Abstract:Gamma ray attenuation coefficients of metal matrix composites have been investigated. For this purpose, the linear attenuation coefficients of composites containing boron carbide (B 4 C) at different rates have been measured using a gamma spectrometer that contains a NaI(Tl) detector and MCA at 662, 1173 and 1332 keV, which are obtained from 137 Cs and 60 Co sources. The measured results were compared with the calculation obtained using computer code of XCOM for 1 keV-1 GeV gamma energies.
“…Furthermore, they are similar to the values reported for B4C Al metal matrix composites [7] at a gamma energy level of 661.7 keV. However, the linear attenuation coefficients of Al2O3.TiO2;mm and Al2O3.TiO2;nm are lower than those of Al-4% Cu/B4C metal matrix composites [6] and TiB2-reinforced B4C-SiC [10] The best HVL value of 3.57 cm obtained in this study is better than the results of [9], but significantly less than the values reported for some stainless and boron steels [8].…”
Section: Resultssupporting
confidence: 86%
“…The linear attenuation coefficients of Al2O3;mm and Al2O3;nm are similar to those of TiB2-reinforced B4C-silicon carbide composites [5] and spark plasmasintered B4C-Al [9]; however, they are higher than the values reported for h-BN and h-BN-TİB2 composites [4] and lower than those of Al-4% Cu/B4C metal matrix composites [6], B4C Al metal matrix composites [7], and some stainless and BSs steels [8] at 661.7 keV. At gamma energies of 1173.2 and 1332.5 keV, Al2O3;mm and Al2O3;nm samples have lower linear attenuation coefficients than Al-4% Cu/B4C metal matrix composites [6] and TiB2-reinforced B4C-SiC [10].…”
Section: Resultssupporting
confidence: 63%
“…The linear attenuation coefficients of Al2O3;mm and Al2O3;nm are similar to those of TiB2-reinforced B4C-silicon carbide composites [5] and spark plasmasintered B4C-Al [9]; however, they are higher than the values reported for h-BN and h-BN-TİB2 composites [4] and lower than those of Al-4% Cu/B4C metal matrix composites [6], B4C Al metal matrix composites [7], and some stainless and BSs steels [8] at 661.7 keV. At gamma energies of 1173.2 and 1332.5 keV, Al2O3;mm and Al2O3;nm samples have lower linear attenuation coefficients than Al-4% Cu/B4C metal matrix composites [6] and TiB2-reinforced B4C-SiC [10]. While the linear attenuation coefficient values of Al2O3.TiO2;mm and Al2O3.TiO2;nm are higher than those of h-BN and h-BN-TİB2 composites [4], TiB2-reinforced B4C-silicon carbide composites [5], and spark-plasma sintered B4C-Al [9], they are lower than the values reported for Al-4% Cu/B4C metal matrix composites [6], and some stainless and BSs steels [8].…”
Section: Resultssupporting
confidence: 63%
“…At gamma energies of 1173.2 and 1332.5 keV, Al2O3;mm and Al2O3;nm samples have lower linear attenuation coefficients than Al-4% Cu/B4C metal matrix composites [6] and TiB2-reinforced B4C-SiC [10]. While the linear attenuation coefficient values of Al2O3.TiO2;mm and Al2O3.TiO2;nm are higher than those of h-BN and h-BN-TİB2 composites [4], TiB2-reinforced B4C-silicon carbide composites [5], and spark-plasma sintered B4C-Al [9], they are lower than the values reported for Al-4% Cu/B4C metal matrix composites [6], and some stainless and BSs steels [8]. Furthermore, they are similar to the values reported for B4C Al metal matrix composites [7] at a gamma energy level of 661.7 keV.…”
Section: Resultsmentioning
confidence: 92%
“…The increasingly widespread usage of radioisotopes in recent years has created a radiation-protection problem, owing to which shielding solutions had to be developed. We conducted a literature search to obtain data on the radiation-attenuation properties of of some materials [1][2][3][4][5][6][7][8][9][10]. Bagheri et al examined the mass attenuation coefficients of silicate glasses containing different concentration of Bi2O3, PbO, and BaO using XCOM and XMuDat programs, in the energy range of 10 keV-10 MeV [1].…”
Abstract:In this study, micro and nanometers-sized powders of Al2O3 and Al2O3.TiO2 were prepared using a hydraulic cold press and their gamma-radiation shielding properties were assessed at photon energies of 661.7, 1173.2 and 1332.5 keV. A sample counting process was implemented using a gamma-ray spectrometer with a 3×3 NaI (Tl) detector and 13384-channel multichannel analyser. The results we obtained indicated that the gamma-shielding properties of the materials increased with TiO2 addition and also, the particle size found to be an important effect on the properties. The results were compared with each other and also compared with the results of similar studies reported in literature.
Al2O3 ve Al2O3.TiO2 Bileşiklerinin Gama Zayıflama Katsayıları Üzerine Bir ÇalışmaAnahtar kelimeler Gama ışını zayıflaması katsayıları, Al2O3, Al2O3.TiO2, NaI (Tl) detektor Özet: Bu çalışmada parçacık boyutları mikrometre ve nanometre düzeyinde olan toz halindeki Al2O3 ve Al2O3.TiO2 bileşikleri, soğuk hidrolik pres metodu kullanılarak deneye hazırlandı ve 661.7, 1173.2 ve 1332.5 keV foton enerjileri dikkate alınarak gama-radyasyonuna karşı zırhlama özellikleri incelendi. Örnekler için sayım işlemi 3×3 NaI (Tl) dedektörü ve 13384-kanalı olan çok kanallı gamaradyasyonu spektrometresi kullanılarak gerçekleştirildi. Elde edilen sonuçlardan, malzemelere TiO2 katkısının, malzemelerin gama zırhlama özelliklerini arttırmakta olduğu ve bu bulguya ilaveten malzemelerin parçacık boyutlarının da zırhlama özelliklerini etkilemekte olduğu anlaşıldı. Elde edilen sonuçlar kendi aralarında ve de literatürdeki mevcut benzer çalışmaların sonuçları ile kıyaslandı.
“…Furthermore, they are similar to the values reported for B4C Al metal matrix composites [7] at a gamma energy level of 661.7 keV. However, the linear attenuation coefficients of Al2O3.TiO2;mm and Al2O3.TiO2;nm are lower than those of Al-4% Cu/B4C metal matrix composites [6] and TiB2-reinforced B4C-SiC [10] The best HVL value of 3.57 cm obtained in this study is better than the results of [9], but significantly less than the values reported for some stainless and boron steels [8].…”
Section: Resultssupporting
confidence: 86%
“…The linear attenuation coefficients of Al2O3;mm and Al2O3;nm are similar to those of TiB2-reinforced B4C-silicon carbide composites [5] and spark plasmasintered B4C-Al [9]; however, they are higher than the values reported for h-BN and h-BN-TİB2 composites [4] and lower than those of Al-4% Cu/B4C metal matrix composites [6], B4C Al metal matrix composites [7], and some stainless and BSs steels [8] at 661.7 keV. At gamma energies of 1173.2 and 1332.5 keV, Al2O3;mm and Al2O3;nm samples have lower linear attenuation coefficients than Al-4% Cu/B4C metal matrix composites [6] and TiB2-reinforced B4C-SiC [10].…”
Section: Resultssupporting
confidence: 63%
“…The linear attenuation coefficients of Al2O3;mm and Al2O3;nm are similar to those of TiB2-reinforced B4C-silicon carbide composites [5] and spark plasmasintered B4C-Al [9]; however, they are higher than the values reported for h-BN and h-BN-TİB2 composites [4] and lower than those of Al-4% Cu/B4C metal matrix composites [6], B4C Al metal matrix composites [7], and some stainless and BSs steels [8] at 661.7 keV. At gamma energies of 1173.2 and 1332.5 keV, Al2O3;mm and Al2O3;nm samples have lower linear attenuation coefficients than Al-4% Cu/B4C metal matrix composites [6] and TiB2-reinforced B4C-SiC [10]. While the linear attenuation coefficient values of Al2O3.TiO2;mm and Al2O3.TiO2;nm are higher than those of h-BN and h-BN-TİB2 composites [4], TiB2-reinforced B4C-silicon carbide composites [5], and spark-plasma sintered B4C-Al [9], they are lower than the values reported for Al-4% Cu/B4C metal matrix composites [6], and some stainless and BSs steels [8].…”
Section: Resultssupporting
confidence: 63%
“…At gamma energies of 1173.2 and 1332.5 keV, Al2O3;mm and Al2O3;nm samples have lower linear attenuation coefficients than Al-4% Cu/B4C metal matrix composites [6] and TiB2-reinforced B4C-SiC [10]. While the linear attenuation coefficient values of Al2O3.TiO2;mm and Al2O3.TiO2;nm are higher than those of h-BN and h-BN-TİB2 composites [4], TiB2-reinforced B4C-silicon carbide composites [5], and spark-plasma sintered B4C-Al [9], they are lower than the values reported for Al-4% Cu/B4C metal matrix composites [6], and some stainless and BSs steels [8]. Furthermore, they are similar to the values reported for B4C Al metal matrix composites [7] at a gamma energy level of 661.7 keV.…”
Section: Resultsmentioning
confidence: 92%
“…The increasingly widespread usage of radioisotopes in recent years has created a radiation-protection problem, owing to which shielding solutions had to be developed. We conducted a literature search to obtain data on the radiation-attenuation properties of of some materials [1][2][3][4][5][6][7][8][9][10]. Bagheri et al examined the mass attenuation coefficients of silicate glasses containing different concentration of Bi2O3, PbO, and BaO using XCOM and XMuDat programs, in the energy range of 10 keV-10 MeV [1].…”
Abstract:In this study, micro and nanometers-sized powders of Al2O3 and Al2O3.TiO2 were prepared using a hydraulic cold press and their gamma-radiation shielding properties were assessed at photon energies of 661.7, 1173.2 and 1332.5 keV. A sample counting process was implemented using a gamma-ray spectrometer with a 3×3 NaI (Tl) detector and 13384-channel multichannel analyser. The results we obtained indicated that the gamma-shielding properties of the materials increased with TiO2 addition and also, the particle size found to be an important effect on the properties. The results were compared with each other and also compared with the results of similar studies reported in literature.
Al2O3 ve Al2O3.TiO2 Bileşiklerinin Gama Zayıflama Katsayıları Üzerine Bir ÇalışmaAnahtar kelimeler Gama ışını zayıflaması katsayıları, Al2O3, Al2O3.TiO2, NaI (Tl) detektor Özet: Bu çalışmada parçacık boyutları mikrometre ve nanometre düzeyinde olan toz halindeki Al2O3 ve Al2O3.TiO2 bileşikleri, soğuk hidrolik pres metodu kullanılarak deneye hazırlandı ve 661.7, 1173.2 ve 1332.5 keV foton enerjileri dikkate alınarak gama-radyasyonuna karşı zırhlama özellikleri incelendi. Örnekler için sayım işlemi 3×3 NaI (Tl) dedektörü ve 13384-kanalı olan çok kanallı gamaradyasyonu spektrometresi kullanılarak gerçekleştirildi. Elde edilen sonuçlardan, malzemelere TiO2 katkısının, malzemelerin gama zırhlama özelliklerini arttırmakta olduğu ve bu bulguya ilaveten malzemelerin parçacık boyutlarının da zırhlama özelliklerini etkilemekte olduğu anlaşıldı. Elde edilen sonuçlar kendi aralarında ve de literatürdeki mevcut benzer çalışmaların sonuçları ile kıyaslandı.
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