Absence of an electron at a point creates a positive charge

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SUMMARY

The absence of an electron at a specific point creates a local positive charge due to the concept of "holes" in solid-state physics. When an electron is displaced, it results in a local deficiency of negative charge at its original position and a corresponding excess at its new location, maintaining global electrical neutrality. This phenomenon can be better understood through band theory, which provides a more accurate model than the simplistic view of electrons as discrete particles. The movement of holes can be likened to peas on a wire grill, where the absence of one allows adjacent particles to shift, creating the appearance of positive charge movement.

PREREQUISITES
  • Understanding of basic electrical charge concepts
  • Familiarity with solid-state physics and band theory
  • Knowledge of local vs. global electrical neutrality
  • Concept of electron mobility and holes in conductors
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  • Study band theory in solid-state physics
  • Explore the concept of electron mobility in semiconductors
  • Research the implications of local and global electrical neutrality
  • Investigate the behavior of charge carriers in different materials
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Students and professionals in physics, electrical engineering, and materials science who are interested in understanding charge dynamics in solids and the behavior of electrons and holes in conductive materials.

johncena
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I can't understand how does the absence of an electron at a point creates a positive charge there. In my opinion, it is wrong on account of conservation of charge. Because if we consider an electron(at a point A) as a system, and if the electron get displaced to another point B(in the system), then if we apply the concept of holes -> firstly, the charge of the system was -e and now the charge is +e-e = 0 !. Which shows that charge can be destroyed.
can anyone help?
 
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You need to distinguish between electrical neutrality at a particular location,(=local neutrality) and electrical neutrality for the whole body or system (=global neutrality).

Atoms, for instance are globally electrically neutral.

But they have regions of local charge, positive in the nucleus and negative in the surrounding electron cloud.
So the sum of all the local non-neutralities balance out to global neutrality overall.

Holes and electrons work similarly. At the site where the electron is displaced from there is a local region of negative deficiency and where is is displaced to there is a corresponding region of local negative excess, but the conductor remains in global neutrality.

I would suggest you don't pursue this concept too far as the model involving electrons as little balls of charge moving around is seriously deficient in solids.
It becomes easier to match more closely to reality when you study band theory.
 


Studiot said:
the model involving electrons as little balls of charge moving around is seriously deficient in solids.

It's OK for this case - just needs a little thought. The same mechanism occurs with landslip along faults and lattice movement at dislocations.

Think about the electrons as being stuck to their atom like peas on a wire grill. Every pea sits in a hole.
If you try to push the peas to one side, they won't move easily because each one resists and the total resistance is huge.

If however, one pea is missing, what happens is that the pea upstream of it can slip into empty space. then the one behind it can slip into the space it vacated - and so on.

The result is that the 'hole' moves in the opposite direction to the push. On a grand scale, you get lots of 'holes' rushing back upstream and looking to all the world like positive charge moving in the opposite direction to the actual electron movement.

Some people like to treat it as if the 'holes' were actual positive charges - in a way they are and when doing calculations it's a lot easier to do the math that way. - but I prefer to keep in mind what's really going on when I think about the actual physics.
 

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