Changes

Jump to navigation Jump to search
712 bytes added ,  02:20, July 11, 2009
no edit summary
Line 1: Line 1:  +
{{math-h}}
 
The '''curl''' is a way of expressing a certain type of [[derivative]] of a [[vector field]].  It is defined for fields of 3-dimensional vectors on 3-dimensional space.  The curl of a vector field is another vector field.
 
The '''curl''' is a way of expressing a certain type of [[derivative]] of a [[vector field]].  It is defined for fields of 3-dimensional vectors on 3-dimensional space.  The curl of a vector field is another vector field.
   −
The curl is written as though it were the [[cross product]] of the special symbol "<math>\nabla</math>" (which is commonly called "del" or "nabla"), with the given vector field, like this: <math>\nabla \times \vec V</math>This is usually pronounced "curl V" or "del cross V".
+
More precisely, it is defined<ref>[http://mathworld.wolfram.com/Curl.html Curl] at Wolfram Mathworld</ref> as the limiting value of rotation per unit areaWritten explicitly,
   −
In ordinary [[Cartesian coordinates]], the curl is calculated as:
+
:<math>(\nabla \times \mathbf{F}) \cdot \mathbf{\hat{n}} \equiv \lim_{A \to 0} \frac{\oint_{C} \mathbf{F} \cdot d\mathbf{s}}{A}</math>
 +
 
 +
where <math>\mathbf{\hat{n}}</math> is the unit [[normal vector]] of the area element A and C is the boundary of the area element (<math>C =\partial A</math>).  The right side of the definition is a path integral along the boundary of the area element A, which is allow to shrink in the limiting process.
 +
 
 +
==Cartesian coordinates==
 +
In [[Cartesian coordinates]], the curl is written as though it were the [[cross product]] of the special symbol "<math>\nabla</math>" (which is commonly called "del" or "nabla"), with the given vector field, like this: <math>\nabla \times \vec V</math>.  This is usually pronounced "curl V" or "del cross V".
 +
 
 +
 
 +
 
 +
In 3-D [[Cartesian coordinates]], the curl is calculated as:
    
:<math>\nabla \times \vec V = (\ \ \frac{\partial V_z}{\partial y} - \frac{\partial V_y}{\partial z},\ \ \ \ \frac{\partial V_x}{\partial z} - \frac{\partial V_z}{\partial x},\ \ \ \ \frac{\partial V_y}{\partial x} - \frac{\partial V_x}{\partial y}\ \ )</math>
 
:<math>\nabla \times \vec V = (\ \ \frac{\partial V_z}{\partial y} - \frac{\partial V_y}{\partial z},\ \ \ \ \frac{\partial V_x}{\partial z} - \frac{\partial V_z}{\partial x},\ \ \ \ \frac{\partial V_y}{\partial x} - \frac{\partial V_x}{\partial y}\ \ )</math>
Line 26: Line 36:     
Vector fields with a curl of zero are called ''irrotational''.
 
Vector fields with a curl of zero are called ''irrotational''.
 +
 +
==References==
 +
{{reflist}}
    
[[Category:Calculus]]
 
[[Category:Calculus]]
 
[[Category:Physics]]
 
[[Category:Physics]]
20

edits

Navigation menu