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J = [itex]\sigma[/itex]E

My question is about the validity of this statement (I know it is just an empirical law, but therefore you can still think of its consequences). If the above is true then the volume current density will depend on the strength of the field at a specific point. But how are you guarenteed that the field through our ohmic material will vary in such a way as to not violate charges being piled up. Let me make my point more clear through an example:

Suppose we have a thin rod through which the field varies like 1/r where r is the distance from the minus pole to a point on the rod. Close to the minus pole you will then have a current density going through a crosssection of the rod which is very large. But as you move away further the current density will according to Ohms law be much less. This is not physical since charge cannot disappear and why would it pile up in a conductor?