Our understanding of the behaviour of electrons in glasses, liquids and non-crystalline materials generally is decades behind the detailed theory available for crystals such as silicon and germanium. This article describes the advances made in the past fifteen years. It includes the work of the Leningrad school on amorphous semiconductors, the reason why they cannot usually be doped, the concept of "variable-range" hopping and the Cohen−Fritzsche−Ovshinsky and other models for the conduction band, and the reason why glass can be transparent. A crucial experiment, that of two-dimensional conduction in an inversion layer at a Si/SiO2 interface, is described. Particular emphasis is given to concepts about which there is a disagreement and indeed controversy, such as the "mobility edge", the "minimum metallic conductivity" and the interpretation to be given to the ovonic threshold switch.
Glass has no free electrons to convey current.
Glass
electrons are transferred from glass to rubber
an insulator
When the electrons in molecules are unable to absorb the energy of incident photon, the photon continues along its path. This happens in the case of glass, even though glass is not 100 percent transparent, as some of the photon energy is absorbed by the glass electrons.
No the electrons are not free to move. This means that the electrical conductivity will be relatively low. -jk
the silk will rub of the electrons on the silk, leaving the glass positively charged
Glass is an insulator.
glass
glass
Yes, rubbing a silk cloth on glass cause electrons to move to the cloth. As a result, glass rod acquires positive charge and silk acquires negative charge.
Glass is an insulator, as it DOES NOT conduct current. It is a material which has no free electrons available to flow as electrical current. Conductors, like copper or aluminum, have free electrons, or electrons in the outer shells of their atoms that are easily knocked loose. These electrons flow from negative to positive when an electrical potential (voltage) is applied across the material. We call the flow of electrons "current".