Hesabat d\u00f6vr\u00fcnd\u0259 \u201cMaye v\u0259 qaz mexanikas\u0131\u201d \u015f\u00f6b\u0259sind\u0259 plana uy\u011fun olaraq t\u0259dqiqat i\u015fl\u0259ri apar\u0131lm\u0131\u015fd\u0131r.<\/p>\n
M\u00f6vzu: HETEROGEN MAYE AXINLARINDA S\u018fRH\u018fD QATLARIN QEYR\u0130-STAS\u0130ONAR PROSESL\u018fR\u018f T\u018fS\u0130RL\u018fR\u0130N\u0130N T\u018fDQ\u0130Q\u0130.
\n\u0130\u015f 1. Heterogen sisteml\u0259rin borularla ax\u0131nlar\u0131nda d\u00f6y\u00fcnt\u00fcl\u00fc rejiml\u0259rin t\u0259dqiqi.
\nBoru k\u0259m\u0259rl\u0259rind\u0259 ax\u0131n x\u00fcsussiyy\u0259tl\u0259rinin d\u0259yi\u015film\u0259sin\u0259 \u0259sas s\u0259b\u0259b, fl\u00fcidl\u0259rin qar\u0131\u015f\u0131qlar \u015f\u0259klind\u0259 h\u0259r\u0259k\u0259t etm\u0259sidir. H\u0259r\u0259k\u0259t ed\u0259n sisteml\u0259rd\u0259 m\u00fcxt\u0259lifliyin olmas\u0131, bu sisteml\u0259rin, ax\u0131n\u0131nda s\u00fcr\u0259tl\u0259rd\u0259 m\u00fcxt\u0259lifliy\u0259 g\u0259tirir. Bel\u0259 m\u00fcxt\u0259lif s\u00fcr\u0259tl\u0259r ax\u0131nda d\u00f6y\u00fcnt\u00fcl\u00fc rejiml\u0259r yarad\u0131r. Hesabat zaman\u0131 bir\u00f6l\u00e7\u00fcl\u00fc ax\u0131n sxemi \u00e7\u0259r\u00e7iv\u0259sind\u0259 heterogen sisteml\u0259rin d\u00f6y\u00fcnt\u00fcl\u00fc rejiml\u0259rin\u0259 bax\u0131lm\u0131\u015fd\u0131r.
\n\u0130\u015f 2. Ax\u0131n rejiml\u0259rind\u0259n s\u0259rh\u0259d qatlarda elektrokinetik v\u0259 uy\u011fun qeyri stasionar prosesl\u0259rin modell\u0259\u015fdirm\u0259si.
\nHesabat zaman\u0131 borularda reoloji m\u00fcr\u0259kk\u0259b sisteml\u0259rin ax\u0131n\u0131ndan yaranan elektrokinetik potensial\u0131n qeyri stasionar rejiml\u0259rin t\u0259nziml\u0259m\u0259si prosesl\u0259ri t\u0259dqiq olunmu\u015fdur. Dispers sisteml\u0259rd\u0259 ax\u0131nda elektrokinetik potensial\u0131n \u0259m\u0259l\u0259 g\u0259lm\u0259si borularda qaz qar\u0131\u015f\u0131ql\u0131 heterogen sisteml\u0259rin h\u0259r\u0259k\u0259tind\u0259 hidrodinamik parametrl\u0259rin t\u0259nziml\u0259nm\u0259si \u015f\u0259rtl\u0259rin\u0259 bax\u0131l\u0131r.
\n\u0130\u015f 3. Qazl\u0131 mayel\u0259rd\u0259 qazyaranman\u0131n dal\u011fa parametrl\u0259r\u0259 t\u0259sirl\u0259rin t\u0259dqiqi:
\n\u0130\u015fd\u0259 qaz-maye qar\u0131\u015f\u0131qlar\u0131n\u0131n n\u0259qli zaman\u0131 yaranan dal\u011falar\u0131n yay\u0131lmas\u0131 v\u0259 qaz qabarc\u0131qlar\u0131n\u0131n hidroz\u0259rb\u0259 prosesin\u0259 t\u0259sirin\u0259 bax\u0131lm\u0131\u015fd\u0131r. Mayenin h\u0259r\u0259k\u0259t v\u0259 k\u0259silm\u0259zlik t\u0259nlikl\u0259rinin riyazi ifad\u0259l\u0259rini n\u0259z\u0259r\u0259 al\u0131nmaqla dal\u011fan\u0131n amplitudas\u0131n\u0131 xaraketriz\u0259 ed\u0259n t\u0259nlik tap\u0131lm\u0131\u015fd\u0131r. Termobarik \u015f\u0259raitd\u0259 t\u0259nlikd\u0259 qabarc\u0131\u011f\u0131n radiusa m\u00fcxt\u0259lif qiym\u0259tl\u0259r verilm\u0259kl\u0259, dal\u011fan\u0131n yay\u0131lma sah\u0259si t\u0259yin edilmi\u015f v\u0259 dal\u011fa amplitudas\u0131n\u0131n qabarc\u0131\u011f\u0131n radiusundan as\u0131l\u0131 olaraq d\u0259yi\u015film\u0259si \u00fc\u00e7\u00fcn uy\u011fun qiym\u0259tl\u0259r m\u00fc\u0259yy\u0259nl\u0259\u015fdirilmi\u015fdir.
\nHesabat zaman\u0131 \u015f\u00f6b\u0259 \u0259m\u0259kda\u015flar\u0131 SOCAR-\u0131n Elm Fondu d\u00f6vl\u0259t v\u0259 c\u0259miyy\u0259t \u00fc\u00e7\u00fcn \u0259h\u0259miyy\u0259t k\u0259sb ed\u0259n fundamental v\u0259 innovasiya y\u00f6n\u00fcml\u00fc elmi-t\u0259dqiqat layih\u0259l\u0259rini v\u0259 dig\u0259r elmi t\u0259dbirl\u0259ri d\u0259st\u0259kl\u0259m\u0259k m\u0259qs\u0259dli elan ed\u0259n m\u00fcsabiq\u0259d\u0259 i\u015ftirak ed\u0259r\u0259k \u201cQeyri bircins laylarda qal\u0131q neftl\u0259rin s\u0131x\u0131\u015fd\u0131rma prosesini optimalla\u015fd\u0131rmaq \u00fc\u00e7\u00fcn yeni hidrodinamik \u00fcsulun i\u015fl\u0259nm\u0259si\u201d m\u00f6vzusunda olan Layih\u0259 qalib g\u0259lmi\u015fdir.<\/p>\n