Showing posts with label Potential Function. Show all posts
Showing posts with label Potential Function. Show all posts

Tuesday, August 21, 2012

Conservative Fields: Examples



In my previous post on the basic theory behind conservative vector fields, I described some of the mathematical properties these fields will have:

- A conservative field has no curl:    

- By extension, a vector of 3 components (Mi + Nj + Pk) can be checked for conservancy with a component test:

            

- A conservative field can be 'integrated' to find a potential function. Conversely, any gradient of a function is conservative: 

This is all good stuff, but I like to see visual examples whenever possible. When we're talking graphs of vector fields and functions in space, this is entirely possible! I'm going to go through some examples now, using the graphs to emphasize the math.

Sunday, August 19, 2012

Conservative Fields: Theory

Next stop: Vector Calculus!

To continue in the present direction--a discussion of Energy methods in Particle Dynamics--it’s necessary to take a quick stop over in mathematician territory. An unfriendly place, it is. Look alive.

The basic idea that will recur in this discussion is that, in certain types of vector fields, the net work done on an object moving from one point to another is independent of the path taken. This is called path-independence, and is a very important property of conservative fields