Why is E proportional to q/R^3 inside a uniformly charged sphere?

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SUMMARY

Inside a uniformly charged sphere, the electric field \bold{E} is defined as \bold{E} = \frac{1}{4 \pi \epsilon_{0}} \frac{q}{R^3} r \bold{\hat{r}}. This relationship is derived using Gauss's Law, which states that the charge enclosed (Q') within a Gaussian surface is proportional to the volume ratio of the inner sphere to the outer sphere. Specifically, Q' is calculated as Q' = Q\frac{r^3}{R^3}, where Q is the total charge and R is the radius of the outer sphere.

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In a uniformly charged sphere, why inside the sphere is [tex]\bold{E} = \frac{1}{4 \pi \epsilon_{0}} \frac{q}{R^3} r \bold{\hat{r}}[/tex]?

I don't see how this follows from Gauss's law.
 
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The ratio of the charges between the inner sphere (Q') and the outer sphere (Q) is equal to the ratio of the volume between the inner and outer spheres.

[tex]\frac{\frac{4}{3}\pi r^3}{\frac{4}{3}\pi R^3}=\frac{Q'}{Q}[/tex]

Thus: [tex]Q' = Q\frac{r^3}{R^3}[/tex]

Now use Gauss's Law to find the electric field inside the inner sphere.
 
Just to clarify what Snazzy said, the inner sphere is your Gaussian Surface.
 

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