Anton Lampa generalized this law for ellipsoidal inclusions, and inputs to it can be replaced with explicit material parameters via the Maxwell-Garnett formula. A modification for this function for dense fields is produced in Feynman's lectures, which states it as 3 times the quantity n squared minu
Anton Lampa generalized this law for ellipsoidal inclusions, and inputs to it can be replaced with explicit material parameters via the Maxwell-Garnett formula. A modification for this function for dense fields is produced in Feynman's lectures, which states it as 3 times the quantity n squared minus one over n squared plus two is equal to N times alpha. The aforementioned formula is multiplied by four pi over 3 in the context of refractivity, when it is known as the (*) Lorentz-Lorenz equation. The main dependent variable in this equation is equal to the dipole moment over the local electric field. For 10 points, name this doubly-eponymous equation that relates molecular polarizability to the dielectric constants of two different media.
Anton Lampa generalized this law for ellipsoidal inclusions, and inputs to it can be replaced with explicit material parameters via the Maxwell-Garnett formula.