Misfit in Inconel-Type Superalloy

An important parameter for the characterization of microstructural changes in nickel base superalloys is the misfit - the relative difference between lattice parameters of γ matrix and γ′ precipitates. The misfit in IN738LC superalloy was examined at POLDI time-of-flight (TOF) neutron diffractometer...

Full description

Bibliographic Details
Main Authors: Pavel Strunz, Martin Petrenec, Vadim Davydov, Jaroslav Polák, Přemysl Beran
Format: Article
Language:English
Published: Hindawi Limited 2013-01-01
Series:Advances in Materials Science and Engineering
Online Access:http://dx.doi.org/10.1155/2013/408347
id doaj-4426745282c14c7e9936792805f60056
record_format Article
spelling doaj-4426745282c14c7e9936792805f600562020-11-24T23:08:56ZengHindawi LimitedAdvances in Materials Science and Engineering1687-84341687-84422013-01-01201310.1155/2013/408347408347Misfit in Inconel-Type SuperalloyPavel Strunz0Martin Petrenec1Vadim Davydov2Jaroslav Polák3Přemysl Beran4Nuclear Physics Institute, ASCR, 25068 Řež, Czech RepublicInstitute of Physics of Materials, ASCR, Žižkova 22, 61662 Brno, Czech RepublicMaterials Science and Simulation, ASQ/NUM, PSI, 5232 Villigen, SwitzerlandInstitute of Physics of Materials, ASCR, Žižkova 22, 61662 Brno, Czech RepublicNuclear Physics Institute, ASCR, 25068 Řež, Czech RepublicAn important parameter for the characterization of microstructural changes in nickel base superalloys is the misfit - the relative difference between lattice parameters of γ matrix and γ′ precipitates. The misfit in IN738LC superalloy was examined at POLDI time-of-flight (TOF) neutron diffractometer both at room temperature and in situ at elevated temperatures using a high-temperature furnace. A careful out-of-furnace measurement yielded the lattice parameters of both γ and γ′ phase at room temperature (aγ=3.58611(10) Å, aγ′=3.58857(17) Å) as well as the misfit (equal to 6.9(6)×10-4). The in situ measurement at elevated temperatures provided the temperature dependence of the lattice parameters of γ (up to 1120°C) and γ′ (up to 1000°C). Using these data, the evolution of the misfit with temperature was calculated. The misfit decreases with increasing temperature until it reaches zero value at a temperature around 800°C. Above 800°C, it becomes negative.http://dx.doi.org/10.1155/2013/408347
collection DOAJ
language English
format Article
sources DOAJ
author Pavel Strunz
Martin Petrenec
Vadim Davydov
Jaroslav Polák
Přemysl Beran
spellingShingle Pavel Strunz
Martin Petrenec
Vadim Davydov
Jaroslav Polák
Přemysl Beran
Misfit in Inconel-Type Superalloy
Advances in Materials Science and Engineering
author_facet Pavel Strunz
Martin Petrenec
Vadim Davydov
Jaroslav Polák
Přemysl Beran
author_sort Pavel Strunz
title Misfit in Inconel-Type Superalloy
title_short Misfit in Inconel-Type Superalloy
title_full Misfit in Inconel-Type Superalloy
title_fullStr Misfit in Inconel-Type Superalloy
title_full_unstemmed Misfit in Inconel-Type Superalloy
title_sort misfit in inconel-type superalloy
publisher Hindawi Limited
series Advances in Materials Science and Engineering
issn 1687-8434
1687-8442
publishDate 2013-01-01
description An important parameter for the characterization of microstructural changes in nickel base superalloys is the misfit - the relative difference between lattice parameters of γ matrix and γ′ precipitates. The misfit in IN738LC superalloy was examined at POLDI time-of-flight (TOF) neutron diffractometer both at room temperature and in situ at elevated temperatures using a high-temperature furnace. A careful out-of-furnace measurement yielded the lattice parameters of both γ and γ′ phase at room temperature (aγ=3.58611(10) Å, aγ′=3.58857(17) Å) as well as the misfit (equal to 6.9(6)×10-4). The in situ measurement at elevated temperatures provided the temperature dependence of the lattice parameters of γ (up to 1120°C) and γ′ (up to 1000°C). Using these data, the evolution of the misfit with temperature was calculated. The misfit decreases with increasing temperature until it reaches zero value at a temperature around 800°C. Above 800°C, it becomes negative.
url http://dx.doi.org/10.1155/2013/408347
work_keys_str_mv AT pavelstrunz misfitininconeltypesuperalloy
AT martinpetrenec misfitininconeltypesuperalloy
AT vadimdavydov misfitininconeltypesuperalloy
AT jaroslavpolak misfitininconeltypesuperalloy
AT premyslberan misfitininconeltypesuperalloy
_version_ 1725612288741736448