Answer on Question #66338 – Math – Differential Equations
Question
Solve the differential equation
1)
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
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
Equation of characteristics:
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
Then:
∫ d x x 2 = ∫ d y y 2 − 1 x = − 1 y + C 1 \int \frac {d x}{x ^ {2}} = \int \frac {d y}{y ^ {2}} - \frac {1}{x} = - \frac {1}{y} + C _ {1} ∫ x 2 d x = ∫ y 2 d y − x 1 = − y 1 + C 1 C 1 = x − y x y C _ {1} = \frac {x - y}{x y} C 1 = x y x − y y = x C 1 x + 1 y = \frac {x}{C _ {1} x + 1} y = C 1 x + 1 x d x x 2 = d z ( x + y ) z = d z ( x + x C 1 x + 1 ) z \frac {d x}{x ^ {2}} = \frac {d z}{(x + y) z} = \frac {d z}{\left(x + \frac {x}{C _ {1} x + 1}\right) z} x 2 d x = ( x + y ) z d z = ( x + C 1 x + 1 x ) z d z C 1 x 2 + 2 x x 2 ( C 1 x + 1 ) d x = C 1 x + 2 x ( C 1 x + 1 ) = d z z \frac {C _ {1} x ^ {2} + 2 x}{x ^ {2} (C _ {1} x + 1)} d x = \frac {C _ {1} x + 2}{x (C _ {1} x + 1)} = \frac {d z}{z} x 2 ( C 1 x + 1 ) C 1 x 2 + 2 x d x = x ( C 1 x + 1 ) C 1 x + 2 = z d z ∫ C 1 x + 2 x ( C 1 x + 1 ) d x = ∫ d z z \int \frac {C _ {1} x + 2}{x (C _ {1} x + 1)} d x = \int \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 ) = 1 x + 1 x ( C 1 x + 1 ) \frac {C _ {1} x + 2}{x \left(C _ {1} x + 1\right)} = \frac {1}{x} + \frac {1}{x \left(C _ {1} x + 1\right)} x ( C 1 x + 1 ) C 1 x + 2 = x 1 + x ( C 1 x + 1 ) 1 1 x ( C 1 x + 1 ) = A x + B C 1 x + 1 \frac {1}{x \left(C _ {1} x + 1\right)} = \frac {A}{x} + \frac {B}{C _ {1} x + 1} x ( C 1 x + 1 ) 1 = x A + C 1 x + 1 B A ( C 1 x + 1 ) + B x = 1 A \left(C _ {1} x + 1\right) + B x = 1 A ( C 1 x + 1 ) + B x = 1 A = 1 ; B = − C 1 A = 1; B = - C _ {1} A = 1 ; B = − C 1 1 x ( C 1 x + 1 ) = 1 x − C 1 C 1 x + 1 \frac {1}{x \left(C _ {1} x + 1\right)} = \frac {1}{x} - \frac {C _ {1}}{C _ {1} x + 1} x ( C 1 x + 1 ) 1 = x 1 − C 1 x + 1 C 1 ∫ ( 2 x − C 1 C 1 x + 1 ) d x = ∫ d z z \int \left(\frac {2}{x} - \frac {C _ {1}}{C _ {1} x + 1}\right) d x = \int \frac {d z}{z} ∫ ( x 2 − C 1 x + 1 C 1 ) d x = ∫ z d z 2 ln ∣ x ∣ − ln ∣ C 1 x + 1 ∣ = ln ∣ z ∣ + ln C 2 2 \ln | x | - \ln | C _ {1} x + 1 | = \ln | z | + \ln C _ {2} 2 ln ∣ x ∣ − ln ∣ C 1 x + 1∣ = ln ∣ z ∣ + ln C 2 C 2 = x 2 z ( C 1 x + 1 ) = x 2 z ( x − y x y x + 1 ) = y x 2 z x = x y z C _ {2} = \frac {x ^ {2}}{z \left(C _ {1} x + 1\right)} = \frac {x ^ {2}}{z \left(\frac {x - y}{x y} x + 1\right)} = \frac {y x ^ {2}}{z x} = \frac {x y}{z} C 2 = z ( C 1 x + 1 ) x 2 = z ( x y x − y x + 1 ) x 2 = z x y x 2 = z x y
Answer: F ( x − y x y , x y z ) = 0 F\left(\frac{x - y}{xy}, \frac{xy}{z}\right) = 0 F ( x y x − y , z x y ) = 0
Question
2)
p 1 / 2 − q 1 / 2 + 3 x = 0 p ^ {1 / 2} - q ^ {1 / 2} + 3 x = 0 p 1/2 − q 1/2 + 3 x = 0 Solution
( ∂ z ∂ x ) 1 / 2 − ( ∂ z ∂ y ) 1 / 2 + 3 x = 0 \left(\frac {\partial z}{\partial x}\right) ^ {1 / 2} - \left(\frac {\partial z}{\partial y}\right) ^ {1 / 2} + 3 x = 0 ( ∂ x ∂ z ) 1/2 − ( ∂ y ∂ z ) 1/2 + 3 x = 0
Equations of characteristics:
x ˙ = d x d τ = 1 2 p ; y ˙ = d y d τ = − 1 2 q ; p ˙ = d p d τ = − 3 ; q ˙ = d q d τ = 0 ; z ˙ = d z d τ = p − q 2 \dot {x} = \frac {d x}{d \tau} = \frac {1}{2 \sqrt {p}}; \dot {y} = \frac {d y}{d \tau} = - \frac {1}{2 \sqrt {q}}; \dot {p} = \frac {d p}{d \tau} = - 3; \dot {q} = \frac {d q}{d \tau} = 0; \dot {z} = \frac {d z}{d \tau} = \frac {\sqrt {p} - \sqrt {q}}{2} x ˙ = d τ d x = 2 p 1 ; y ˙ = d τ d y = − 2 q 1 ; p ˙ = d τ d p = − 3 ; q ˙ = d τ d q = 0 ; z ˙ = d τ d z = 2 p − q
Then:
p = − 3 ∫ d τ = − 3 τ + C 1 p = -3 \int d\tau = -3\tau + C_1 p = − 3 ∫ d τ = − 3 τ + C 1 q = C 2 q = C_2 q = C 2 y = − ∫ d τ 2 q = − τ 2 q + C 3 = − τ 2 C 2 + C 3 y = -\int \frac{d\tau}{2\sqrt{q}} = -\frac{\tau}{2\sqrt{q}} + C_3 = -\frac{\tau}{2\sqrt{C_2}} + C_3 y = − ∫ 2 q d τ = − 2 q τ + C 3 = − 2 C 2 τ + C 3 x = ∫ d τ 2 p = ∫ d τ 2 3 τ + C 1 = − 1 6 3 τ + C 1 + C 4 x = \int \frac{d\tau}{2\sqrt{p}} = \int \frac{d\tau}{2\sqrt{3\tau + C_1}} = -\frac{1}{6}\sqrt{3\tau + C_1} + C_4 x = ∫ 2 p d τ = ∫ 2 3 τ + C 1 d τ = − 6 1 3 τ + C 1 + C 4 z = ∫ p − q 2 d τ = ∫ 3 τ + C 1 − C 2 2 d τ = − 1 9 ( − 3 τ + C 1 ) 3 / 2 − 1 2 τ C 2 + C 5 z = \int \frac{\sqrt{p} - \sqrt{q}}{2} d\tau = \int \frac{\sqrt{3\tau + C_1} - \sqrt{C_2}}{2} d\tau = -\frac{1}{9}(-3\tau + C_1)^{3/2} - \frac{1}{2}\tau\sqrt{C_2} + C_5 z = ∫ 2 p − q d τ = ∫ 2 3 τ + C 1 − C 2 d τ = − 9 1 ( − 3 τ + C 1 ) 3/2 − 2 1 τ C 2 + C 5 3 τ + C 1 = 6 ( C 4 − x ) ; τ = 2 C 2 ( C 3 − y ) \sqrt{3\tau + C_1} = 6(C_4 - x) \quad ; \quad \tau = 2\sqrt{C_2}(C_3 - y) 3 τ + C 1 = 6 ( C 4 − x ) ; τ = 2 C 2 ( C 3 − y ) z = − 24 ( C 4 − x ) 3 − C 2 ( C 3 − y ) + C 5 z = -24(C_4 - x)^3 - C_2(C_3 - y) + C_5 z = − 24 ( C 4 − x ) 3 − C 2 ( C 3 − y ) + C 5
Answer: z = 24 ( x − c 1 ) 3 + c 2 y + c 3 z = 24(x - c_1)^3 + c_2y + c_3 z = 24 ( x − c 1 ) 3 + c 2 y + c 3 ; c 2 = q c_2 = q c 2 = q .
Reference:
E. A. Kuznetsov, D. A. Shapiro, Methods of Mathematical Physics, Part I, Chapter 2, 2011.
Answer provided by https://www.AssignmentExpert.com