Math Problem Statement

Obtain the solution of the wave equation ∂²u/∂t² = 4 ∂²u/∂x² with initial conditions u(x,0) = 0 and u_t(x,0) = x

Solution

The problem presented involves solving the wave equation:

2ut2=42ux2,x(,),t>0\frac{\partial^2 u}{\partial t^2} = 4 \frac{\partial^2 u}{\partial x^2}, \quad x \in (-\infty, \infty), \quad t > 0 with the initial conditions: u(x,0)=0,ut(x,0)=xu(x, 0) = 0, \quad u_t(x, 0) = x

This is a classic second-order linear partial differential equation (PDE), often known as the 1-dimensional wave equation. The factor of 4 on the right-hand side implies a wave speed of c=2c = 2, as the general form of the wave equation is:

2ut2=c22ux2\frac{\partial^2 u}{\partial t^2} = c^2 \frac{\partial^2 u}{\partial x^2}

Solution Approach

The solution to the wave equation can be found using d'Alembert's formula for the general solution of the 1D wave equation. For c=2c = 2, d'Alembert's solution is:

u(x,t)=f(x2t)+g(x+2t)u(x, t) = f(x - 2t) + g(x + 2t) where ff and gg are functions to be determined from the initial conditions.

Step 1: Apply the first initial condition u(x,0)=0u(x, 0) = 0

This gives: u(x,0)=f(x)+g(x)=0f(x)=g(x)u(x, 0) = f(x) + g(x) = 0 \quad \Rightarrow \quad f(x) = -g(x)

Step 2: Apply the second initial condition ut(x,0)=xu_t(x, 0) = x

The time derivative of the solution is: ut(x,t)=2f(x2t)+2g(x+2t)u_t(x, t) = -2 f'(x - 2t) + 2 g'(x + 2t) At t=0t = 0, this becomes: ut(x,0)=2f(x)+2g(x)=xu_t(x, 0) = -2 f'(x) + 2 g'(x) = x Using f(x)=g(x)f'(x) = -g'(x), we substitute: 2f(x)+2(f(x))=x4f(x)=x-2 f'(x) + 2 (-f'(x)) = x \quad \Rightarrow \quad -4 f'(x) = x Thus, we solve for f(x)f'(x): f(x)=x4f'(x) = -\frac{x}{4} Integrating this gives: f(x)=x28+Cf(x) = -\frac{x^2}{8} + C Since f(x)=g(x)f(x) = -g(x), we also have g(x)=x28Cg(x) = \frac{x^2}{8} - C.

Step 3: Form the general solution

The general solution is: u(x,t)=f(x2t)+g(x+2t)u(x, t) = f(x - 2t) + g(x + 2t) Substituting for ff and gg: u(x,t)=((x2t)28+C)+((x+2t)28C)u(x, t) = \left( -\frac{(x - 2t)^2}{8} + C \right) + \left( \frac{(x + 2t)^2}{8} - C \right) Simplifying: u(x,t)=(x+2t)2(x2t)28u(x, t) = \frac{(x + 2t)^2 - (x - 2t)^2}{8} This expression simplifies further using the difference of squares: u(x,t)=(x2+4xt+4t2)(x24xt+4t2)8=8xt8=xtu(x, t) = \frac{(x^2 + 4xt + 4t^2) - (x^2 - 4xt + 4t^2)}{8} = \frac{8xt}{8} = xt

Final Solution

Thus, the solution to the wave equation is: u(x,t)=xtu(x, t) = xt

Would you like any further clarifications or additional details on this solution?

Related Questions:

  1. How is the wave speed cc derived from the wave equation?
  2. What is d'Alembert's formula, and how is it used to solve wave equations?
  3. How do the initial conditions influence the solution of a PDE?
  4. Can this method of solving the wave equation be extended to higher dimensions?
  5. How would the solution change if different initial conditions were applied?

Tip:

For wave equations, always check for symmetry in the initial conditions, as it can simplify finding f(x)f(x) and g(x)g(x) in d'Alembert's solution.

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Math Problem Analysis

Mathematical Concepts

Partial Differential Equations
Wave Equation
D'Alembert's Solution

Formulas

∂²u/∂t² = 4 ∂²u/∂x²
D'Alembert's formula: u(x, t) = f(x - 2t) + g(x + 2t)
f'(x) = -x/4

Theorems

D'Alembert's solution for the wave equation

Suitable Grade Level

Undergraduate Level (Mathematics or Physics)