Melting of pentaerythritol tetranitrate (PETN) nanoconfined in controlled pore glasses (CPG)

Ben Xu; Xiaojun Di; Gregory B. McKenna

doi:10.1007/s10973-013-3075-6

Melting of pentaerythritol tetranitrate (PETN) nanoconfined in controlled pore glasses (CPG)

Ben Xu, Xiaojun Di, Gregory B. McKenna

Chemical Engineering

Research output: Contribution to journal › Article › peer-review

11 Scopus citations

Abstract

The melting temperature depression of pentaerythritol tetranitrate, nanoconfined in controlled pore glasses (CPG), was systematically studied by differential scanning calorimetry (DSC). The solid-liquid interfacial energy σ _sl was obtained from the Gibbs-Thomson equation fit to melting temperature vs. reciprocal pore diameter. The pore size distribution of the CPG pores was also estimated from the DSC data. Pore sizes obtained from the manufacturer by BET are compared with those determined from the DSC curves using either the curves directly or by assuming spherical shaped confining cavities. The thermal mass vales are in better agreement with the BET estimation.

Original language	English
Pages (from-to)	539-543
Number of pages	5
Journal	Journal of Thermal Analysis and Calorimetry
Volume	113
Issue number	2
DOIs	https://doi.org/10.1007/s10973-013-3075-6
State	Published - Aug 2013

Keywords

Energetic materials
Melting
Nanoconfinement
PETN

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title = "Melting of pentaerythritol tetranitrate (PETN) nanoconfined in controlled pore glasses (CPG)",

abstract = "The melting temperature depression of pentaerythritol tetranitrate, nanoconfined in controlled pore glasses (CPG), was systematically studied by differential scanning calorimetry (DSC). The solid-liquid interfacial energy σ sl was obtained from the Gibbs-Thomson equation fit to melting temperature vs. reciprocal pore diameter. The pore size distribution of the CPG pores was also estimated from the DSC data. Pore sizes obtained from the manufacturer by BET are compared with those determined from the DSC curves using either the curves directly or by assuming spherical shaped confining cavities. The thermal mass vales are in better agreement with the BET estimation.",

keywords = "Energetic materials, Melting, Nanoconfinement, PETN",

author = "Ben Xu and Xiaojun Di and McKenna, {Gregory B.}",

note = "Funding Information: Acknowledgments We thank Brandon L. Weeks for providing the PETN and useful discussions to the content of this paper. We are grateful to the Office of Naval Research under Project No. N00014-11-1-0424, N00014-06-1-0922 and the John R. Bradford endowment at Texas Tech University for partial support of this work.",

year = "2013",

month = aug,

doi = "10.1007/s10973-013-3075-6",

language = "English",

volume = "113",

pages = "539--543",

journal = "Journal of Thermal Analysis and Calorimetry",

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T1 - Melting of pentaerythritol tetranitrate (PETN) nanoconfined in controlled pore glasses (CPG)

AU - Xu, Ben

AU - Di, Xiaojun

AU - McKenna, Gregory B.

N1 - Funding Information: Acknowledgments We thank Brandon L. Weeks for providing the PETN and useful discussions to the content of this paper. We are grateful to the Office of Naval Research under Project No. N00014-11-1-0424, N00014-06-1-0922 and the John R. Bradford endowment at Texas Tech University for partial support of this work.

PY - 2013/8

Y1 - 2013/8

N2 - The melting temperature depression of pentaerythritol tetranitrate, nanoconfined in controlled pore glasses (CPG), was systematically studied by differential scanning calorimetry (DSC). The solid-liquid interfacial energy σ sl was obtained from the Gibbs-Thomson equation fit to melting temperature vs. reciprocal pore diameter. The pore size distribution of the CPG pores was also estimated from the DSC data. Pore sizes obtained from the manufacturer by BET are compared with those determined from the DSC curves using either the curves directly or by assuming spherical shaped confining cavities. The thermal mass vales are in better agreement with the BET estimation.

AB - The melting temperature depression of pentaerythritol tetranitrate, nanoconfined in controlled pore glasses (CPG), was systematically studied by differential scanning calorimetry (DSC). The solid-liquid interfacial energy σ sl was obtained from the Gibbs-Thomson equation fit to melting temperature vs. reciprocal pore diameter. The pore size distribution of the CPG pores was also estimated from the DSC data. Pore sizes obtained from the manufacturer by BET are compared with those determined from the DSC curves using either the curves directly or by assuming spherical shaped confining cavities. The thermal mass vales are in better agreement with the BET estimation.

KW - Energetic materials

KW - Melting

KW - Nanoconfinement

KW - PETN

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U2 - 10.1007/s10973-013-3075-6

DO - 10.1007/s10973-013-3075-6

M3 - Article

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VL - 113

SP - 539

EP - 543

JO - Journal of Thermal Analysis and Calorimetry

JF - Journal of Thermal Analysis and Calorimetry

SN - 1388-6150

IS - 2

ER -

Melting of pentaerythritol tetranitrate (PETN) nanoconfined in controlled pore glasses (CPG)

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