Math Problem Statement

Use the method of characteristics to find the general solution for 𝑒(π‘₯, 𝑦, 𝑧) of 𝑒π‘₯ + 𝑒𝑦 + 𝑒𝑧 = 0. Find a particular solution which satisfies the auxiliary condition 𝑒(π‘₯,𝑦,0)=π‘₯2 +𝑦2.

Solution

To solve the first-order partial differential equation (PDE) using the method of characteristics, let's first outline the problem:

We are given the PDE: ux+uy+uz=0u_x + u_y + u_z = 0 and we want to find the general solution u(x,y,z)u(x, y, z).

Step 1: Set up the characteristic equations

The method of characteristics involves converting the PDE into a system of ordinary differential equations (ODEs) along characteristic curves. The PDE can be written as: βˆ‚uβˆ‚x+βˆ‚uβˆ‚y+βˆ‚uβˆ‚z=0.\frac{\partial u}{\partial x} + \frac{\partial u}{\partial y} + \frac{\partial u}{\partial z} = 0. This gives the following system of characteristic equations: dxds=1,dyds=1,dzds=1.\frac{dx}{ds} = 1, \quad \frac{dy}{ds} = 1, \quad \frac{dz}{ds} = 1.

Step 2: Solve the characteristic system

From the equations dxds=1\frac{dx}{ds} = 1, dyds=1\frac{dy}{ds} = 1, and dzds=1\frac{dz}{ds} = 1, we can integrate to find: x=s+C1,y=s+C2,z=s+C3,x = s + C_1, \quad y = s + C_2, \quad z = s + C_3, where C1,C2,C3C_1, C_2, C_3 are constants of integration.

Now, subtracting these equations from each other to eliminate ss, we get: xβˆ’y=C1βˆ’C2=C,xβˆ’z=C1βˆ’C3=D,x - y = C_1 - C_2 = C, \quad x - z = C_1 - C_3 = D, where CC and DD are constants. Therefore, the general solution must be a function of these two constants: u(x,y,z)=f(xβˆ’y,xβˆ’z).u(x, y, z) = f(x - y, x - z). This is the general solution for the PDE.

Step 3: Apply the auxiliary condition

We are given the auxiliary condition: u(x,y,0)=x2+y2.u(x, y, 0) = x^2 + y^2. Substitute z=0z = 0 into the general solution u(x,y,z)=f(xβˆ’y,xβˆ’z)u(x, y, z) = f(x - y, x - z): u(x,y,0)=f(xβˆ’y,x)=x2+y2.u(x, y, 0) = f(x - y, x) = x^2 + y^2. Now we need to find f(ΞΎ1,ΞΎ2)f(\xi_1, \xi_2) such that: f(xβˆ’y,x)=x2+y2.f(x - y, x) = x^2 + y^2. Let’s assume f(ΞΎ1,ΞΎ2)=g(ΞΎ1)+h(ΞΎ2)f(\xi_1, \xi_2) = g(\xi_1) + h(\xi_2). This gives: g(xβˆ’y)+h(x)=x2+y2.g(x - y) + h(x) = x^2 + y^2. We can now separate variables. Since g(xβˆ’y)g(x - y) is a function of xβˆ’yx - y and h(x)h(x) is a function of xx, the only way to satisfy this equation is: g(xβˆ’y)=y2,h(x)=x2.g(x - y) = y^2, \quad h(x) = x^2. Thus, g(ΞΎ1)=ΞΎ12g(\xi_1) = \xi_1^2 and h(ΞΎ2)=ΞΎ22h(\xi_2) = \xi_2^2, giving: f(ΞΎ1,ΞΎ2)=ΞΎ12+ΞΎ22.f(\xi_1, \xi_2) = \xi_1^2 + \xi_2^2.

Step 4: Write the particular solution

Substitute ΞΎ1=xβˆ’y\xi_1 = x - y and ΞΎ2=xβˆ’z\xi_2 = x - z into the expression for f(ΞΎ1,ΞΎ2)f(\xi_1, \xi_2): u(x,y,z)=(xβˆ’y)2+(xβˆ’z)2.u(x, y, z) = (x - y)^2 + (x - z)^2. This is the particular solution to the PDE that satisfies the auxiliary condition u(x,y,0)=x2+y2u(x, y, 0) = x^2 + y^2.

Final Answer

The particular solution to the PDE ux+uy+uz=0u_x + u_y + u_z = 0 that satisfies u(x,y,0)=x2+y2u(x, y, 0) = x^2 + y^2 is: u(x,y,z)=(xβˆ’y)2+(xβˆ’z)2.u(x, y, z) = (x - y)^2 + (x - z)^2.

Would you like more details or explanations on any step?

Here are 5 related questions to explore:

  1. What is the geometric interpretation of characteristic curves in this context?
  2. How do you handle non-linear PDEs with the method of characteristics?
  3. Can the method of characteristics be used for second-order PDEs?
  4. How does the auxiliary condition affect the general solution?
  5. What happens if we change the auxiliary condition to something more complex?

Tip: Always double-check if the auxiliary condition is correctly applied to ensure consistency in solving PDEs using methods like characteristics.

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Math Problem Analysis

Mathematical Concepts

Partial Differential Equations (PDEs)
Method of Characteristics
First-Order PDEs
Auxiliary Conditions

Formulas

Characteristic Equations: dx/ds = 1, dy/ds = 1, dz/ds = 1
General Solution: u(x, y, z) = f(x - y, x - z)

Theorems

Method of Characteristics
Separation of Variables

Suitable Grade Level

Undergraduate