It's a generalization of the derivative operator to multiple dimensions. That's all.
In one dimension, say along the x-axis, the derivative operator looks like this:
<br />
\frac{d}<br />
{{dx}} = \frac{\partial }<br />
{{\partial x}} = \vec i \frac{\partial }<br />
{{\partial x}}<br />
Since there's only one dimension, the "normal" derivative and partial derivative are the same. Also, there's only way way to take a derivative in one dimension -- along that dimension. Thus, the \vec i[/tex] is implied.<br />
<br />
In multiple dimensions, say x, y and z, it looks like:<br />
<br />
<br />
\nabla = <br />
\vec i \frac{\partial }<br />
{{\partial x}} + \vec j \frac{\partial }<br />
{{\partial y}} + \vec k \frac{\partial }<br />
{{\partial z}}<br /><br />
<br />
Same thing, just with more dimensions.<br />
<br />
- Warren