Difference between revisions of "Forest UCM Energy CurlFcons"

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Stokes theorem related the line integral of a vecotr field over its boundary
 
Stokes theorem related the line integral of a vecotr field over its boundary
  
:<math>\int \vec F \cdot d \vec r</math>
+
:<math>\oint \vec F \cdot d \vec r</math>
  
 
to the surface integral of the curl of the vector field over a surface
 
to the surface integral of the curl of the vector field over a surface
  
:<math>\dint \ve \nabla \times \vec F dA</math>
+
:<math>\iint \ve \nabla \times \vec F dA</math>
  
  
 
[[Forest_UCM_Energy#Second_requirement_for_Conservative_Force]]
 
[[Forest_UCM_Energy#Second_requirement_for_Conservative_Force]]

Revision as of 02:41, 24 September 2014

A force with a curl of zero is a conservative force.

Thus taking the curl of the force is an easier way to test for conservative forces rather than calculating the work and inspecting to see if it only depends on the endpoints of the motion.

Definition of curl

We have seen that the gradient operator is defined in cartesian coordinates as

[math]\vec \nabla = \frac{\partial}{\partial x} \hat i +\frac{\partial}{\partial y} \hat j +\frac{\partial}{\partial z} \hat k[/math]

can be used to find the function form of a conservative force given its potential energy

Stokes Theorem

Stokes theorem related the line integral of a vecotr field over its boundary

[math]\oint \vec F \cdot d \vec r[/math]

to the surface integral of the curl of the vector field over a surface

[math]\iint \ve \nabla \times \vec F dA[/math]


Forest_UCM_Energy#Second_requirement_for_Conservative_Force