R. Marjunus, Yusril Al Fath, Y. Yulianti, W. Widanarto
Chemical reactions simulation in detecting hydrogen gas (H2) on Pt80Au14Ti6 sensor surface based on work function change (Δɸ) has been conducted. The simulation result is compared with laboratory results of detecting H2 gas. Three chemical reactions contained three coverages, H coverage (θH), O coverage (θO), and H2O coverage (θH2O). The simulation was run using MATLAB. This research can find the reaction parameter values such as the Arrhenius coefficient of H2O forming reaction on Pt (υf3Pt), H2O forming reaction on Au (υf3Au), i.e., H2O dissociation on Au (υf3Au ), O2 desorption on Ti (υd2Ti), H2O forming reaction on Ti (υf3Ti), and H2O dissociation on Ti (υf3Ti), i.e., 7.5×1014 s–1, 9.85×1015 s–1, 3.25×1015 s–1, 7.11×1015 s–1, 3.425×1015 s–1 and 2.725×1015 s–1, respectively. The simulation results also have the same trend as the laboratory results. However, the contact potential difference (CPD) simulation result, i.e., –240 mV, is not the same as the laboratory result, (–297± 9) mV. In addition, this simulation also obtained approximation coverage for atoms/molecules on PT80Au14Ti6 surface, i.e., θH = 0.665154 Mono Layer (ML); θO = 1.5621× 10–6 ML; and θH2O = 5.41676 ×10–5 ML.
{"title":"Simulation of Pt80Au14Ti6 Work Function Change-Based Sensor of H2 Gas","authors":"R. Marjunus, Yusril Al Fath, Y. Yulianti, W. Widanarto","doi":"10.21315/jps2022.33.3.4","DOIUrl":"https://doi.org/10.21315/jps2022.33.3.4","url":null,"abstract":"Chemical reactions simulation in detecting hydrogen gas (H2) on Pt80Au14Ti6 sensor surface based on work function change (Δɸ) has been conducted. The simulation result is compared with laboratory results of detecting H2 gas. Three chemical reactions contained three coverages, H coverage (θH), O coverage (θO), and H2O coverage (θH2O). The simulation was run using MATLAB. This research can find the reaction parameter values such as the Arrhenius coefficient of H2O forming reaction on Pt (υf3Pt), H2O forming reaction on Au (υf3Au), i.e., H2O dissociation on Au (υf3Au ), O2 desorption on Ti (υd2Ti), H2O forming reaction on Ti (υf3Ti), and H2O dissociation on Ti (υf3Ti), i.e., 7.5×1014 s–1, 9.85×1015 s–1, 3.25×1015 s–1, 7.11×1015 s–1, 3.425×1015 s–1 and 2.725×1015 s–1, respectively. The simulation results also have the same trend as the laboratory results. However, the contact potential difference (CPD) simulation result, i.e., –240 mV, is not the same as the laboratory result, (–297± 9) mV. In addition, this simulation also obtained approximation coverage for atoms/molecules on PT80Au14Ti6 surface, i.e., θH = 0.665154 Mono Layer (ML); θO = 1.5621× 10–6 ML; and θH2O = 5.41676 ×10–5 ML.","PeriodicalId":16757,"journal":{"name":"Journal of Physical Science","volume":"27 1","pages":""},"PeriodicalIF":0.7,"publicationDate":"2022-11-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"72510220","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
K. E. H. Ku Ishak, S. F. Saiyid Hashim, Khairun Azizi Mohd Azizli, S. Palaniandy, H. Hussin
High quartz content in clay substantially impacts the grinding of raw mix, quality of clinker and final cement produced. The presence of quartz requires very fine grinding and a long sintering time to react significantly, all of which are very expensive. This study assessed an extensive plant sample which involved a vertical roller mill to determine the correlation between quartz content in clay to the 90 μm residue, feed rate, clinker microstructure and mill power. The characterisation study performed on raw materials revealed three clay categories based on quartz content, namely low, normal and high quartz at (42.4%–48.8%), (57.1%–64.9%) and (81.5%–89.3%), respectively. The grinding test showed an increment of 90 μm residue for high-quartz clay. Meanwhile, high, medium and low feed rates generated the most coarse, coarse and fine products, respectively. Based on the distribution curve of mill products, high quartz content in clay significantly reduced the particles passing percentage. Coarser particles were observed to be present in mill products for the high-quartz category compared to the low-quartz clay and normal-quartz clay, signifying inadequate size reduction for the high-quartz clay in the vertical roller miller. The power consumption was higher (7.2 kWh/t–9.0 kWh/t) for grinding raw mixes that contained high-quartz clay than low-quartz clay. This study provided a significant relationship between grindability and the amount of quartz content in clay with the purpose of optimising the grinding process when dealing with high-quartz content in clay.
{"title":"Effect of Quartz in Clay on Grindability of Raw Mixes for Cement Production","authors":"K. E. H. Ku Ishak, S. F. Saiyid Hashim, Khairun Azizi Mohd Azizli, S. Palaniandy, H. Hussin","doi":"10.21315/jps2022.33.2.3","DOIUrl":"https://doi.org/10.21315/jps2022.33.2.3","url":null,"abstract":"High quartz content in clay substantially impacts the grinding of raw mix, quality of clinker and final cement produced. The presence of quartz requires very fine grinding and a long sintering time to react significantly, all of which are very expensive. This study assessed an extensive plant sample which involved a vertical roller mill to determine the correlation between quartz content in clay to the 90 μm residue, feed rate, clinker microstructure and mill power. The characterisation study performed on raw materials revealed three clay categories based on quartz content, namely low, normal and high quartz at (42.4%–48.8%), (57.1%–64.9%) and (81.5%–89.3%), respectively. The grinding test showed an increment of 90 μm residue for high-quartz clay. Meanwhile, high, medium and low feed rates generated the most coarse, coarse and fine products, respectively. Based on the distribution curve of mill products, high quartz content in clay significantly reduced the particles passing percentage. Coarser particles were observed to be present in mill products for the high-quartz category compared to the low-quartz clay and normal-quartz clay, signifying inadequate size reduction for the high-quartz clay in the vertical roller miller. The power consumption was higher (7.2 kWh/t–9.0 kWh/t) for grinding raw mixes that contained high-quartz clay than low-quartz clay. This study provided a significant relationship between grindability and the amount of quartz content in clay with the purpose of optimising the grinding process when dealing with high-quartz content in clay.","PeriodicalId":16757,"journal":{"name":"Journal of Physical Science","volume":"56 1","pages":""},"PeriodicalIF":0.7,"publicationDate":"2022-08-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"78623595","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Emulsion liquid membrane (ELM) is a potential method for extracting ibuprofen (IBP) from aqueous solution. The concentrations of the carrier, surfactant and internal phases are important parameters to optimise the extraction efficiency of IBP. The Box-Behnken design (BBD) is used to optimise the main parameters of ELM, which are Aliquat 336 (A), Span 80 (B) and sodium carbonate, Na2CO3 (C). The responses were calculated using quadratic polynomial regression and the model suggests a significant result with the experimental data set, with the F-value and p-value calculated at 17.88% and 0.05%, respectively. Span 80 and Na2CO3 had a mutual interaction which was significant for the IBP extraction by ELM. At the optimised parameters, namely Aliquat 336 concentration (2 wt%), Span 80 concentration (4 wt%) and Na2CO3 concentration (0.1 M) resulted in 96.78% of IBP extraction.
{"title":"Optimisation of Ibuprofen Extraction by Emulsion Liquid Membrane Using Box-Behnken Design","authors":"Mohd Hazarel Zairy Mohd Harun, A. Ahmad","doi":"10.21315/jps2022.33.2.6","DOIUrl":"https://doi.org/10.21315/jps2022.33.2.6","url":null,"abstract":"Emulsion liquid membrane (ELM) is a potential method for extracting ibuprofen (IBP) from aqueous solution. The concentrations of the carrier, surfactant and internal phases are important parameters to optimise the extraction efficiency of IBP. The Box-Behnken design (BBD) is used to optimise the main parameters of ELM, which are Aliquat 336 (A), Span 80 (B) and sodium carbonate, Na2CO3 (C). The responses were calculated using quadratic polynomial regression and the model suggests a significant result with the experimental data set, with the F-value and p-value calculated at 17.88% and 0.05%, respectively. Span 80 and Na2CO3 had a mutual interaction which was significant for the IBP extraction by ELM. At the optimised parameters, namely Aliquat 336 concentration (2 wt%), Span 80 concentration (4 wt%) and Na2CO3 concentration (0.1 M) resulted in 96.78% of IBP extraction.","PeriodicalId":16757,"journal":{"name":"Journal of Physical Science","volume":"15 1","pages":""},"PeriodicalIF":0.7,"publicationDate":"2022-08-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"75824758","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Hamisah Ismail, Z. Zainuddin, H. Mohamad, Muhammad Azmi Abdul Hamid
Maghemite (γ-Fe2O3) nanoparticles were synthesised using the coprecipitation method, with different concentrations (5 M, 10 M, 11 M, 12 M and 13.4 M) of sodium hydroxide (NaOH) as the precipitation agent. The resulting powder was characterised using x-ray diffraction (XRD), vibrating sample magnetometer (VSM), and transmission electron microscope (TEM). All characterisations were performed at room temperature. The XRD results showed that the γ-Fe2O3 powder was in a single phase for samples synthesised using 11 M, 12 M and 13.4 M NaOH and the crystallite size ranged between 5.74 nm–6.42 nm. TEM observations and analysis showed that the particles were in a cubo-spheroidal shape and the mean physical size of the nanoparticles was between 8.52 nm and 8.59 nm. Hysteresis loop indicated that γ-Fe2O3 nanoparticles have superparamagnetic properties with an acceptable range of saturation magnetisation of 31.08 emu/g–48.88 emu/g and negligible coercivity value. MTT assay demonstrated that the γ-Fe2O3 nanoparticles exhibited biocompatibility with V79-4 cells at different dosages (1000 μg/mL–50 μg/mL) for 48 h. The results suggested that maghemite can be a valuable low-cost biomagnetic material in biomedical applications.
{"title":"Compatibility of Concentrated NaOH as a Precipitation Agent in the Synthesis of Maghemite (γ-Fe2O3) Nanoparticles via Co-precipitation Method","authors":"Hamisah Ismail, Z. Zainuddin, H. Mohamad, Muhammad Azmi Abdul Hamid","doi":"10.21315/jps2022.33.2.4","DOIUrl":"https://doi.org/10.21315/jps2022.33.2.4","url":null,"abstract":"Maghemite (γ-Fe2O3) nanoparticles were synthesised using the coprecipitation method, with different concentrations (5 M, 10 M, 11 M, 12 M and 13.4 M) of sodium hydroxide (NaOH) as the precipitation agent. The resulting powder was characterised using x-ray diffraction (XRD), vibrating sample magnetometer (VSM), and transmission electron microscope (TEM). All characterisations were performed at room temperature. The XRD results showed that the γ-Fe2O3 powder was in a single phase for samples synthesised using 11 M, 12 M and 13.4 M NaOH and the crystallite size ranged between 5.74 nm–6.42 nm. TEM observations and analysis showed that the particles were in a cubo-spheroidal shape and the mean physical size of the nanoparticles was between 8.52 nm and 8.59 nm. Hysteresis loop indicated that γ-Fe2O3 nanoparticles have superparamagnetic properties with an acceptable range of saturation magnetisation of 31.08 emu/g–48.88 emu/g and negligible coercivity value. MTT assay demonstrated that the γ-Fe2O3 nanoparticles exhibited biocompatibility with V79-4 cells at different dosages (1000 μg/mL–50 μg/mL) for 48 h. The results suggested that maghemite can be a valuable low-cost biomagnetic material in biomedical applications.","PeriodicalId":16757,"journal":{"name":"Journal of Physical Science","volume":"4 1","pages":""},"PeriodicalIF":0.7,"publicationDate":"2022-08-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"87676449","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Bismuth ferrite (BFO) nanoparticles were synthesised by an environment-friendly process using the moringa oleifera leaf extract. The synthesised BFO nanoparticles were used as nanofiller to synthesise PVA-PANI-BFO polymernanocomposite membrane. Also, the PVA-PANI polymer membrane was synthesised for a comparative study purpose between PVA-PANI and PVA-PANI-BFO membranes. Both the polymer and polymer-nanocomposite membranes were synthesised by the solution cast technique. The Green synthesised BFO nanoparticles and the synthesised membranes were characterised by spectroscopic techniques such as X-ray diffraction (XRD), RAMAN and fourier-transform infrared spectroscopy (FTIR). XRD patterns confirm the BiFeO3 phase of the synthesised BFO nanoparticles, as well as the existence of PVA, PANI and BFO in the membrane. The Raman spectrum for the synthesised nanoparticles exhibits BFO characteristic bands. The bands of polyvinyl alcohol (PVA) and polyaniline (PANI) are also seen for the membranes. FTIR spectrum indicates some phytochemicals as the functional groups in the synthesised BFO nanoparticles. The surface structures of the synthesised membranes were characterised by field emission scanning electron microscopy (FESEM). Ionic conductivities of the synthesised membranes were calculated by estimating bulk resistance of them from Cole-Cole plots that were obtained with the help of an impedance spectrometer. The conductivities of the membranes change with the relative humidity (RH).
{"title":"Green Synthesised Bismuth Ferrite for PVA-PANI-BFO Polymer-Nanocomposite Membrane: Impacts on Ionic Conductivity with Variation of Relative Humidity","authors":"Diptarka Roy, Kamlesh Pandey, A. Yadav","doi":"10.21315/jps2022.33.2.2","DOIUrl":"https://doi.org/10.21315/jps2022.33.2.2","url":null,"abstract":"Bismuth ferrite (BFO) nanoparticles were synthesised by an environment-friendly process using the moringa oleifera leaf extract. The synthesised BFO nanoparticles were used as nanofiller to synthesise PVA-PANI-BFO polymernanocomposite membrane. Also, the PVA-PANI polymer membrane was synthesised for a comparative study purpose between PVA-PANI and PVA-PANI-BFO membranes. Both the polymer and polymer-nanocomposite membranes were synthesised by the solution cast technique. The Green synthesised BFO nanoparticles and the synthesised membranes were characterised by spectroscopic techniques such as X-ray diffraction (XRD), RAMAN and fourier-transform infrared spectroscopy (FTIR). XRD patterns confirm the BiFeO3 phase of the synthesised BFO nanoparticles, as well as the existence of PVA, PANI and BFO in the membrane. The Raman spectrum for the synthesised nanoparticles exhibits BFO characteristic bands. The bands of polyvinyl alcohol (PVA) and polyaniline (PANI) are also seen for the membranes. FTIR spectrum indicates some phytochemicals as the functional groups in the synthesised BFO nanoparticles. The surface structures of the synthesised membranes were characterised by field emission scanning electron microscopy (FESEM). Ionic conductivities of the synthesised membranes were calculated by estimating bulk resistance of them from Cole-Cole plots that were obtained with the help of an impedance spectrometer. The conductivities of the membranes change with the relative humidity (RH).","PeriodicalId":16757,"journal":{"name":"Journal of Physical Science","volume":"32 1","pages":""},"PeriodicalIF":0.7,"publicationDate":"2022-08-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"88150195","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The goal of this paper is to compare and investigate the radiation attenuation properties of Mundrabilla and NWA 7629 meteorites in terms of the photon, fast neutron and charged particles. The linear attenuation coefficients of Mundrabilla are higher than those of NWA 7629. The half value layers, tenth value layers and mean free paths of NWA 7629 are greater than those of Mundrabilla. The effective atomic number, effective electron density, equivalent atomic number and effective conductivity of the Mundrabilla are nearly constant between 0.015 MeV–15 MeV. Both the exposure build-up factors and energy absorption build-up factors are maximum at 0.8 MeV for Mundrabilla and NWA 7629. The projected/ continuous-slowing-down approximation (CSDA) ranges for charged particles for NWA 7629 are higher than those of Mundrabilla. The fast neutron attenuation of Mundrabilla is better than those of NWA 7629. Consequently, it can be concluded that photon, fast neutron and charged particles attenuation capability of Mundrabilla are better than NWA 7629 due to the nickel content, higher density and higher content of iron.
{"title":"A Comparative Study on the Radiation Attenuation Properties of Iron and Stony Meteorites: A Case of Mundrabilla and NWA 7629 Meteorites","authors":"C. Eke","doi":"10.21315/aos2022.33.2.5","DOIUrl":"https://doi.org/10.21315/aos2022.33.2.5","url":null,"abstract":"The goal of this paper is to compare and investigate the radiation attenuation properties of Mundrabilla and NWA 7629 meteorites in terms of the photon, fast neutron and charged particles. The linear attenuation coefficients of Mundrabilla are higher than those of NWA 7629. The half value layers, tenth value layers and mean free paths of NWA 7629 are greater than those of Mundrabilla. The effective atomic number, effective electron density, equivalent atomic number and effective conductivity of the Mundrabilla are nearly constant between 0.015 MeV–15 MeV. Both the exposure build-up factors and energy absorption build-up factors are maximum at 0.8 MeV for Mundrabilla and NWA 7629. The projected/ continuous-slowing-down approximation (CSDA) ranges for charged particles for NWA 7629 are higher than those of Mundrabilla. The fast neutron attenuation of Mundrabilla is better than those of NWA 7629. Consequently, it can be concluded that photon, fast neutron and charged particles attenuation capability of Mundrabilla are better than NWA 7629 due to the nickel content, higher density and higher content of iron.","PeriodicalId":16757,"journal":{"name":"Journal of Physical Science","volume":"77 1","pages":""},"PeriodicalIF":0.7,"publicationDate":"2022-08-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"80017697","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The magnetic lens (magnetic field lens) uses a magnetic field rather than an equipotential plane. This work presents a modelling of the design of a focused magnetic lens. Its main purpose is to reveal the possibility of this lens to eliminate aberrations and to determine the extent of its potential to be included in the design of electron microscopes and electron beam melting systems. This work was accomplished by using COMSOL Multiphysics simulation software. The magnetic lens was tested to determine the possibility of its inclusion in electron microscopes by changing the bore radius from 1 to 4 step by step. The proposed mathematical model was proven as an excellent tool in electron optics.
{"title":"Performance and Analysis of a Designed Magnetic Lens for Microscopic Applications","authors":"Emad H. Ahmed, Adnan K. Hasan","doi":"10.21315/jps2022.33.2.8","DOIUrl":"https://doi.org/10.21315/jps2022.33.2.8","url":null,"abstract":"The magnetic lens (magnetic field lens) uses a magnetic field rather than an equipotential plane. This work presents a modelling of the design of a focused magnetic lens. Its main purpose is to reveal the possibility of this lens to eliminate aberrations and to determine the extent of its potential to be included in the design of electron microscopes and electron beam melting systems. This work was accomplished by using COMSOL Multiphysics simulation software. The magnetic lens was tested to determine the possibility of its inclusion in electron microscopes by changing the bore radius from 1 to 4 step by step. The proposed mathematical model was proven as an excellent tool in electron optics.","PeriodicalId":16757,"journal":{"name":"Journal of Physical Science","volume":"34 1","pages":""},"PeriodicalIF":0.7,"publicationDate":"2022-08-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"80568213","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
In this work, zinc oxide (ZnO) nanoballs were directly deposited on porous silicon (PS) substrates using RF magnetron sputtering method. The PS substrates were synthesised at room temperature via metal assisted chemical etching technique. The structural, surface morphological and cross-sectional properties of as prepared ZnO nanoballs were investigated by x-ray diffraction, Raman spectroscopy and field emission scanning electron microscopy techniques, respectively. The interaction of nitrogen dioxide (NO2 ) gas molecules with sensing layer and all sensing properties under lower detection limit (2 ppm–100 ppm) were studied in detail. The proposed ZnO nanoballs sensor chip exhibits high sensing response (29.2%) with fast response/recovery times (70 sec/96 sec) to 20 ppm NO2 in dry air at 250°C. Thus, the findings recommend the viability of ZnO nanoballs sensor as highly sensitive and selective NO2 gas sensor at moderate operating temperature regime.
{"title":"RF Sputtered ZnO Nanoballs on Porous Substrate for Highly Sensitive NO2 Gas Sensing Applications","authors":"Pankaj Varshney, Vinay Kumar, Pankaj R. Singh, Ramphal Sharma, Arvind Kumar","doi":"10.21315/jps2022.33.2.1","DOIUrl":"https://doi.org/10.21315/jps2022.33.2.1","url":null,"abstract":"In this work, zinc oxide (ZnO) nanoballs were directly deposited on porous silicon (PS) substrates using RF magnetron sputtering method. The PS substrates were synthesised at room temperature via metal assisted chemical etching technique. The structural, surface morphological and cross-sectional properties of as prepared ZnO nanoballs were investigated by x-ray diffraction, Raman spectroscopy and field emission scanning electron microscopy techniques, respectively. The interaction of nitrogen dioxide (NO2 ) gas molecules with sensing layer and all sensing properties under lower detection limit (2 ppm–100 ppm) were studied in detail. The proposed ZnO nanoballs sensor chip exhibits high sensing response (29.2%) with fast response/recovery times (70 sec/96 sec) to 20 ppm NO2 in dry air at 250°C. Thus, the findings recommend the viability of ZnO nanoballs sensor as highly sensitive and selective NO2 gas sensor at moderate operating temperature regime.","PeriodicalId":16757,"journal":{"name":"Journal of Physical Science","volume":"11 1","pages":""},"PeriodicalIF":0.7,"publicationDate":"2022-08-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"82975965","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
N. Rosli, German A. Islan, R. Hasham, Guillermo R. Castro, Azila Abdul Aziz
This research focused on the formulation of Ca2+ cross-linked alginate (Alg) gels containing Zingiber officinale oil extract (ZOE) loaded into a nanostructured lipid carrier (NLC). The NLC is intended to protect the Zingiber officinale oil against physical and chemical degradation during topical administration to sustain the drug release and reduce drug leakage during storage. The NLC was prepared using hot homogenisation and ultrasonication of glyceryl monostearate. Virgin coconut oil was used as the liquid lipid. The NLC-ZOE had a mean size diameter of 100 nm and a zeta potential value of −40 mV. The ZOE released from NLC followed the Korsmeyer- Peppas model case I (Fickian diffusion). The NLC-ZOE formulation was then incorporated into Alg. The gels were prepared via ionotropic gelation in the presence of calcium. Scanning electron microscopy (SEM) images of Alg films revealed successful intercalation of NLC within the Alg matrix. The in vitro ZOE release from NLC-ZOEAlg occurred in a sustained manner from the cross-linked Alg hydrogels compared to the free NLC. The profiles of NLC-ZOE released from the Alg films depended on the nanoparticles amount. The results demonstrated the importance of designing a local delivery system to entrap and control the release of the bioactive components of ZOE from within the Alg matrix. Ca2+ cross-linked Alg gels containing ZOE loaded into NLC was found to be suitable for topical delivery applications, as shown by the sustained release of ZOE from calcium cross-linked Alg films containing NLC that was demonstrated in this study.
{"title":"Incorporation of Nanoparticles Based on Zingiber Officinale Essential Oil into Alginate Films for Sustained Release","authors":"N. Rosli, German A. Islan, R. Hasham, Guillermo R. Castro, Azila Abdul Aziz","doi":"10.21315/jps2022.33.2.7","DOIUrl":"https://doi.org/10.21315/jps2022.33.2.7","url":null,"abstract":"This research focused on the formulation of Ca2+ cross-linked alginate (Alg) gels containing Zingiber officinale oil extract (ZOE) loaded into a nanostructured lipid carrier (NLC). The NLC is intended to protect the Zingiber officinale oil against physical and chemical degradation during topical administration to sustain the drug release and reduce drug leakage during storage. The NLC was prepared using hot homogenisation and ultrasonication of glyceryl monostearate. Virgin coconut oil was used as the liquid lipid. The NLC-ZOE had a mean size diameter of 100 nm and a zeta potential value of −40 mV. The ZOE released from NLC followed the Korsmeyer- Peppas model case I (Fickian diffusion). The NLC-ZOE formulation was then incorporated into Alg. The gels were prepared via ionotropic gelation in the presence of calcium. Scanning electron microscopy (SEM) images of Alg films revealed successful intercalation of NLC within the Alg matrix. The in vitro ZOE release from NLC-ZOEAlg occurred in a sustained manner from the cross-linked Alg hydrogels compared to the free NLC. The profiles of NLC-ZOE released from the Alg films depended on the nanoparticles amount. The results demonstrated the importance of designing a local delivery system to entrap and control the release of the bioactive components of ZOE from within the Alg matrix. Ca2+ cross-linked Alg gels containing ZOE loaded into NLC was found to be suitable for topical delivery applications, as shown by the sustained release of ZOE from calcium cross-linked Alg films containing NLC that was demonstrated in this study.","PeriodicalId":16757,"journal":{"name":"Journal of Physical Science","volume":"196 1","pages":""},"PeriodicalIF":0.7,"publicationDate":"2022-08-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"73449716","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Karn Sourprae, E. Kalkornsurapranee, N. Lehman, Arthittaya Chuaybamrung, A. Tuljittraporn, Y. Nakaramontri, A. Krainoi, J. Johns, L. Songtipya, N. Uthaipan
This research was conducted to study x-ray and gamma radiation shielding parameters such as mass attenuation coefficient, mean free path, half value layer, tenth value layer, effective atomic numbers, effective electron density for the xBi2O3-(95-x)B2O3-5BaO (where x = 20 mol%, 35 mol%, 50 mol%, and 70 mol%) glass systems with different molar composition. The studied ceramic specimens were denoted by BB20, BB35, BB50 and BB70 and their density values were 4.438 g/cm3, 5.973 g/cm3, 7.156 g/cm3, and 8.005 g/cm3, respectively. Radiation shielding parameters of the samples were investigated by using web based XCOM programme. The obtained results revealed that the highest mass attenuation coefficients were reported for BB70 sample, which has the highest Bi2O3 additive in its chemical structure. At 7 MeV photon energy, half value layer (HVL) values were reported as 5.7812 cm, 3.8065 cm, 2.8533 cm, and 2.2457 cm for BB20, BB35, BB50 and BB70, respectively. Therefore, it can be concluded that the present bismuth sesquioxide based glasses in the Bi2O3-B2O3-BaO glass system have a good quality in radiation protection purposes. Therefore, this glass system can be used as an alternative to conventional materials with the right molar compositon in its chemical formation.
{"title":"Leather-Like Material Based on Natural Rubber Composites","authors":"Karn Sourprae, E. Kalkornsurapranee, N. Lehman, Arthittaya Chuaybamrung, A. Tuljittraporn, Y. Nakaramontri, A. Krainoi, J. Johns, L. Songtipya, N. Uthaipan","doi":"10.21315/aos2022.33.1.5","DOIUrl":"https://doi.org/10.21315/aos2022.33.1.5","url":null,"abstract":"This research was conducted to study x-ray and gamma radiation shielding parameters such as mass attenuation coefficient, mean free path, half value layer, tenth value layer, effective atomic numbers, effective electron density for the xBi2O3-(95-x)B2O3-5BaO (where x = 20 mol%, 35 mol%, 50 mol%, and 70 mol%) glass systems with different molar composition. The studied ceramic specimens were denoted by BB20, BB35, BB50 and BB70 and their density values were 4.438 g/cm3, 5.973 g/cm3, 7.156 g/cm3, and 8.005 g/cm3, respectively. Radiation shielding parameters of the samples were investigated by using web based XCOM programme. The obtained results revealed that the highest mass attenuation coefficients were reported for BB70 sample, which has the highest Bi2O3 additive in its chemical structure. At 7 MeV photon energy, half value layer (HVL) values were reported as 5.7812 cm, 3.8065 cm, 2.8533 cm, and 2.2457 cm for BB20, BB35, BB50 and BB70, respectively. Therefore, it can be concluded that the present bismuth sesquioxide based glasses in the Bi2O3-B2O3-BaO glass system have a good quality in radiation protection purposes. Therefore, this glass system can be used as an alternative to conventional materials with the right molar compositon in its chemical formation.","PeriodicalId":16757,"journal":{"name":"Journal of Physical Science","volume":"107 1","pages":""},"PeriodicalIF":0.7,"publicationDate":"2022-04-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"88341506","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
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