This quantity, squared, is multiplied by three k squared in a rewriting of the Bohm-Gross DispersionRelation. When cubed and multiplied by four pi n, it gives a parameter that is greater than one forweakly-coupled materials and less for strongly-coupled ones. A formula for this quantity can bederived by solving Poisson's equation for phi after imagining a small (*) point charge affecting anequilibrium electron distribution. This quantity, which is proportional to the square root of absolutetemperature over the electron density, gives the charac
This quantity, squared, is multiplied by three k squared in a rewriting of the Bohm-Gross DispersionRelation. When cubed and multiplied by four pi n, it gives a parameter that is greater than one forweakly-coupled materials and less for strongly-coupled ones. A formula for this quantity can bederived by solving Poisson's equation for phi after imagining a small (*) point charge affecting anequilibrium electron distribution. This quantity, which is proportional to the square root of absolutetemperature over the electron density, gives the characteristic thickness of a double layer and arisesfrom the fact that opposite charges shield each other. For 10 points, name this characteristic lengthimportant in plasma physics.
This quantity, squared, is multiplied by three k squared in a rewriting of the Bohm-Gross DispersionRelation.
Debye length