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Electric Current
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Construction Mechanic Basic Volume 02 - Construction methods and practices
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Figure 1-7.—Hole movement theory.

SEMICONDUCTORS A semiconductor is an electrical device that acts as a   conductor   under   certain   conditions   and   as   a nonconductor  under  other  conditions.  The  most popular  of  all  semiconductors  is  silicon.  In  its  pure state, silicon is neither a good conductor nor insulator. But  by  processing  silicon  in  the  following  ways,  its conductive or insulative properties can be adjusted to suit  just  about  any  need.  When  a  number  of  silicon atoms  are  jammed  together  in  crystalline  (glasslike) form, they form a covalent (sharing) bond. Therefore, the electrons in the outer ring of one silicon atom join with the outer ring of other silicon atoms, resulting in a sharing  of  outer  ring  electrons  between  all  of  the atoms. It can be seen in figure 1-4 that covalent sharing gives  each  atom  eight  electrons  in  its  outer  orbit, making the orbit complete. This makes the material an insulator because it contains more than four electrons in  its  outer  orbit.  When  certain  materials,  such  as phosphorus, are added to the silicon crystal in highly controlled  amounts,  the  resultant  mixture  becomes  a conductor  (fig.  1-5).  This  is  because  phosphorus, which  has  five  electrons  in  forming  a  covalent  bond with  silicon  (which  has  four  electrons  in  its  outer shell),  will  yield  one  free  electron  per  molecule,  thus making  the  material  an  electrical  conductor.  The process  of  adding  impurities  to  a  semiconductor  is called   doping.   Any   semiconductor   material   that   is doped  to  yield  free  electrons  is  called  N-type  material. When boron, which has three electrons in its outer ring,  is  used  to  dope  the  silicon  crystal,  the  resultant Figure 1-4.—Covalent bonding of silicon. Figure    l-5.-Phosphorus-doped    silicon. 1-4

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