Современные методы исследования и описания кристаллических структур. Самойлов А.М. - 10 стр.

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n
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 b l ^ G_h[oh^bfh hl\_lblv qlh \u\h^u g_ baf_gylky Ijb aZibkb
mjZ\g_gby\\b^_
d
n
hkl
=
λλ
2sinΘΘ
,
( 1.9 )
]^_
n -
ihjy^hdki_dljZp_eh_qbkehjZ\gh_bl^
Ihkdhevdm
d
n
dd
hkl
nhnknl h k l
= =
***
( 1.10 )
gZijbf_j
d
d
111
222
2
=
;
d
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3
=
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d
hkl***
sin
=
λ
2 Θ
( 1.11 )
>jm]b fb keh\Zfb hl iehkdhklb
( h*k*l*)
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mjZ\g_gbx<mevnZ-;jw]]Zb\ua\Zggucki_dljZfb-]h-]hbl^ihjy^dZ
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djbklZeebq_kdhckljmdlmjuijb\_^_gZgZjbkHkgh\guf
                                                    7
\hagbdgmlv \iheg_ mf_klguc \hijhk ihq_fm ijb jZkq_lZo \hafh`guo j_ne_dkh\ ih
mjZ\g_gbx   ijbgbfZ_lkyihjy^hdki_dljZ n  b\dZdhcf_j_baf_gylky\u\h^u

ijb n    b l ^ G_h[oh^bfh hl\_lblv qlh \u\h^u g_ baf_gylky Ijb aZibkb
mjZ\g_gby  \\b^_

            d hkl                λ
                  =
             n                2 sin Θ                   ,         ( 1.9 )

     ]^_n - ihjy^hdki_dljZp_eh_qbkehjZ\gh_bl^
     Ihkdhevdm

          d = d
             hkl
                          nhnknl   = d      h * k * l *               ( 1.10 )
           n
     gZijbf_j

        d   111
                  = d   222   ;
                                   d  111
                                             = d    333
         2                          3
     Ih^klZ\eyy  \  fh`ghihemqblv

                                      λ
          dh *     k * l*     =
                                   2 sin Θ                       ( 1.11 )



     >jm]bfb keh\Zfb hl iehkdhklb ( h*k*l*) \hagbdZ_l j_ne_dk ih^qbgyxsbcky
mjZ\g_gbxEYJ?GL=?GH=J:NBQ?KDBO
        BKKE?>H<:GBC


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djbklZeebq_kdhckljmdlmjuijb\_^_gZgZjbkHkgh\guf