This isn't quite right either.
pmb_phy said:
No. It isn't. Its
[tex]\bar{\Phi} =\frac{1}{A}\int d\Phi[/tex]
where A is the area of the sphere.
Pete
It isn't clear what you mean by [itex]\int d\Phi[/itex]
since usually the integral of an exact differential
is just the function evaluated at the endpoints.
Or alternatively
[tex]\int d\Phi = \int \frac{\partial \Phi}{\partial x} dx +<br />
\int \frac{\partial \Phi}{\partial y} dy +<br />
\int \frac{\partial \Phi}{\partial z} dz[/tex]
which is, of course, a line integral (which isn't what we
want).
dextercobi said:
[tex]\bar{\Phi} =\frac{1}{4\pi R}\int \Phi \ dA[/tex]
This doesn't have the right dimensions. On the left
we have dimensions of [Phi]; and on the right we have
dimensions of [Phi]x[Area]/[Length].
I propose another formula:
[tex]
\bar{\Phi} = \frac{1}{4 \pi R^2} \int_A \Phi dA [/tex]
This also has the advantage that if Phi is constant
on the sphere we have
[tex]
\bar{\Phi} = \frac{1}{4 \pi R^2} \int_A \Phi dA = <br />
\frac{1}{4 \pi R^2} \Phi \int_A dA = <br />
\frac{1}{4 \pi R^2} \Phi ( 4 \pi R^2 ) =<br />
\Phi[/tex]