − 2 q 1 .
The characteristic system of ordinary differential equations is
d x F p = d y F q = d z p F p + q F q = − d p F x + p F z = − d q F y + q F z \frac {d x}{F _ {p}} = \frac {d y}{F _ {q}} = \frac {d z}{p F _ {p} + q F _ {q}} = - \frac {d p}{F _ {x} + p F _ {z}} = - \frac {d q}{F _ {y} + q F _ {z}} F p d x = F q d y = p F p + q F q d z = − F x + p F z d p = − F y + q F z d q d x 1 2 p = d y − 1 2 q = d z p ⋅ 1 2 p + q ⋅ ( − 1 2 q ) = − d p 3 = − d q 0 \frac {d x}{\frac {1}{2 \sqrt {p}}} = \frac {d y}{- \frac {1}{2 \sqrt {q}}} = \frac {d z}{p \cdot \frac {1}{2 \sqrt {p}} + q \cdot \left(- \frac {1}{2 \sqrt {q}}\right)} = - \frac {d p}{3} = - \frac {d q}{0} 2 p 1 d x = − 2 q 1 d y = p ⋅ 2 p 1 + q ⋅ ( − 2 q 1 ) d z = − 3 d p = − 0 d q d x 1 2 p = d y − 1 2 q = d z p 2 − q 2 = − d p 3 = − d q 0 \frac {d x}{\frac {1}{2 \sqrt {p}}} = \frac {d y}{- \frac {1}{2 \sqrt {q}}} = \frac {d z}{\frac {\sqrt {p}}{2} - \frac {\sqrt {q}}{2}} = - \frac {d p}{3} = - \frac {d q}{0} 2 p 1 d x = − 2 q 1 d y = 2 p − 2 q d z = − 3 d p = − 0 d q
If
d y 1 1 2 q = − d q 0 , \frac {\frac {d y}{1}}{\frac {1}{2 \sqrt {q}}} = - \frac {d q}{0}, 2 q 1 1 d y = − 0 d q , 2 q d y = d q 0 , 2 \sqrt {q} d y = \frac {d q}{0}, 2 q d y = 0 d q , d q q = 0 d y , \frac {d q}{\sqrt {q}} = 0 d y, q d q = 0 d y , 2 q = K , 2 \sqrt {q} = K, 2 q = K , ∂ z ∂ y = q = C 1 2 \frac {\partial z}{\partial y} = q = C _ {1} ^ {2} ∂ y ∂ z = q = C 1 2 ( K , C 1 (K, C_{1} ( K , C 1 are arbitrary constants),
hence
z = C 1 2 y + φ ( x ) , z = C _ {1} ^ {2} y + \varphi (x), z = C 1 2 y + φ ( x ) , p = ∂ z ∂ x = φ ′ ( x ) p = \frac {\partial z}{\partial x} = \varphi^ {\prime} (x) p = ∂ x ∂ z = φ ′ ( x )
Substituting (6), (7) into equation (5)
φ ′ ( x ) − C 1 + 3 x = 0 , \sqrt {\varphi^ {\prime} (x)} - C _ {1} + 3 x = 0, φ ′ ( x ) − C 1 + 3 x = 0 , φ ′ ( x ) = − 3 x + C 1 \sqrt {\varphi^ {\prime} (x)} = - 3 x + C _ {1} φ ′ ( x ) = − 3 x + C 1 φ ′ ( x ) = ( − 3 x + C 1 ) 2 = 9 x 2 − 6 x C 1 + C 1 2 \varphi^ {\prime} (x) = (- 3 x + C _ {1}) ^ {2} = 9 x ^ {2} - 6 x C _ {1} + C _ {1} ^ {2} φ ′ ( x ) = ( − 3 x + C 1 ) 2 = 9 x 2 − 6 x C 1 + C 1 2 φ ( x ) = 9 x 3 3 − 6 C 1 x 2 2 + C 1 2 x + C 2 = 3 x 3 − 3 C 1 x 2 + C 1 2 x + C 2 , \varphi (x) = 9 \frac {x ^ {3}}{3} - 6 C _ {1} \frac {x ^ {2}}{2} + C _ {1} ^ {2} x + C _ {2} = 3 x ^ {3} - 3 C _ {1} x ^ {2} + C _ {1} ^ {2} x + C _ {2}, φ ( x ) = 9 3 x 3 − 6 C 1 2 x 2 + C 1 2 x + C 2 = 3 x 3 − 3 C 1 x 2 + C 1 2 x + C 2 ,
where C 2 C_2 C 2 is arbitrary constant.
Then
z = C 1 2 y + φ ( x ) = 3 x 3 − 3 C 1 x 2 + C 1 2 x + C 2 + C 1 2 y z = C _ {1} ^ {2} y + \varphi (x) = 3 x ^ {3} - 3 C _ {1} x ^ {2} + C _ {1} ^ {2} x + C _ {2} + C _ {1} ^ {2} y z = C 1 2 y + φ ( x ) = 3 x 3 − 3 C 1 x 2 + C 1 2 x + C 2 + C 1 2 y
If ∂ z ∂ x = p = 0 \frac{\partial z}{\partial x} = p = 0 ∂ x ∂ z = p = 0 , then it follows from (5) that
∂ z ∂ y = q = 9 x 2 ⇒ z = 9 x 2 y + φ ( x ) = 9 C 1 2 y + C 2 \frac{\partial z}{\partial y} = q = 9x^2 \Rightarrow z = 9x^2y + \varphi(x) = 9C_1^2y + C_2 ∂ y ∂ z = q = 9 x 2 ⇒ z = 9 x 2 y + φ ( x ) = 9 C 1 2 y + C 2 (formula (8) already contains this solution).
If ∂ z ∂ y = q = 0 \frac{\partial z}{\partial y} = q = 0 ∂ y ∂ z = q = 0 , then it follows from (5) that
∂ z ∂ x = p = 9 x 2 ⇒ z = 3 x 3 + ψ ( y ) = 3 x 3 + c \frac{\partial z}{\partial x} = p = 9x^2 \Rightarrow z = 3x^3 + \psi(y) = 3x^3 + c ∂ x ∂ z = p = 9 x 2 ⇒ z = 3 x 3 + ψ ( y ) = 3 x 3 + c (formula (8) already contains this solution).
Answer: z = 3 x 3 − 3 C 1 x 2 + C 1 2 x + C 2 + C 1 2 y z = 3x^{3} - 3C_{1}x^{2} + C_{1}^{2}x + C_{2} + C_{1}^{2}y z = 3 x 3 − 3 C 1 x 2 + C 1 2 x + C 2 + C 1 2 y .
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