Effect of structural factors on the yield strength of beryllium
Conclusions The coefficients of the Hall—Petch equation are determined in relation to the percentage of resistance to basal and prismatic slip in the flow stress of polycrystalline beryllium.With increasing testing temperatures the variation of $ σ_{i} $ is similar to the variation of the yield stre...
Ausführliche Beschreibung
Autor*in: |
Khristenko, I. N. [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
1976 |
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Schlagwörter: |
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Anmerkung: |
© Consultants Bureau 1976 |
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Übergeordnetes Werk: |
Enthalten in: Metal science and heat treatment - Kluwer Academic Publishers-Plenum Publishers, 1959, 18(1976), 7 vom: Juli, Seite 597-600 |
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Übergeordnetes Werk: |
volume:18 ; year:1976 ; number:7 ; month:07 ; pages:597-600 |
Links: |
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DOI / URN: |
10.1007/BF00703810 |
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Katalog-ID: |
OLC2048012507 |
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520 | |a Conclusions The coefficients of the Hall—Petch equation are determined in relation to the percentage of resistance to basal and prismatic slip in the flow stress of polycrystalline beryllium.With increasing testing temperatures the variation of $ σ_{i} $ is similar to the variation of the yield strength; coefficient Ky changes little up to 500°K and then decreases at higher temperatures.With increasing impurity concentrations the value of $ σ_{i} $ increases, Ky remaining almost unchanged. | ||
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700 | 1 | |a Tikhinskii, G. F. |4 aut | |
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10.1007/BF00703810 doi (DE-627)OLC2048012507 (DE-He213)BF00703810-p DE-627 ger DE-627 rakwb eng 670 620 660 VZ Khristenko, I. N. verfasserin aut Effect of structural factors on the yield strength of beryllium 1976 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Consultants Bureau 1976 Conclusions The coefficients of the Hall—Petch equation are determined in relation to the percentage of resistance to basal and prismatic slip in the flow stress of polycrystalline beryllium.With increasing testing temperatures the variation of $ σ_{i} $ is similar to the variation of the yield strength; coefficient Ky changes little up to 500°K and then decreases at higher temperatures.With increasing impurity concentrations the value of $ σ_{i} $ increases, Ky remaining almost unchanged. Yield Strength Structural Factor Flow Stress Testing Temperature Beryllium Papirov, I. I. aut Tikhinskii, G. F. aut Enthalten in Metal science and heat treatment Kluwer Academic Publishers-Plenum Publishers, 1959 18(1976), 7 vom: Juli, Seite 597-600 (DE-627)129596981 (DE-600)240858-2 (DE-576)015090159 0026-0673 nnns volume:18 year:1976 number:7 month:07 pages:597-600 https://doi.org/10.1007/BF00703810 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_11 GBV_ILN_30 GBV_ILN_70 GBV_ILN_2015 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4319 AR 18 1976 7 07 597-600 |
spelling |
10.1007/BF00703810 doi (DE-627)OLC2048012507 (DE-He213)BF00703810-p DE-627 ger DE-627 rakwb eng 670 620 660 VZ Khristenko, I. N. verfasserin aut Effect of structural factors on the yield strength of beryllium 1976 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Consultants Bureau 1976 Conclusions The coefficients of the Hall—Petch equation are determined in relation to the percentage of resistance to basal and prismatic slip in the flow stress of polycrystalline beryllium.With increasing testing temperatures the variation of $ σ_{i} $ is similar to the variation of the yield strength; coefficient Ky changes little up to 500°K and then decreases at higher temperatures.With increasing impurity concentrations the value of $ σ_{i} $ increases, Ky remaining almost unchanged. Yield Strength Structural Factor Flow Stress Testing Temperature Beryllium Papirov, I. I. aut Tikhinskii, G. F. aut Enthalten in Metal science and heat treatment Kluwer Academic Publishers-Plenum Publishers, 1959 18(1976), 7 vom: Juli, Seite 597-600 (DE-627)129596981 (DE-600)240858-2 (DE-576)015090159 0026-0673 nnns volume:18 year:1976 number:7 month:07 pages:597-600 https://doi.org/10.1007/BF00703810 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_11 GBV_ILN_30 GBV_ILN_70 GBV_ILN_2015 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4319 AR 18 1976 7 07 597-600 |
allfields_unstemmed |
10.1007/BF00703810 doi (DE-627)OLC2048012507 (DE-He213)BF00703810-p DE-627 ger DE-627 rakwb eng 670 620 660 VZ Khristenko, I. N. verfasserin aut Effect of structural factors on the yield strength of beryllium 1976 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Consultants Bureau 1976 Conclusions The coefficients of the Hall—Petch equation are determined in relation to the percentage of resistance to basal and prismatic slip in the flow stress of polycrystalline beryllium.With increasing testing temperatures the variation of $ σ_{i} $ is similar to the variation of the yield strength; coefficient Ky changes little up to 500°K and then decreases at higher temperatures.With increasing impurity concentrations the value of $ σ_{i} $ increases, Ky remaining almost unchanged. Yield Strength Structural Factor Flow Stress Testing Temperature Beryllium Papirov, I. I. aut Tikhinskii, G. F. aut Enthalten in Metal science and heat treatment Kluwer Academic Publishers-Plenum Publishers, 1959 18(1976), 7 vom: Juli, Seite 597-600 (DE-627)129596981 (DE-600)240858-2 (DE-576)015090159 0026-0673 nnns volume:18 year:1976 number:7 month:07 pages:597-600 https://doi.org/10.1007/BF00703810 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_11 GBV_ILN_30 GBV_ILN_70 GBV_ILN_2015 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4319 AR 18 1976 7 07 597-600 |
allfieldsGer |
10.1007/BF00703810 doi (DE-627)OLC2048012507 (DE-He213)BF00703810-p DE-627 ger DE-627 rakwb eng 670 620 660 VZ Khristenko, I. N. verfasserin aut Effect of structural factors on the yield strength of beryllium 1976 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Consultants Bureau 1976 Conclusions The coefficients of the Hall—Petch equation are determined in relation to the percentage of resistance to basal and prismatic slip in the flow stress of polycrystalline beryllium.With increasing testing temperatures the variation of $ σ_{i} $ is similar to the variation of the yield strength; coefficient Ky changes little up to 500°K and then decreases at higher temperatures.With increasing impurity concentrations the value of $ σ_{i} $ increases, Ky remaining almost unchanged. Yield Strength Structural Factor Flow Stress Testing Temperature Beryllium Papirov, I. I. aut Tikhinskii, G. F. aut Enthalten in Metal science and heat treatment Kluwer Academic Publishers-Plenum Publishers, 1959 18(1976), 7 vom: Juli, Seite 597-600 (DE-627)129596981 (DE-600)240858-2 (DE-576)015090159 0026-0673 nnns volume:18 year:1976 number:7 month:07 pages:597-600 https://doi.org/10.1007/BF00703810 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_11 GBV_ILN_30 GBV_ILN_70 GBV_ILN_2015 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4319 AR 18 1976 7 07 597-600 |
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10.1007/BF00703810 doi (DE-627)OLC2048012507 (DE-He213)BF00703810-p DE-627 ger DE-627 rakwb eng 670 620 660 VZ Khristenko, I. N. verfasserin aut Effect of structural factors on the yield strength of beryllium 1976 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Consultants Bureau 1976 Conclusions The coefficients of the Hall—Petch equation are determined in relation to the percentage of resistance to basal and prismatic slip in the flow stress of polycrystalline beryllium.With increasing testing temperatures the variation of $ σ_{i} $ is similar to the variation of the yield strength; coefficient Ky changes little up to 500°K and then decreases at higher temperatures.With increasing impurity concentrations the value of $ σ_{i} $ increases, Ky remaining almost unchanged. Yield Strength Structural Factor Flow Stress Testing Temperature Beryllium Papirov, I. I. aut Tikhinskii, G. F. aut Enthalten in Metal science and heat treatment Kluwer Academic Publishers-Plenum Publishers, 1959 18(1976), 7 vom: Juli, Seite 597-600 (DE-627)129596981 (DE-600)240858-2 (DE-576)015090159 0026-0673 nnns volume:18 year:1976 number:7 month:07 pages:597-600 https://doi.org/10.1007/BF00703810 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_11 GBV_ILN_30 GBV_ILN_70 GBV_ILN_2015 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4319 AR 18 1976 7 07 597-600 |
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Conclusions The coefficients of the Hall—Petch equation are determined in relation to the percentage of resistance to basal and prismatic slip in the flow stress of polycrystalline beryllium.With increasing testing temperatures the variation of $ σ_{i} $ is similar to the variation of the yield strength; coefficient Ky changes little up to 500°K and then decreases at higher temperatures.With increasing impurity concentrations the value of $ σ_{i} $ increases, Ky remaining almost unchanged. © Consultants Bureau 1976 |
abstractGer |
Conclusions The coefficients of the Hall—Petch equation are determined in relation to the percentage of resistance to basal and prismatic slip in the flow stress of polycrystalline beryllium.With increasing testing temperatures the variation of $ σ_{i} $ is similar to the variation of the yield strength; coefficient Ky changes little up to 500°K and then decreases at higher temperatures.With increasing impurity concentrations the value of $ σ_{i} $ increases, Ky remaining almost unchanged. © Consultants Bureau 1976 |
abstract_unstemmed |
Conclusions The coefficients of the Hall—Petch equation are determined in relation to the percentage of resistance to basal and prismatic slip in the flow stress of polycrystalline beryllium.With increasing testing temperatures the variation of $ σ_{i} $ is similar to the variation of the yield strength; coefficient Ky changes little up to 500°K and then decreases at higher temperatures.With increasing impurity concentrations the value of $ σ_{i} $ increases, Ky remaining almost unchanged. © Consultants Bureau 1976 |
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N.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Effect of structural factors on the yield strength of beryllium</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1976</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">© Consultants Bureau 1976</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Conclusions The coefficients of the Hall—Petch equation are determined in relation to the percentage of resistance to basal and prismatic slip in the flow stress of polycrystalline beryllium.With increasing testing temperatures the variation of $ σ_{i} $ is similar to the variation of the yield strength; coefficient Ky changes little up to 500°K and then decreases at higher temperatures.With increasing impurity concentrations the value of $ σ_{i} $ increases, Ky remaining almost unchanged.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Yield Strength</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Structural Factor</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Flow Stress</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Testing Temperature</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Beryllium</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Papirov, I. 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