Evaluation of Bioactive Borosilicate Added Ag Glasses in Terms of Radiation Shielding, Structural, Optical, and Electrical Properties
Abstract Bioactive borosilicate glasses are the most preferred and well-known glasses for orthopedic applications due to their excellent properties. However, some negative aspects of borosilicate glasses like low optical, structural, and electrical features restricted their use. Thus, to enhance the...
Ausführliche Beschreibung
Autor*in: |
Boodaghi Malidarre, Roya [verfasserIn] |
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E-Artikel |
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Sprache: |
Englisch |
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2022 |
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Anmerkung: |
© The Author(s), under exclusive licence to Springer Nature B.V. 2022 |
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Übergeordnetes Werk: |
Enthalten in: Silicon - Dordrecht : Springer Netherlands, 2009, 14(2022), 18 vom: 18. Mai, Seite 12371-12379 |
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Übergeordnetes Werk: |
volume:14 ; year:2022 ; number:18 ; day:18 ; month:05 ; pages:12371-12379 |
Links: |
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DOI / URN: |
10.1007/s12633-022-01925-y |
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Katalog-ID: |
SPR049034820 |
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520 | |a Abstract Bioactive borosilicate glasses are the most preferred and well-known glasses for orthopedic applications due to their excellent properties. However, some negative aspects of borosilicate glasses like low optical, structural, and electrical features restricted their use. Thus, to enhance the mentioned drawbacks, $ Ag_{2} $O with different ratios of x = 0, 2, 4, 6, 8, and 10 wt.% are added to the borosilicate glasses. The obtained results show that the Polaron radius ($ r_{p} $), Inter-nuclear distance ($ r_{i} $), and Field Strength will increase up to 4.8181 Å, 11.9570 Å, and 2.0246 × $ 10^{16} $ $ cm^{− 2} $. The transmittance, absorbance, and absorbance coefficient (α) are highly improved from BS-Ag0 to BS-Ag10. Furthermore, the values of constraint number ($ N_{S} $) and cross-linking density (CD) show that the chosen samples’ rigidity increase from 11.080 to 11.090 and 9.080 to 9.090. In addition, at the low energy region sudden peaks are recorded in $ C_{eff} $ curves for BS-Ag2, BS-Ag4, BS-Ag6, BS-Ag8, and BS-Ag10 at E = 25.51 KeV which is related to the K-edge absorption of the Ag element. From the obtained results it can be concluded that $ Ag_{2} $O is responsible for the enhancement of the radiation shielding, structural, optical, and electrical features of the bioactive borosilicate glasses. | ||
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10.1007/s12633-022-01925-y doi (DE-627)SPR049034820 (SPR)s12633-022-01925-y-e DE-627 ger DE-627 rakwb eng Boodaghi Malidarre, Roya verfasserin aut Evaluation of Bioactive Borosilicate Added Ag Glasses in Terms of Radiation Shielding, Structural, Optical, and Electrical Properties 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Nature B.V. 2022 Abstract Bioactive borosilicate glasses are the most preferred and well-known glasses for orthopedic applications due to their excellent properties. However, some negative aspects of borosilicate glasses like low optical, structural, and electrical features restricted their use. Thus, to enhance the mentioned drawbacks, $ Ag_{2} $O with different ratios of x = 0, 2, 4, 6, 8, and 10 wt.% are added to the borosilicate glasses. The obtained results show that the Polaron radius ($ r_{p} $), Inter-nuclear distance ($ r_{i} $), and Field Strength will increase up to 4.8181 Å, 11.9570 Å, and 2.0246 × $ 10^{16} $ $ cm^{− 2} $. The transmittance, absorbance, and absorbance coefficient (α) are highly improved from BS-Ag0 to BS-Ag10. Furthermore, the values of constraint number ($ N_{S} $) and cross-linking density (CD) show that the chosen samples’ rigidity increase from 11.080 to 11.090 and 9.080 to 9.090. In addition, at the low energy region sudden peaks are recorded in $ C_{eff} $ curves for BS-Ag2, BS-Ag4, BS-Ag6, BS-Ag8, and BS-Ag10 at E = 25.51 KeV which is related to the K-edge absorption of the Ag element. From the obtained results it can be concluded that $ Ag_{2} $O is responsible for the enhancement of the radiation shielding, structural, optical, and electrical features of the bioactive borosilicate glasses. Borosilicate Biocomposites (dpeaa)DE-He213 Coordination number (CN) (dpeaa)DE-He213 Optical Properties (dpeaa)DE-He213 Field Strength (dpeaa)DE-He213 Relative dose distribution (RDD) (dpeaa)DE-He213 Electrical conductivity (dpeaa)DE-He213 Akkurt, Iskender aut Enthalten in Silicon Dordrecht : Springer Netherlands, 2009 14(2022), 18 vom: 18. Mai, Seite 12371-12379 (DE-627)598789545 (DE-600)2491562-2 1876-9918 nnns volume:14 year:2022 number:18 day:18 month:05 pages:12371-12379 https://dx.doi.org/10.1007/s12633-022-01925-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 14 2022 18 18 05 12371-12379 |
spelling |
10.1007/s12633-022-01925-y doi (DE-627)SPR049034820 (SPR)s12633-022-01925-y-e DE-627 ger DE-627 rakwb eng Boodaghi Malidarre, Roya verfasserin aut Evaluation of Bioactive Borosilicate Added Ag Glasses in Terms of Radiation Shielding, Structural, Optical, and Electrical Properties 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Nature B.V. 2022 Abstract Bioactive borosilicate glasses are the most preferred and well-known glasses for orthopedic applications due to their excellent properties. However, some negative aspects of borosilicate glasses like low optical, structural, and electrical features restricted their use. Thus, to enhance the mentioned drawbacks, $ Ag_{2} $O with different ratios of x = 0, 2, 4, 6, 8, and 10 wt.% are added to the borosilicate glasses. The obtained results show that the Polaron radius ($ r_{p} $), Inter-nuclear distance ($ r_{i} $), and Field Strength will increase up to 4.8181 Å, 11.9570 Å, and 2.0246 × $ 10^{16} $ $ cm^{− 2} $. The transmittance, absorbance, and absorbance coefficient (α) are highly improved from BS-Ag0 to BS-Ag10. Furthermore, the values of constraint number ($ N_{S} $) and cross-linking density (CD) show that the chosen samples’ rigidity increase from 11.080 to 11.090 and 9.080 to 9.090. In addition, at the low energy region sudden peaks are recorded in $ C_{eff} $ curves for BS-Ag2, BS-Ag4, BS-Ag6, BS-Ag8, and BS-Ag10 at E = 25.51 KeV which is related to the K-edge absorption of the Ag element. From the obtained results it can be concluded that $ Ag_{2} $O is responsible for the enhancement of the radiation shielding, structural, optical, and electrical features of the bioactive borosilicate glasses. Borosilicate Biocomposites (dpeaa)DE-He213 Coordination number (CN) (dpeaa)DE-He213 Optical Properties (dpeaa)DE-He213 Field Strength (dpeaa)DE-He213 Relative dose distribution (RDD) (dpeaa)DE-He213 Electrical conductivity (dpeaa)DE-He213 Akkurt, Iskender aut Enthalten in Silicon Dordrecht : Springer Netherlands, 2009 14(2022), 18 vom: 18. Mai, Seite 12371-12379 (DE-627)598789545 (DE-600)2491562-2 1876-9918 nnns volume:14 year:2022 number:18 day:18 month:05 pages:12371-12379 https://dx.doi.org/10.1007/s12633-022-01925-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 14 2022 18 18 05 12371-12379 |
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10.1007/s12633-022-01925-y doi (DE-627)SPR049034820 (SPR)s12633-022-01925-y-e DE-627 ger DE-627 rakwb eng Boodaghi Malidarre, Roya verfasserin aut Evaluation of Bioactive Borosilicate Added Ag Glasses in Terms of Radiation Shielding, Structural, Optical, and Electrical Properties 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Nature B.V. 2022 Abstract Bioactive borosilicate glasses are the most preferred and well-known glasses for orthopedic applications due to their excellent properties. However, some negative aspects of borosilicate glasses like low optical, structural, and electrical features restricted their use. Thus, to enhance the mentioned drawbacks, $ Ag_{2} $O with different ratios of x = 0, 2, 4, 6, 8, and 10 wt.% are added to the borosilicate glasses. The obtained results show that the Polaron radius ($ r_{p} $), Inter-nuclear distance ($ r_{i} $), and Field Strength will increase up to 4.8181 Å, 11.9570 Å, and 2.0246 × $ 10^{16} $ $ cm^{− 2} $. The transmittance, absorbance, and absorbance coefficient (α) are highly improved from BS-Ag0 to BS-Ag10. Furthermore, the values of constraint number ($ N_{S} $) and cross-linking density (CD) show that the chosen samples’ rigidity increase from 11.080 to 11.090 and 9.080 to 9.090. In addition, at the low energy region sudden peaks are recorded in $ C_{eff} $ curves for BS-Ag2, BS-Ag4, BS-Ag6, BS-Ag8, and BS-Ag10 at E = 25.51 KeV which is related to the K-edge absorption of the Ag element. From the obtained results it can be concluded that $ Ag_{2} $O is responsible for the enhancement of the radiation shielding, structural, optical, and electrical features of the bioactive borosilicate glasses. Borosilicate Biocomposites (dpeaa)DE-He213 Coordination number (CN) (dpeaa)DE-He213 Optical Properties (dpeaa)DE-He213 Field Strength (dpeaa)DE-He213 Relative dose distribution (RDD) (dpeaa)DE-He213 Electrical conductivity (dpeaa)DE-He213 Akkurt, Iskender aut Enthalten in Silicon Dordrecht : Springer Netherlands, 2009 14(2022), 18 vom: 18. Mai, Seite 12371-12379 (DE-627)598789545 (DE-600)2491562-2 1876-9918 nnns volume:14 year:2022 number:18 day:18 month:05 pages:12371-12379 https://dx.doi.org/10.1007/s12633-022-01925-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 14 2022 18 18 05 12371-12379 |
allfieldsGer |
10.1007/s12633-022-01925-y doi (DE-627)SPR049034820 (SPR)s12633-022-01925-y-e DE-627 ger DE-627 rakwb eng Boodaghi Malidarre, Roya verfasserin aut Evaluation of Bioactive Borosilicate Added Ag Glasses in Terms of Radiation Shielding, Structural, Optical, and Electrical Properties 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Nature B.V. 2022 Abstract Bioactive borosilicate glasses are the most preferred and well-known glasses for orthopedic applications due to their excellent properties. However, some negative aspects of borosilicate glasses like low optical, structural, and electrical features restricted their use. Thus, to enhance the mentioned drawbacks, $ Ag_{2} $O with different ratios of x = 0, 2, 4, 6, 8, and 10 wt.% are added to the borosilicate glasses. The obtained results show that the Polaron radius ($ r_{p} $), Inter-nuclear distance ($ r_{i} $), and Field Strength will increase up to 4.8181 Å, 11.9570 Å, and 2.0246 × $ 10^{16} $ $ cm^{− 2} $. The transmittance, absorbance, and absorbance coefficient (α) are highly improved from BS-Ag0 to BS-Ag10. Furthermore, the values of constraint number ($ N_{S} $) and cross-linking density (CD) show that the chosen samples’ rigidity increase from 11.080 to 11.090 and 9.080 to 9.090. In addition, at the low energy region sudden peaks are recorded in $ C_{eff} $ curves for BS-Ag2, BS-Ag4, BS-Ag6, BS-Ag8, and BS-Ag10 at E = 25.51 KeV which is related to the K-edge absorption of the Ag element. From the obtained results it can be concluded that $ Ag_{2} $O is responsible for the enhancement of the radiation shielding, structural, optical, and electrical features of the bioactive borosilicate glasses. Borosilicate Biocomposites (dpeaa)DE-He213 Coordination number (CN) (dpeaa)DE-He213 Optical Properties (dpeaa)DE-He213 Field Strength (dpeaa)DE-He213 Relative dose distribution (RDD) (dpeaa)DE-He213 Electrical conductivity (dpeaa)DE-He213 Akkurt, Iskender aut Enthalten in Silicon Dordrecht : Springer Netherlands, 2009 14(2022), 18 vom: 18. Mai, Seite 12371-12379 (DE-627)598789545 (DE-600)2491562-2 1876-9918 nnns volume:14 year:2022 number:18 day:18 month:05 pages:12371-12379 https://dx.doi.org/10.1007/s12633-022-01925-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 14 2022 18 18 05 12371-12379 |
allfieldsSound |
10.1007/s12633-022-01925-y doi (DE-627)SPR049034820 (SPR)s12633-022-01925-y-e DE-627 ger DE-627 rakwb eng Boodaghi Malidarre, Roya verfasserin aut Evaluation of Bioactive Borosilicate Added Ag Glasses in Terms of Radiation Shielding, Structural, Optical, and Electrical Properties 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Nature B.V. 2022 Abstract Bioactive borosilicate glasses are the most preferred and well-known glasses for orthopedic applications due to their excellent properties. However, some negative aspects of borosilicate glasses like low optical, structural, and electrical features restricted their use. Thus, to enhance the mentioned drawbacks, $ Ag_{2} $O with different ratios of x = 0, 2, 4, 6, 8, and 10 wt.% are added to the borosilicate glasses. The obtained results show that the Polaron radius ($ r_{p} $), Inter-nuclear distance ($ r_{i} $), and Field Strength will increase up to 4.8181 Å, 11.9570 Å, and 2.0246 × $ 10^{16} $ $ cm^{− 2} $. The transmittance, absorbance, and absorbance coefficient (α) are highly improved from BS-Ag0 to BS-Ag10. Furthermore, the values of constraint number ($ N_{S} $) and cross-linking density (CD) show that the chosen samples’ rigidity increase from 11.080 to 11.090 and 9.080 to 9.090. In addition, at the low energy region sudden peaks are recorded in $ C_{eff} $ curves for BS-Ag2, BS-Ag4, BS-Ag6, BS-Ag8, and BS-Ag10 at E = 25.51 KeV which is related to the K-edge absorption of the Ag element. From the obtained results it can be concluded that $ Ag_{2} $O is responsible for the enhancement of the radiation shielding, structural, optical, and electrical features of the bioactive borosilicate glasses. Borosilicate Biocomposites (dpeaa)DE-He213 Coordination number (CN) (dpeaa)DE-He213 Optical Properties (dpeaa)DE-He213 Field Strength (dpeaa)DE-He213 Relative dose distribution (RDD) (dpeaa)DE-He213 Electrical conductivity (dpeaa)DE-He213 Akkurt, Iskender aut Enthalten in Silicon Dordrecht : Springer Netherlands, 2009 14(2022), 18 vom: 18. Mai, Seite 12371-12379 (DE-627)598789545 (DE-600)2491562-2 1876-9918 nnns volume:14 year:2022 number:18 day:18 month:05 pages:12371-12379 https://dx.doi.org/10.1007/s12633-022-01925-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 14 2022 18 18 05 12371-12379 |
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However, some negative aspects of borosilicate glasses like low optical, structural, and electrical features restricted their use. Thus, to enhance the mentioned drawbacks, $ Ag_{2} $O with different ratios of x = 0, 2, 4, 6, 8, and 10 wt.% are added to the borosilicate glasses. The obtained results show that the Polaron radius ($ r_{p} $), Inter-nuclear distance ($ r_{i} $), and Field Strength will increase up to 4.8181 Å, 11.9570 Å, and 2.0246 × $ 10^{16} $ $ cm^{− 2} $. The transmittance, absorbance, and absorbance coefficient (α) are highly improved from BS-Ag0 to BS-Ag10. Furthermore, the values of constraint number ($ N_{S} $) and cross-linking density (CD) show that the chosen samples’ rigidity increase from 11.080 to 11.090 and 9.080 to 9.090. In addition, at the low energy region sudden peaks are recorded in $ C_{eff} $ curves for BS-Ag2, BS-Ag4, BS-Ag6, BS-Ag8, and BS-Ag10 at E = 25.51 KeV which is related to the K-edge absorption of the Ag element. 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Boodaghi Malidarre, Roya |
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Boodaghi Malidarre, Roya misc Borosilicate Biocomposites misc Coordination number (CN) misc Optical Properties misc Field Strength misc Relative dose distribution (RDD) misc Electrical conductivity Evaluation of Bioactive Borosilicate Added Ag Glasses in Terms of Radiation Shielding, Structural, Optical, and Electrical Properties |
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Evaluation of Bioactive Borosilicate Added Ag Glasses in Terms of Radiation Shielding, Structural, Optical, and Electrical Properties Borosilicate Biocomposites (dpeaa)DE-He213 Coordination number (CN) (dpeaa)DE-He213 Optical Properties (dpeaa)DE-He213 Field Strength (dpeaa)DE-He213 Relative dose distribution (RDD) (dpeaa)DE-He213 Electrical conductivity (dpeaa)DE-He213 |
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evaluation of bioactive borosilicate added ag glasses in terms of radiation shielding, structural, optical, and electrical properties |
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Evaluation of Bioactive Borosilicate Added Ag Glasses in Terms of Radiation Shielding, Structural, Optical, and Electrical Properties |
abstract |
Abstract Bioactive borosilicate glasses are the most preferred and well-known glasses for orthopedic applications due to their excellent properties. However, some negative aspects of borosilicate glasses like low optical, structural, and electrical features restricted their use. Thus, to enhance the mentioned drawbacks, $ Ag_{2} $O with different ratios of x = 0, 2, 4, 6, 8, and 10 wt.% are added to the borosilicate glasses. The obtained results show that the Polaron radius ($ r_{p} $), Inter-nuclear distance ($ r_{i} $), and Field Strength will increase up to 4.8181 Å, 11.9570 Å, and 2.0246 × $ 10^{16} $ $ cm^{− 2} $. The transmittance, absorbance, and absorbance coefficient (α) are highly improved from BS-Ag0 to BS-Ag10. Furthermore, the values of constraint number ($ N_{S} $) and cross-linking density (CD) show that the chosen samples’ rigidity increase from 11.080 to 11.090 and 9.080 to 9.090. In addition, at the low energy region sudden peaks are recorded in $ C_{eff} $ curves for BS-Ag2, BS-Ag4, BS-Ag6, BS-Ag8, and BS-Ag10 at E = 25.51 KeV which is related to the K-edge absorption of the Ag element. From the obtained results it can be concluded that $ Ag_{2} $O is responsible for the enhancement of the radiation shielding, structural, optical, and electrical features of the bioactive borosilicate glasses. © The Author(s), under exclusive licence to Springer Nature B.V. 2022 |
abstractGer |
Abstract Bioactive borosilicate glasses are the most preferred and well-known glasses for orthopedic applications due to their excellent properties. However, some negative aspects of borosilicate glasses like low optical, structural, and electrical features restricted their use. Thus, to enhance the mentioned drawbacks, $ Ag_{2} $O with different ratios of x = 0, 2, 4, 6, 8, and 10 wt.% are added to the borosilicate glasses. The obtained results show that the Polaron radius ($ r_{p} $), Inter-nuclear distance ($ r_{i} $), and Field Strength will increase up to 4.8181 Å, 11.9570 Å, and 2.0246 × $ 10^{16} $ $ cm^{− 2} $. The transmittance, absorbance, and absorbance coefficient (α) are highly improved from BS-Ag0 to BS-Ag10. Furthermore, the values of constraint number ($ N_{S} $) and cross-linking density (CD) show that the chosen samples’ rigidity increase from 11.080 to 11.090 and 9.080 to 9.090. In addition, at the low energy region sudden peaks are recorded in $ C_{eff} $ curves for BS-Ag2, BS-Ag4, BS-Ag6, BS-Ag8, and BS-Ag10 at E = 25.51 KeV which is related to the K-edge absorption of the Ag element. From the obtained results it can be concluded that $ Ag_{2} $O is responsible for the enhancement of the radiation shielding, structural, optical, and electrical features of the bioactive borosilicate glasses. © The Author(s), under exclusive licence to Springer Nature B.V. 2022 |
abstract_unstemmed |
Abstract Bioactive borosilicate glasses are the most preferred and well-known glasses for orthopedic applications due to their excellent properties. However, some negative aspects of borosilicate glasses like low optical, structural, and electrical features restricted their use. Thus, to enhance the mentioned drawbacks, $ Ag_{2} $O with different ratios of x = 0, 2, 4, 6, 8, and 10 wt.% are added to the borosilicate glasses. The obtained results show that the Polaron radius ($ r_{p} $), Inter-nuclear distance ($ r_{i} $), and Field Strength will increase up to 4.8181 Å, 11.9570 Å, and 2.0246 × $ 10^{16} $ $ cm^{− 2} $. The transmittance, absorbance, and absorbance coefficient (α) are highly improved from BS-Ag0 to BS-Ag10. Furthermore, the values of constraint number ($ N_{S} $) and cross-linking density (CD) show that the chosen samples’ rigidity increase from 11.080 to 11.090 and 9.080 to 9.090. In addition, at the low energy region sudden peaks are recorded in $ C_{eff} $ curves for BS-Ag2, BS-Ag4, BS-Ag6, BS-Ag8, and BS-Ag10 at E = 25.51 KeV which is related to the K-edge absorption of the Ag element. From the obtained results it can be concluded that $ Ag_{2} $O is responsible for the enhancement of the radiation shielding, structural, optical, and electrical features of the bioactive borosilicate glasses. © The Author(s), under exclusive licence to Springer Nature B.V. 2022 |
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title_short |
Evaluation of Bioactive Borosilicate Added Ag Glasses in Terms of Radiation Shielding, Structural, Optical, and Electrical Properties |
url |
https://dx.doi.org/10.1007/s12633-022-01925-y |
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|
score |
7.399585 |