Flux through a nonconducting shell

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A particle of charge q is inside a nonconducting spherical shell of uniformly spread charge of Q. What is the flux through a spherical Gaussian surface concentric with the shell if the radius of this Gaussian surface is less than the shell's radius?

I know we can use the formula for Gauss' Law:
Flux = charge enclosed / Epsilon not.

However I am not sure specifically what the charge enclosed is. Certainly there is charge enclosed of size q, however is there not a portion of the Q charge enclosed since the Q is uniformly distributed?
 
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Sure, I could integrate to find that. However the answer appears to be that the only charge that contributes is the q, meaning that the answer is simply q/Epsilon not.
 
And hence the answer states that the charge Q does not play a role unless you are at a radius greater than or equal to R (where R = radius of entire charge distribution)
 
Yes, this is a homework problem that I have the book's answer to.
 
Quoted from the answer: "If the radius of the G-sphere is less than that of the shell then the only charge enclosed by the G-sphere is the charge of the particle"
 
I now see what the problem is. A shell has two radii, one larger than the other.
Let a = smaller radius and b = larger radius.

If your Gaussian surface has radius r < a, then the only charge enclosed is q.
If your Gaussian surface has radius a < r < b, then the charge enclosed is q plus a fraction of Q that depends on r.
If your Gaussian surface has radius r > b, then the charge enclosed is q + Q.
 
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Oh I understand. I assumed the "less than the shell's radius" was referring to the outer radius. The wording was a bit ambiguous. But yes, if it refers to the inner radius, this makes much more sense.