Melt-crystal phase transition in a two-component system
Abstract The melt-crystal phase transition in a two-component system is described by a generalized Ornstein-Zernicke equation for one- and two-particle distribution functions. The jump in the density δn under melt crystallization is a small parameter. The desired distribution functions are found as...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Agrafonov, Yu. V. [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2000 |
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| Schlagwörter: |
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| Anmerkung: |
© Kluwer Academic/Plenum Publishers 2000 |
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| Übergeordnetes Werk: |
Enthalten in: Russian physics journal - Kluwer Academic Publishers-Plenum Publishers, 1992, 43(2000), 2 vom: Feb., Seite 129-136 |
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| Übergeordnetes Werk: |
volume:43 ; year:2000 ; number:2 ; month:02 ; pages:129-136 |
| Links: |
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| DOI / URN: |
10.1007/BF02508600 |
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OLC2033054128 |
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| 520 | |a Abstract The melt-crystal phase transition in a two-component system is described by a generalized Ornstein-Zernicke equation for one- and two-particle distribution functions. The jump in the density δn under melt crystallization is a small parameter. The desired distribution functions are found as δn power series. The two-particle distribution function for the melt along its crystallization line is chosen as a zeroth approximation. | ||
| 650 | 4 | |a Power Series Expansion | |
| 650 | 4 | |a Zeroth Approximation | |
| 650 | 4 | |a Partial Amplitude | |
| 650 | 4 | |a Linear Integral Equation | |
| 650 | 4 | |a Crystallization Line | |
| 700 | 1 | |a Biryulina, T. V. |4 aut | |
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10.1007/BF02508600 doi (DE-627)OLC2033054128 (DE-He213)BF02508600-p DE-627 ger DE-627 rakwb eng 530 370 VZ Agrafonov, Yu. V. verfasserin aut Melt-crystal phase transition in a two-component system 2000 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic/Plenum Publishers 2000 Abstract The melt-crystal phase transition in a two-component system is described by a generalized Ornstein-Zernicke equation for one- and two-particle distribution functions. The jump in the density δn under melt crystallization is a small parameter. The desired distribution functions are found as δn power series. The two-particle distribution function for the melt along its crystallization line is chosen as a zeroth approximation. Power Series Expansion Zeroth Approximation Partial Amplitude Linear Integral Equation Crystallization Line Biryulina, T. V. aut Enthalten in Russian physics journal Kluwer Academic Publishers-Plenum Publishers, 1992 43(2000), 2 vom: Feb., Seite 129-136 (DE-627)131169718 (DE-600)1138228-4 (DE-576)033029253 1064-8887 nnns volume:43 year:2000 number:2 month:02 pages:129-136 https://doi.org/10.1007/BF02508600 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2021 GBV_ILN_4700 AR 43 2000 2 02 129-136 |
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10.1007/BF02508600 doi (DE-627)OLC2033054128 (DE-He213)BF02508600-p DE-627 ger DE-627 rakwb eng 530 370 VZ Agrafonov, Yu. V. verfasserin aut Melt-crystal phase transition in a two-component system 2000 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic/Plenum Publishers 2000 Abstract The melt-crystal phase transition in a two-component system is described by a generalized Ornstein-Zernicke equation for one- and two-particle distribution functions. The jump in the density δn under melt crystallization is a small parameter. The desired distribution functions are found as δn power series. The two-particle distribution function for the melt along its crystallization line is chosen as a zeroth approximation. Power Series Expansion Zeroth Approximation Partial Amplitude Linear Integral Equation Crystallization Line Biryulina, T. V. aut Enthalten in Russian physics journal Kluwer Academic Publishers-Plenum Publishers, 1992 43(2000), 2 vom: Feb., Seite 129-136 (DE-627)131169718 (DE-600)1138228-4 (DE-576)033029253 1064-8887 nnns volume:43 year:2000 number:2 month:02 pages:129-136 https://doi.org/10.1007/BF02508600 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2021 GBV_ILN_4700 AR 43 2000 2 02 129-136 |
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Abstract The melt-crystal phase transition in a two-component system is described by a generalized Ornstein-Zernicke equation for one- and two-particle distribution functions. The jump in the density δn under melt crystallization is a small parameter. The desired distribution functions are found as δn power series. The two-particle distribution function for the melt along its crystallization line is chosen as a zeroth approximation. © Kluwer Academic/Plenum Publishers 2000 |
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Abstract The melt-crystal phase transition in a two-component system is described by a generalized Ornstein-Zernicke equation for one- and two-particle distribution functions. The jump in the density δn under melt crystallization is a small parameter. The desired distribution functions are found as δn power series. The two-particle distribution function for the melt along its crystallization line is chosen as a zeroth approximation. © Kluwer Academic/Plenum Publishers 2000 |
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Abstract The melt-crystal phase transition in a two-component system is described by a generalized Ornstein-Zernicke equation for one- and two-particle distribution functions. The jump in the density δn under melt crystallization is a small parameter. The desired distribution functions are found as δn power series. The two-particle distribution function for the melt along its crystallization line is chosen as a zeroth approximation. © Kluwer Academic/Plenum Publishers 2000 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">OLC2033054128</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230504035708.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200820s2000 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/BF02508600</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2033054128</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)BF02508600-p</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="a">370</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Agrafonov, Yu. V.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Melt-crystal phase transition in a two-component system</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2000</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Kluwer Academic/Plenum Publishers 2000</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The melt-crystal phase transition in a two-component system is described by a generalized Ornstein-Zernicke equation for one- and two-particle distribution functions. The jump in the density δn under melt crystallization is a small parameter. The desired distribution functions are found as δn power series. The two-particle distribution function for the melt along its crystallization line is chosen as a zeroth approximation.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Power Series Expansion</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Zeroth Approximation</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Partial Amplitude</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Linear Integral Equation</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Crystallization Line</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Biryulina, T. V.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Russian physics journal</subfield><subfield code="d">Kluwer Academic Publishers-Plenum Publishers, 1992</subfield><subfield code="g">43(2000), 2 vom: Feb., Seite 129-136</subfield><subfield code="w">(DE-627)131169718</subfield><subfield code="w">(DE-600)1138228-4</subfield><subfield code="w">(DE-576)033029253</subfield><subfield code="x">1064-8887</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:43</subfield><subfield code="g">year:2000</subfield><subfield code="g">number:2</subfield><subfield code="g">month:02</subfield><subfield code="g">pages:129-136</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/BF02508600</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_21</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2021</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4700</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">43</subfield><subfield code="j">2000</subfield><subfield code="e">2</subfield><subfield code="c">02</subfield><subfield code="h">129-136</subfield></datafield></record></collection>
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