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Next: Computational part Up: Homework 1 Previous: Prerequisites

Theoretical part

You can either write your answers on paper or edit them in the file hw1/paper.tex. Please show all the mathematical derivations that you perform.

  1. In class, we used a mysterious parameter $\sigma$ to represent a variable continuously increasing along a ray. There are other variables that can play a similar role.
    1. Transform the isotropic ray tracing system
      $\displaystyle \frac{d \mathbf{x}}{d \sigma}$ $\textstyle =$ $\displaystyle \mathbf{p}$ (1)
      $\displaystyle \frac{d \mathbf{p}}{d \sigma}$ $\textstyle =$ $\displaystyle S(\mathbf{x})\,\nabla S$ (2)
      $\displaystyle \frac{d T}{d \sigma}$ $\textstyle =$ $\displaystyle S^2(\mathbf{x})$ (3)

      into an equivalent system that uses $\lambda$ instead of $\sigma$, where $\lambda$ represents the length of the ray trajectory:
      $\displaystyle \frac{d \mathbf{x}}{d \lambda}$ $\textstyle =$   (4)
      $\displaystyle \frac{d \mathbf{p}}{d \lambda}$ $\textstyle =$   (5)
      $\displaystyle \frac{d T}{d \lambda}$ $\textstyle =$ $\displaystyle S(\mathbf{x})\;.$ (6)

      Remember to check physical dimensions.
    2. Suppose you are given $T(\mathbf{x})$ - the traveltime from the source to all points $\mathbf{x}$ in the domain of interest. Your task is to find $\lambda(\mathbf{x})$ - the length of the ray trajectory at all $\mathbf{x}$. Derive a first-order partial differential equation that connects $\nabla \lambda$ and $\nabla T$.

  2. The elliptically anisotropic 2-D eikonal equation has the form
    \begin{displaymath}
V_1^2(\mathbf{x})\,\left(\frac{\partial T}{\partial x_1}\...
...bf{x})\,\left(\frac{\partial T}{\partial x_2}\right)^2 = 1\;,
\end{displaymath} (7)

    where $\mathbf{x}=\{x_1,x_2\}$ is a point in space, $T(\mathbf{x})$ is the traveltime, $V_1(\mathbf{x})$ is the horizontal velocity, and $V_2(\mathbf{x})$ is the vertical velocity.
    1. Derive the ray tracing system
      $\displaystyle \frac{d x_1}{d T}$ $\textstyle =$ $\displaystyle \hspace{5in}$ (8)
      $\displaystyle \frac{d x_2}{d T}$ $\textstyle =$   (9)
      $\displaystyle \frac{d p_1}{d T}$ $\textstyle =$   (10)
      $\displaystyle \frac{d p_2}{d T}$ $\textstyle =$   (11)

      where $p_1$ represents $\partial T/\partial x_1$ and $p_2$ represents $\partial T/\partial x_2$.
    2. Assuming constant (but unequal) velocities $V_1$ and $V_2$, solve the ray tracing system for a point source at the origin $x_1(0)=0$, $x_2(0)=0$ to show that the wavefronts in this case have an elliptical shape.
    3. The isotropic eikonal equation
      \begin{displaymath}
\left(\frac{\partial T}{\partial x_1}\right)^2 +
\left(\frac{\partial T}{\partial x_2}\right)^2 = S^2(\mathbf{x})
\end{displaymath} (12)

      describes wavefronts of the wave equation
      \begin{displaymath}
S^2(\mathbf{x})\,\frac{\partial^2 P}{\partial t^2} =
\nabla^2 P + \cdots
\end{displaymath} (13)

      with omitted possible first- and zero-order terms. equation (7)? What wave equation corresponds to equation (7)?
      \begin{displaymath}
{\frac{\partial^2 P}{\partial t^2}} =
\end{displaymath} (14)


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Next: Computational part Up: Homework 1 Previous: Prerequisites

2008-03-02