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If we suppose that we want to find the electric field at some point P. Let's consider a small volume element $ \Delta V_i$ , which contains an amount of charge $\Delta q_i$. The distance between charges within the volume element $\Delta V_i$ are much smaller than compared to $r$, the distance between $ \Delta V_i$ and $P$. So, the volume charge density $\rho(\vec r)$ as: $$\rho(\vec r)= \frac{dq}{dV}$$

This is the definition given for Volume Density Charge. Why is $\rho(\vec r)$ a function of $\vec r$ ?

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  • $\begingroup$ If I understand your question, it's because other volume elements are at a different distance from P, and the amount of charge could vary from point to point , so the charge density depends on r. $\endgroup$ Commented Feb 23, 2020 at 1:58
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    $\begingroup$ Why do you think it should not be? $\endgroup$ Commented Feb 23, 2020 at 4:28

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It becomes quite evident when you draw a figure and label the vectors involved. enter image description here

When we define the charge density $\rho$, what we are defining is $\rho(r’)$. And if you want to find field at point $P$, we can rewrite it as $\rho(r-R)$. Now you can see why it’ll depend on $r$.

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$\rho$ is dependent on r because it describes the charge density in all of space.

Looks like the author of this text is using r for two purposes. An parameter for $\rho$ and one to descripe a point P in reasonable distance to the charges.

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