SUMMARY
The discussion focuses on determining the electric field inside and outside a polarized sphere with a polarization defined as \(\vec{P} = k\vec{r}\). It is established that the electric field outside the sphere is zero due to the cancellation of polarization charges. Inside the sphere, the electric field cannot be assumed to be \(-\frac{1}{3\epsilon_0} \vec{P}\) because the polarization is not uniform. Instead, the bound charge density \(\rho_b = -\vec{\nabla} \cdot \vec{P}\) must be calculated, and Gauss' law should be applied to find the electric field as a function of the radial distance \(r\).
PREREQUISITES
- Understanding of electric polarization and bound charge density
- Familiarity with Gauss' law in electrostatics
- Knowledge of vector calculus, specifically divergence
- Basic concepts of electric fields in dielectric materials
NEXT STEPS
- Calculate the bound charge density \(\rho_b\) for the given polarization \(\vec{P} = k\vec{r}\)
- Apply Gauss' law to derive the electric field \(E(r)\) inside the polarized sphere
- Explore the implications of non-uniform polarization on electric fields
- Study the behavior of electric fields in uniformly polarized spheres for comparison
USEFUL FOR
Students and professionals in physics, particularly those studying electromagnetism, as well as educators seeking to clarify concepts related to electric fields in polarized materials.