Why cant charge move in an insulator?

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SUMMARY

The discussion clarifies the fundamental differences between conductors and insulators, emphasizing that conductors have free electrons that can move in response to an external electric field, while insulators lack the necessary energy levels for electrons to transition from the valence band to the conduction band. The concept of energy bands is crucial, as it defines the energy gap that prevents electrons in insulators from becoming free. High voltages are required to overcome this energy gap, allowing electrons to escape from conductors, which leads to positive charge accumulation. The breakdown voltage is a critical factor in determining when an insulator can conduct electricity.

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  • Understanding of energy bands in solid-state physics
  • Knowledge of electric fields and their effects on charged particles
  • Familiarity with the concepts of valence and conduction bands
  • Basic principles of electron behavior in metals and insulators
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  • Research the concept of energy gaps in semiconductors and insulators
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  • Explore the role of cathodes in electron emission and their applications
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I am a bit confused about what actually makes something insulating. As far as I know a conductor has free electrons so when you put it in an external E-field these will move to terminate the external field thereby producing a currrent. But then I sat down and thought, why do charges pile up at the surface of a conductor in air?

Why don't they just continue through air. Surely air is almost empty space so why wouldn't they? My book say's it's because air insulates, so can someone tell me what insulative proterty that makes the charges unable to continue through air? or vacuum for that matter
 
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Well, I'll be not 100% accurate, but I suppose electrons in metals are not really free, but they are "shared" between adjacent atoms which have them in common on their external orbits.
So electrons are free must they must still belong to an atom.
To pull off electrons from metals, you need high voltages. Pieces of metals that emits electrons are called cathodes. You need E-fields of thousands of V/m, and if the cathode is hot is better. You may look how it works in the "old" CRT tubes.
 
hi aaaa202! :smile:

how can an electron leave the conductor?

that would make the conductor positively charged, and it would just attract the electron back again, a lot more strongly than the field is trying to pull it out

inside the conductor, the electron is attracted to various positive sites, and doesn't much mind which one it's nearest to … a small field will make it move from one to the next

but an insulator has no such sites for the electron to go to … the electric field would have to be extremely strong (the breakdown voltage for the insulator) to launch the electron through it
 
Energy Bands

Recall that the valence shell of an atom represents a band of energy levels and that the valence electrons are confined to that band. When an electron acquires enough additional energy, it can leave the valence shell, become a free electron, and exist in what is known as the conduction band.

The difference in energy between the valence band and the conduction band is called an
energy gap. This is the amount of energy that a valence electron must have in order to jump from the valence band to the conduction band. Once in the conduction band, the electron is free to move throughout the material and is not tied to any given atom.
http://img38.imageshack.us/img38/6591/bandsn.jpg
 
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The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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