cp-frenkel defect.pptx

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    Frenkel defect

    Derivation of equilibrium

    number of Frenkel defectspresent in elemental solids ormonatomic solids

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    Frenkel defect: derivation

    • Frenkel defect = Vacancy +interstitial atoms

    • Interstitial atoms are the extra atomsthat are squeezed in beteen normalatom sites!

    • "tom from a re#ular lattice site isremoved and placed it at theinterstitial position!

    •  $here by vacancy and interstitial is

    simultaneously created% knon as

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    • &imilar to previous derivations in the caseof &chottky defect

    •'alculate the number of Frenkel defects inequilibrium at a temperature $

    • (et

    )i = the ener#y required to displace an

    atom from re#ular lattice site to aninterstitial position *activation ener#y tocreate Frenkel defect

    ,= $otal number of atoms in the crystal,i = $otal number of interstitial sites

    present in the crystal

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     $otal number of ays in hich n Frenkel defects can be formed by

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    and is% therefore% termed as ionic conductivity! $he above fact of ion motion #ivin# rise toconductivity is easily at hand if a potentialdi-erence is applied beteen to oppositefaces of an ionic crystal and the current ismeasured! $hese currents are too lar#e to be

    explained in terms of the motion of electronsbecause the number of electrons in theconduction band at the temperatures involvedill be much too small! 'onsequently% the

    currents must be a result of the mi#ration ofions under the in.uence of the electric /eld!Further% for the mi#ration of ions 0di-usion1 thelattice must have some vacant sites to #ive

    place to mi#rated ions! $his implies that

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    Question:

    Derive the equation forequilibrium number ofFrenkel defects for

    ionic solids