mgb_phys said:
The drag equation ( propertional Area * velocity^2) is an approximation for high Reynolds number flow (eg air) it isn't necessarily correct for low speed or high viscosity cases.
The drag coefficient is quite a function of Reynolds, and potentially other factors. Man, I must be in a good mood today. Let's see what I can find. For REALLY low Reynolds numbers, (Re < 1), we have
[tex]C_f = \frac{24}{R^*} \left( 1 + \frac{3}{16}R^* - \frac{7k}{48}R^* \right)\,\,R^*=2R[/tex]
Not sure why it's written like that, but oh well. [tex]R\equiv[/tex] Reynolds number of course. [tex]k = V^* / U_\infty[/tex] where V* is the radial velocity of blowing through the surface...which I assume you can take to be zero in your case.
There is also a "famous" Oseen's (1910) drag coefficient forumula for a sphere in uniform stream:
[tex]C_D = \frac{24}{{Re}_D}\left(1+\frac{3}{16}{Re}_D\right)[/tex]
Stokes gave an exact solution in the limit as Re->0, such as creeping flow, where:
[tex]C_D = \frac{24}{{Re}_D}[/tex]
However, that's only valid where Reynolds is less than 0.2.
What type of Reynolds are you looking at?