Molecular dynamics research on effect of doping defects on properties of PETN
To investigate the effect of doping defects on properties of pentaerythritol tetranitrate (PETN), the “perfect” and doping defective crystal models of PETN containing pentaerythritol (PE), pentaerythritol mononitrate (PEMonoN), pentaerythritol dinitrate (PEDiN), and pentaerythritol trinitrate (PETRI...
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description | To investigate the effect of doping defects on properties of pentaerythritol tetranitrate (PETN), the “perfect” and doping defective crystal models of PETN containing pentaerythritol (PE), pentaerythritol mononitrate (PEMonoN), pentaerythritol dinitrate (PEDiN), and pentaerythritol trinitrate (PETRIN) were established, respectively. Molecular dynamics (MD) method was applied to perform simulations, and sensitivity, detonation performance, and mechanical properties were calculated and compared. The results indicate that compared with PETN (1 1 0) supercell model, the interaction energy of trigger bond and cohesive energy density of the doped defect models decreased by 2.21~12.43 kJ mol
−1
and 0.0219~0.0421 kJ cm
−3
, respectively, indicating that the sensitivity of defective models increases and the safety decreases. The density, detonation velocity, and detonation pressure of the doped defect model decreased by 0.018~0.061 g cm
−3
, 77.833~272.809 m s
−1
, and 0.746~2.544 GPa, respectively, and the oxygen balance is declined, indicating that the energy density of PETN decreased and the power decreased. Doped defects also cause the elastic modulus, bulk modulus, and shear modulus of PETN to decrease by 0.75~2.16 GPa, 0.44~0.89 GPa, and 0.30~0.89 GPa, respectively. The ratio of bulk modulus to shear modulus and Cauchy pressure increased by 0.05~0.28 GPa and 0.09~1.13 GPa, respectively, indicating that the deformation resistance, fracture strength, and hardness of the doped defect model decrease, stiffness decreases, and flexibility and ductility increase. |
doi_str_mv | 10.1007/s00894-019-4183-4 |
format | Article |
fullrecord | <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_miscellaneous_2283109155</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2283109155</sourcerecordid><originalsourceid>FETCH-LOGICAL-c372t-60cc2bd03b6eda178f27f3cfe8f11efe81dbfa74f75d6893b02f9c6d7399a4953</originalsourceid><addsrcrecordid>eNp1kE1LxDAQhoMouuj-AC9S8OKlOpOkTXMU8Qv8Oug5pMlEK912TbYH_70tuyoIngLzPvNmeBg7RDhFAHWWACotc0CdS6xELrfYDLSs8gK42GYzLBFyriXssXlK7wCAvCgLznfZnkCpsJRqxu7v-5bc0NqY-c_OLhqXskiJbHRvWd9lFAK5VdaHzPfLpnvNPE2DNGXL2C8prhpKU_50-fxwwHaCbRPNN-8-e7m6fL64ye8er28vzu9yJxRf5SU4x2sPoi7JW1RV4CoIF6gKiGN_hb4OVsmgCl9WWtTAg3alV0JrK3Uh9tnJunc84WOgtDKLJjlqW9tRPyTDeSUQNBYTevwHfe-H2I3XTRTXSmMpRgrXlIt9SpGCWcZmYeOnQTCTbrPWbUbdZtJt5LhztGke6gX5n41vuSPA10Aao-6V4u_X_7d-AQiBiW8</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2282979163</pqid></control><display><type>article</type><title>Molecular dynamics research on effect of doping defects on properties of PETN</title><source>SpringerLink Journals - AutoHoldings</source><creator>Qi, Chun-bao ; Wang, Tao ; Miao, Shuang ; Wang, Yu-ling ; Hang, Gui-yun</creator><creatorcontrib>Qi, Chun-bao ; Wang, Tao ; Miao, Shuang ; Wang, Yu-ling ; Hang, Gui-yun</creatorcontrib><description>To investigate the effect of doping defects on properties of pentaerythritol tetranitrate (PETN), the “perfect” and doping defective crystal models of PETN containing pentaerythritol (PE), pentaerythritol mononitrate (PEMonoN), pentaerythritol dinitrate (PEDiN), and pentaerythritol trinitrate (PETRIN) were established, respectively. Molecular dynamics (MD) method was applied to perform simulations, and sensitivity, detonation performance, and mechanical properties were calculated and compared. The results indicate that compared with PETN (1 1 0) supercell model, the interaction energy of trigger bond and cohesive energy density of the doped defect models decreased by 2.21~12.43 kJ mol
−1
and 0.0219~0.0421 kJ cm
−3
, respectively, indicating that the sensitivity of defective models increases and the safety decreases. The density, detonation velocity, and detonation pressure of the doped defect model decreased by 0.018~0.061 g cm
−3
, 77.833~272.809 m s
−1
, and 0.746~2.544 GPa, respectively, and the oxygen balance is declined, indicating that the energy density of PETN decreased and the power decreased. Doped defects also cause the elastic modulus, bulk modulus, and shear modulus of PETN to decrease by 0.75~2.16 GPa, 0.44~0.89 GPa, and 0.30~0.89 GPa, respectively. The ratio of bulk modulus to shear modulus and Cauchy pressure increased by 0.05~0.28 GPa and 0.09~1.13 GPa, respectively, indicating that the deformation resistance, fracture strength, and hardness of the doped defect model decrease, stiffness decreases, and flexibility and ductility increase.</description><identifier>ISSN: 1610-2940</identifier><identifier>EISSN: 0948-5023</identifier><identifier>DOI: 10.1007/s00894-019-4183-4</identifier><identifier>PMID: 31471647</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer Berlin Heidelberg</publisher><subject>Bulk modulus ; Characterization and Evaluation of Materials ; Chemistry ; Chemistry and Materials Science ; Computer Appl. in Life Sciences ; Computer Applications in Chemistry ; Computer simulation ; Crystal defects ; Defects ; Deformation resistance ; Detonation ; Doping ; Flux density ; Fracture strength ; Mechanical properties ; Modulus of elasticity ; Molecular dynamics ; Molecular Medicine ; Original Paper ; PETN ; Sensitivity ; Shear modulus ; Stiffness ; Theoretical and Computational Chemistry</subject><ispartof>Journal of molecular modeling, 2019-09, Vol.25 (9), p.287-9, Article 287</ispartof><rights>Springer-Verlag GmbH Germany, part of Springer Nature 2019</rights><rights>Copyright Springer Nature B.V. 2019</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c372t-60cc2bd03b6eda178f27f3cfe8f11efe81dbfa74f75d6893b02f9c6d7399a4953</citedby><cites>FETCH-LOGICAL-c372t-60cc2bd03b6eda178f27f3cfe8f11efe81dbfa74f75d6893b02f9c6d7399a4953</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s00894-019-4183-4$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s00894-019-4183-4$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,780,784,27924,27925,41488,42557,51319</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/31471647$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Qi, Chun-bao</creatorcontrib><creatorcontrib>Wang, Tao</creatorcontrib><creatorcontrib>Miao, Shuang</creatorcontrib><creatorcontrib>Wang, Yu-ling</creatorcontrib><creatorcontrib>Hang, Gui-yun</creatorcontrib><title>Molecular dynamics research on effect of doping defects on properties of PETN</title><title>Journal of molecular modeling</title><addtitle>J Mol Model</addtitle><addtitle>J Mol Model</addtitle><description>To investigate the effect of doping defects on properties of pentaerythritol tetranitrate (PETN), the “perfect” and doping defective crystal models of PETN containing pentaerythritol (PE), pentaerythritol mononitrate (PEMonoN), pentaerythritol dinitrate (PEDiN), and pentaerythritol trinitrate (PETRIN) were established, respectively. Molecular dynamics (MD) method was applied to perform simulations, and sensitivity, detonation performance, and mechanical properties were calculated and compared. The results indicate that compared with PETN (1 1 0) supercell model, the interaction energy of trigger bond and cohesive energy density of the doped defect models decreased by 2.21~12.43 kJ mol
−1
and 0.0219~0.0421 kJ cm
−3
, respectively, indicating that the sensitivity of defective models increases and the safety decreases. The density, detonation velocity, and detonation pressure of the doped defect model decreased by 0.018~0.061 g cm
−3
, 77.833~272.809 m s
−1
, and 0.746~2.544 GPa, respectively, and the oxygen balance is declined, indicating that the energy density of PETN decreased and the power decreased. Doped defects also cause the elastic modulus, bulk modulus, and shear modulus of PETN to decrease by 0.75~2.16 GPa, 0.44~0.89 GPa, and 0.30~0.89 GPa, respectively. The ratio of bulk modulus to shear modulus and Cauchy pressure increased by 0.05~0.28 GPa and 0.09~1.13 GPa, respectively, indicating that the deformation resistance, fracture strength, and hardness of the doped defect model decrease, stiffness decreases, and flexibility and ductility increase.</description><subject>Bulk modulus</subject><subject>Characterization and Evaluation of Materials</subject><subject>Chemistry</subject><subject>Chemistry and Materials Science</subject><subject>Computer Appl. in Life Sciences</subject><subject>Computer Applications in Chemistry</subject><subject>Computer simulation</subject><subject>Crystal defects</subject><subject>Defects</subject><subject>Deformation resistance</subject><subject>Detonation</subject><subject>Doping</subject><subject>Flux density</subject><subject>Fracture strength</subject><subject>Mechanical properties</subject><subject>Modulus of elasticity</subject><subject>Molecular dynamics</subject><subject>Molecular Medicine</subject><subject>Original Paper</subject><subject>PETN</subject><subject>Sensitivity</subject><subject>Shear modulus</subject><subject>Stiffness</subject><subject>Theoretical and Computational Chemistry</subject><issn>1610-2940</issn><issn>0948-5023</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNp1kE1LxDAQhoMouuj-AC9S8OKlOpOkTXMU8Qv8Oug5pMlEK912TbYH_70tuyoIngLzPvNmeBg7RDhFAHWWACotc0CdS6xELrfYDLSs8gK42GYzLBFyriXssXlK7wCAvCgLznfZnkCpsJRqxu7v-5bc0NqY-c_OLhqXskiJbHRvWd9lFAK5VdaHzPfLpnvNPE2DNGXL2C8prhpKU_50-fxwwHaCbRPNN-8-e7m6fL64ye8er28vzu9yJxRf5SU4x2sPoi7JW1RV4CoIF6gKiGN_hb4OVsmgCl9WWtTAg3alV0JrK3Uh9tnJunc84WOgtDKLJjlqW9tRPyTDeSUQNBYTevwHfe-H2I3XTRTXSmMpRgrXlIt9SpGCWcZmYeOnQTCTbrPWbUbdZtJt5LhztGke6gX5n41vuSPA10Aao-6V4u_X_7d-AQiBiW8</recordid><startdate>20190901</startdate><enddate>20190901</enddate><creator>Qi, Chun-bao</creator><creator>Wang, Tao</creator><creator>Miao, Shuang</creator><creator>Wang, Yu-ling</creator><creator>Hang, Gui-yun</creator><general>Springer Berlin Heidelberg</general><general>Springer Nature B.V</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope></search><sort><creationdate>20190901</creationdate><title>Molecular dynamics research on effect of doping defects on properties of PETN</title><author>Qi, Chun-bao ; Wang, Tao ; Miao, Shuang ; Wang, Yu-ling ; Hang, Gui-yun</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c372t-60cc2bd03b6eda178f27f3cfe8f11efe81dbfa74f75d6893b02f9c6d7399a4953</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Bulk modulus</topic><topic>Characterization and Evaluation of Materials</topic><topic>Chemistry</topic><topic>Chemistry and Materials Science</topic><topic>Computer Appl. in Life Sciences</topic><topic>Computer Applications in Chemistry</topic><topic>Computer simulation</topic><topic>Crystal defects</topic><topic>Defects</topic><topic>Deformation resistance</topic><topic>Detonation</topic><topic>Doping</topic><topic>Flux density</topic><topic>Fracture strength</topic><topic>Mechanical properties</topic><topic>Modulus of elasticity</topic><topic>Molecular dynamics</topic><topic>Molecular Medicine</topic><topic>Original Paper</topic><topic>PETN</topic><topic>Sensitivity</topic><topic>Shear modulus</topic><topic>Stiffness</topic><topic>Theoretical and Computational Chemistry</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Qi, Chun-bao</creatorcontrib><creatorcontrib>Wang, Tao</creatorcontrib><creatorcontrib>Miao, Shuang</creatorcontrib><creatorcontrib>Wang, Yu-ling</creatorcontrib><creatorcontrib>Hang, Gui-yun</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><jtitle>Journal of molecular modeling</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Qi, Chun-bao</au><au>Wang, Tao</au><au>Miao, Shuang</au><au>Wang, Yu-ling</au><au>Hang, Gui-yun</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Molecular dynamics research on effect of doping defects on properties of PETN</atitle><jtitle>Journal of molecular modeling</jtitle><stitle>J Mol Model</stitle><addtitle>J Mol Model</addtitle><date>2019-09-01</date><risdate>2019</risdate><volume>25</volume><issue>9</issue><spage>287</spage><epage>9</epage><pages>287-9</pages><artnum>287</artnum><issn>1610-2940</issn><eissn>0948-5023</eissn><abstract>To investigate the effect of doping defects on properties of pentaerythritol tetranitrate (PETN), the “perfect” and doping defective crystal models of PETN containing pentaerythritol (PE), pentaerythritol mononitrate (PEMonoN), pentaerythritol dinitrate (PEDiN), and pentaerythritol trinitrate (PETRIN) were established, respectively. Molecular dynamics (MD) method was applied to perform simulations, and sensitivity, detonation performance, and mechanical properties were calculated and compared. The results indicate that compared with PETN (1 1 0) supercell model, the interaction energy of trigger bond and cohesive energy density of the doped defect models decreased by 2.21~12.43 kJ mol
−1
and 0.0219~0.0421 kJ cm
−3
, respectively, indicating that the sensitivity of defective models increases and the safety decreases. The density, detonation velocity, and detonation pressure of the doped defect model decreased by 0.018~0.061 g cm
−3
, 77.833~272.809 m s
−1
, and 0.746~2.544 GPa, respectively, and the oxygen balance is declined, indicating that the energy density of PETN decreased and the power decreased. Doped defects also cause the elastic modulus, bulk modulus, and shear modulus of PETN to decrease by 0.75~2.16 GPa, 0.44~0.89 GPa, and 0.30~0.89 GPa, respectively. The ratio of bulk modulus to shear modulus and Cauchy pressure increased by 0.05~0.28 GPa and 0.09~1.13 GPa, respectively, indicating that the deformation resistance, fracture strength, and hardness of the doped defect model decrease, stiffness decreases, and flexibility and ductility increase.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><pmid>31471647</pmid><doi>10.1007/s00894-019-4183-4</doi><tpages>9</tpages></addata></record> |
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subjects | Bulk modulus Characterization and Evaluation of Materials Chemistry Chemistry and Materials Science Computer Appl. in Life Sciences Computer Applications in Chemistry Computer simulation Crystal defects Defects Deformation resistance Detonation Doping Flux density Fracture strength Mechanical properties Modulus of elasticity Molecular dynamics Molecular Medicine Original Paper PETN Sensitivity Shear modulus Stiffness Theoretical and Computational Chemistry |
title | Molecular dynamics research on effect of doping defects on properties of PETN |
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