Journal article 1858 views 534 downloads
Evolution of Wilshire equations for creep life prediction
Materials at High Temperatures, Volume: 31, Issue: 3, Pages: 233 - 238
Swansea University Authors:
Mark Whittaker , Will Harrison
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DOI (Published version): 10.1179/1878641314Y.0000000019
Abstract
In the past decade, a new approach to predictive creep lifing has been developed, known as the Wilshire equations. Having been applied to a range of power generation and aerospace materials, the understanding of material behaviour associated with the equations has developed significantly. With the e...
Published in: | Materials at High Temperatures |
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2014
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URI: | https://cronfa.swan.ac.uk/Record/cronfa21246 |
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2016-04-18T12:19:35.2501630 v2 21246 2015-05-08 Evolution of Wilshire equations for creep life prediction a146c6d442cb2c466d096179f9ac97ca 0000-0002-5854-0726 Mark Whittaker Mark Whittaker true false dae59f76fa4f63123aa028abfcd2b07a 0000-0002-0380-7075 Will Harrison Will Harrison true false 2015-05-08 EAAS In the past decade, a new approach to predictive creep lifing has been developed, known as the Wilshire equations. Having been applied to a range of power generation and aerospace materials, the understanding of material behaviour associated with the equations has developed significantly. With the equations based around the dominance of diffusion controlled dislocation movement for creep deformation under typical engineering stresses and behaviours, the predictions made are related to microstructural phenomena, such as the onset of yield. The current paper seeks to review the application and development of the Wilshire equations, with suggestions for future research in the area. Journal Article Materials at High Temperatures 31 3 233 238 31 12 2014 2014-12-31 10.1179/1878641314Y.0000000019 COLLEGE NANME Engineering and Applied Sciences School COLLEGE CODE EAAS Swansea University 2016-04-18T12:19:35.2501630 2015-05-08T13:37:08.3035591 M. T. Whittaker 1 W. J. Harrison 2 Mark Whittaker 0000-0002-5854-0726 3 Will Harrison 0000-0002-0380-7075 4 0021246-14032016134525.pdf CronfaPDF.pdf 2016-03-14T13:45:25.4830000 Output 790179 application/pdf Accepted Manuscript true 2016-03-14T00:00:00.0000000 true |
title |
Evolution of Wilshire equations for creep life prediction |
spellingShingle |
Evolution of Wilshire equations for creep life prediction Mark Whittaker Will Harrison |
title_short |
Evolution of Wilshire equations for creep life prediction |
title_full |
Evolution of Wilshire equations for creep life prediction |
title_fullStr |
Evolution of Wilshire equations for creep life prediction |
title_full_unstemmed |
Evolution of Wilshire equations for creep life prediction |
title_sort |
Evolution of Wilshire equations for creep life prediction |
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a146c6d442cb2c466d096179f9ac97ca dae59f76fa4f63123aa028abfcd2b07a |
author_id_fullname_str_mv |
a146c6d442cb2c466d096179f9ac97ca_***_Mark Whittaker dae59f76fa4f63123aa028abfcd2b07a_***_Will Harrison |
author |
Mark Whittaker Will Harrison |
author2 |
M. T. Whittaker W. J. Harrison Mark Whittaker Will Harrison |
format |
Journal article |
container_title |
Materials at High Temperatures |
container_volume |
31 |
container_issue |
3 |
container_start_page |
233 |
publishDate |
2014 |
institution |
Swansea University |
doi_str_mv |
10.1179/1878641314Y.0000000019 |
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description |
In the past decade, a new approach to predictive creep lifing has been developed, known as the Wilshire equations. Having been applied to a range of power generation and aerospace materials, the understanding of material behaviour associated with the equations has developed significantly. With the equations based around the dominance of diffusion controlled dislocation movement for creep deformation under typical engineering stresses and behaviours, the predictions made are related to microstructural phenomena, such as the onset of yield. The current paper seeks to review the application and development of the Wilshire equations, with suggestions for future research in the area. |
published_date |
2014-12-31T06:36:45Z |
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1829264535242932224 |
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11.0578165 |