In Griffiths' book, Introduction to Electrodynamics 3rd, problem 4.3,it requires me to find the condition on ρ(r) such that equation $p = αE$ will hold in the weak-field limit. The answer gives $ρ(r)=Ar$, and i don't understand why, either that it requires $p$ is proportional to $E$ while the answer gives $E^{1/2}$,is it because of the weak-field limit? And why the answer requires $E$ to be proportional to $r$ and $ρ$ to be zero at the origin?
$$p=αE \tag{4.1}\label{}$$ α means atomic polarization
Question: Problem 4.3 According to Eq. 4.1, the induced dipole moment of an atom is proportional to the external field. This is a"rule of thumb not a fundamental law, and it is easy to concoct exceptions--in theory. Suppose, for example, the charge density of the electron cloud were proportional to the distance from the center, out to a radius $R$. To what power of E would p be proportional in that case? Find the condition on ρ(r) such that Eq. 4.1 will hold in the weak-field limit
Answer: ρ(r)=Ar. Electric field( by Gauss's Law:$$∮E·da=E(4πr²)=Q/(ε₀),or E=(Ar²)/(4ε₀)$$ This “internal” field balances the external field $E$ when nucleus is “off-center” an amount $$d:(ad²)/(4ε₀)=E⇨d={\sqrt {(4ε₀E)/A}}$$So the induced dipole moment is $$p= ed= 2e·{\sqrt {ε₀/A}}E^{1/2}$$ Evidently p is proportional to $E^{1/2}$. For Eq. 4.1 to hold in the weak-field limit, E must be proportional to r, for small r, which means that ρ must go to a constant(not zero)at the origin:ρ(0)≠0(nor infinite)