Fluid Mechanics equations in Cartesian and Cylindrical coordinates?

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silentwf
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Homework Statement


Not really a homework question, but more of a concept question which I'm unfamiliar with. So as we know, equations can be in any coordinate, but how do you convert them from one to another?
For example, a few equations from fluid mechanics. the first equation is the vector form of equation 2 and 3. i don't get why there's an extra 1/r. the same goes for equations 4 and 5. 4 is in cartesian while 5 is in cylindrical.

(let u,v,w be velocities. u is a function of x, v is a function of y and w is a function of z; v(theta) is velocity, function of theta, v(r) velocity, function of r)
(typo in equation 4, it should be partial u and not partial mu)

http://img341.imageshack.us/img341/8350/fluid.png


Homework Equations



(none, i guess?)

The Attempt at a Solution


(dont know where to begin)
 
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By the chain rule, as hunt mat suggests, for any function, u, of x and y,
[tex]\frac{\partial u}{\partial x}= \frac{\partial u}{\partial r}\frac{\partial r}{\partial x}+ \frac{\partial u}{\partial \theta}\frac{\partial \theta}{\partial x}[/tex]

[itex]r= (x^2+ y^2)^{1/2}[/itex] so
[tex]\frac{\partial r}{\partial x}= (1/2)(x^2+ y^2)^{1/2}(2x)= \frac{x}{(x^2+ y^2)^{1/2}}= \frac{r cos(\theta)}{r}= cos(\theta)[/tex]

[itex]\theta= arctan(y/x)[/itex] so
[tex]\frac{\partial \theta}{\partial x}= \frac{1}{1+ \frac{y^2}{x^2}}\left(-\frac{y}{x^2}\right)= -\frac{y}{x^2+ y^2}= -\frac{r sin(\theta)}{r^2}= -\frac{1}{r} sin(\theta)[/tex]

So that
[tex]\frac{\partial u}{\partial x}= cos(\theta)\frac{\partial u}{\partial r}- \frac{1}{r}sin(\theta)\frac{\partial u}{\partial \theta}[/tex]
 
OH! ok, I was wondering how to do it for a while.
Sorry for the late response! and thanks guys!