Consider a sphere of radius R which carries a
uniform charge density $\rho . If a sphere of radius {{R \over 2}} is carved out of it, as shown, the ratio {{\left| {\overrightarrow {{E_A}} } \right|} \over {\left| {\overrightarrow {{E_B}} } \right|}} of magnitude of electric field {\overrightarrow {{E_A}} } and {\overrightarrow {{E_B}} }$,
respectively, at points A and B due to the
remaining portion is :