
Let's first explore the
way the density and velocity change as a function of radius. Assume that
the spray sets up a steady state of outgoing flow so that the fields
describing the fluid density and velocity are independent of time and angle.
So they are just a function of radius, ρ(r) and v(r).
(a) Rewrite the mass conservation theorem
as an integral equation by integrating both sides and applying a vector fundamental theorem of calculus to the side with the gradient operator to get rid of it. (b) Assume that the velocity is constant. If we are ignoring gravity, this is reasonable. What would slow the bits of fluid down? If they are all emitted with the same speed, they should keep the same speed. So we assume v(r) = v_{0} independent of r. Show what this implies for the density as a function of radius by applying your result from part (a) to the volume consisting of a small angular wedge stretching from a distance r_{1} to a distance r_{2} as shown in the figure at the right below.
 
(c) Write a general
theorem analogous to Gauss's law of electrostatics for this fluid. What
is your analog of the "charge" in this case? (Hint: Consider the value
of the integral over the full sphere for the case in part (b) and consider
how it changes with radius. What does this integral mean physically?)
(d) If the density of the fluid had to stay constant, what would your integral theorem imply for the velocity as a function of radius?  . 
Last revision 5. December, 2004.