# Ecuación del rayo

Series | Geophysical References Series |
---|---|

Title | Digital Imaging and Deconvolution: The ABCs of Seismic Exploration and Processing |

Author | Enders A. Robinson and Sven Treitel |

Chapter | 2 |

DOI | http://dx.doi.org/10.1190/1.9781560801610 |

ISBN | 9781560801481 |

Store | SEG Online Store |

We need to understand how a single ray moving along a particular path - say, a seismic ray - can know what is an extremal path in the variational sense. To illustrate the problem, consider a seismic wave traveling through a medium whose slowness *n* increases in the direction of travel. Because the raypath is parallel to the gradient of the slowness, it undergoes no bending. However, if the contour lines of slowness are at an angle to the ray, then the ray will bend, even though the slowness at each point along the path is identical to what it was before when there was no bending. This shows that a ray’s path cannot be explained solely in terms of the value of the slowness on that path. We also must consider the slowness along neighboring paths - hat is, along paths not taken.

The classical wave explanation, proposed by Huygens, resolves this problem by saying that light does not propagate in the form of a single ray. According to the wave interpretation, light propagates as a wavefront possessing transverse width. If a small section of a propagating wavefront encounters the same value of slowness along its width, then the ray will not bend. If a small section of a propagating wavefront encounters different values of slowness along its width, then the ray will bend. The amount of bending depends on the gradient of the slowness. The wavefront propagates more rapidly on the side where the slowness is low (i.e., where the velocity is high) than it does on the side where the slowness is high. As a result, the wavefront naturally turns in the direction of increasing slowness.

In this section, the *position vector* **r** always represents a point on a specific raypath and not any arbitrary point in space. As time increases, **r** traces out the particular raypath in question. The seismic ray at any given point follows the direction of the gradient of the traveltime field . As before, let **u** be the unit vector along the ray. The ray in general will follow a curved path, and the *raypath vector* will be tangent to this curved raypath.

Let us derive the *ray equation*. This equation tells us how the raypath vector changes along the curved raypath. The equation for the unit tangent vector is

**(**)

We also know that

**(**)

Thus, the unit tangent vector **u** is

**(**)

The slowness is a scalar function that depends on coordinates *x* and *y*. However, we can hold *y* constant and consider the curve that gives the variation of slowness with *x* alone. The slope of this curve is called the partial derivative of slowness with respect to *x*. The partial derivative is defined similarly. The gradient of the slowness surface is the vector with these partial derivatives as components; that is,

**(**)

We know that the gradient of the traveltime is

**(**)

We recall eikonal equation **14**. Now we will do the mathematics. We take the derivative of the eikonal equation with respect to path length *s*. We obtain

**(**)

On the right side, we interchange the two operations to obtain

**(**)

We recognize as the slowness *n*. Thus, the right side of equation **23** is the gradient of the slowness, so we can write

**(**)

If we put together the above equations, we obtain the ray equation

**(**)

Ray equation **25** says that the rate of change of the raypath vector is equal to the gradient of the slowness. We know that eikonal equation **14** says that the raypath vector is a flow line on the traveltime surface. The ray equation says that the rate of change of the ray-path vector is a flow line on the slowness surface.

## Sigue leyendo

Sección previa | Siguiente sección |
---|---|

Ley de Snell | Ecuacón del rayo para velocidad lineal con la profundidad |

Capítulo previo | Siguiente capítulo |

Movimiento de ondas | Visualización |

## También en este capítulo

- Sismología de Reflexión
- Procesamiento digitales
- Realce de señales
- Migración
- Interpretación
- Rayos
- Vector unitario tangente
- Tiempo de viaje
- El gradiente
- La derivada direccional
- El principio de tiempo mínimo
- La ecuación de Eikonal
- Ley de Snell
- Ecuacón del rayo para velocidad lineal con la profundidad
- Camino del rayo para velocidad lineal con la profundidad
- Tiempo de viaje para velocidad lineal con la profundidad
- Punto de máxima profundidad
- Frente de onda para velocidad lineal con la profundidad
- Dos conjuntos ortogonales de círculos
- Migración en el caso de velocidad constante
- Implementación de la migración
- Apéndice B: Ejercicios