11 research outputs found

    Application of Hilbert-Huang Transform in the Field of Power Quality Events Analysis

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    Abstract—This paper deals with the analysis of PQ abnormalities using Hilbert–Huang Transform (HHT). HHT can be applied to both non-stationary as well as non-linear signals and it provides the energy-frequency-time representation of the signal. HHT is a time–frequency analysis method having low order of complexity and does not include the frequency resolution and time resolution fundamentals. So, it has the potential to outperform the frequency resolution and time resolution based methods. Several cases have been considered to present the efficiency of HHT. For the case study, various PQ abnormalities like voltage sag, swell and harmonics with sag are considered. These PQ abnormalities are subjected to HHT and the results are shown in the form of IMFs, instantaneous frequency, absolute value, phase and Hilbert Huang Spectrum. The results shows that the HHT performs better than the any other time resolution and frequency resolution based methods

    Investigating the Effects of Advanced Heat Treatment Techniques on the Mechanical Properties of Cast Components

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    This paper presents a comprehensive investigation into the effects of advanced heat treatment techniques on the mechanical properties of cast components. The study employs cutting-edge methodologies, including induction hardening, laser hardening, and cryogenic treatment, to modify the microstructure of various cast alloys. The primary focus is on the impact of these treatments on the hardness, tensile strength, ductility, and fatigue resistance of the materials. The experimental results reveal a significant enhancement in the mechanical properties of the treated components, with notable improvements in wear resistance and structural integrity. The findings also underscore the potential of these advanced heat treatment techniques in extending the service life of cast components, thereby contributing to the sustainability of mechanical systems. This research provides a novel perspective on the optimization of heat treatment processes, offering valuable insights for the design and manufacturing sectors. The outcomes of this study have far-reaching implications for industries that rely heavily on cast components, including automotive, aerospace, and heavy machinery, and pave the way for future research in this critical area of mechanical engineering

    Characterization of Microstructure and Mechanical Properties of Cast Materials using Advanced Techniques

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    In this study, we present an in-depth analysis of the microstructure and mechanical properties of cast materials, employing advanced characterization techniques. The research focuses on the utilization of Scanning Electron Microscopy (SEM), X-ray Diffraction (XRD), and Electron Backscatter Diffraction (EBSD) for microstructural analysis, alongside nanoindentation and tensile testing for mechanical property evaluation. The materials under investigation include a variety of industrially relevant cast alloys, providing a comprehensive understanding of their behavior under different casting conditions. Our findings reveal a strong correlation between the microstructural features, such as grain size, phase distribution, and defect morphology, and the mechanical properties, including hardness, yield strength, and ductility. The study also highlights the influence of casting parameters on these properties, offering insights for optimizing casting processes. The results of this research not only contribute to the existing body of knowledge on cast materials but also pave the way for the development of advanced materials with tailored properties for specific applications. This work underscores the importance of integrated microstructural and mechanical characterization in understanding and predicting the performance of cast materials, thereby aiding in their effective utilization in various industrial sectors

    Reciprocal regulation of human immunodeficiency virus-1 gene expression and replication by heat shock proteins 40 and 70

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    Cellular heat shock proteins (Hsps) are induced upon heat shock, UV irradiation and microbial or viral infection. They are also known to be involved in apoptosis and immune response in addition to their chaperone function. Although some literature exists regarding the role of Hsps in human immunodeficiency virus (HIV)-1 infection, a clear understanding of their role remains elusive. Previously, we have shown that Hsp40, a co-chaperone of Hsp70, interacts with HIV-1 negative regulatory factor (Nef) and is required for Nef-mediated increase in viral gene expression and replication. We now show that Hsp70 is also present in the Nef–Hsp40 complex reported earlier. Furthermore, Hsp70 inhibits viral gene expression and replication; however, Hsp40 can rescue this down regulation of viral gene expression induced by Hsp70. We also show that HIV-1 viral protein R is required for this inhibitory effect of Hsp70 on viral replication. Our data further show that Hsp40 is consistently up regulated in HIV-1 infection, whereas Hsp70 is down regulated after initial up regulation favoring viral replication. Finally, Hsp70 expression inhibits the phosphorylation of cyclin-dependent kinase 9 required for high-affinity binding of HIV-1 transactivator of transcription–positive transcription elongation factor b complex to transactivation response RNA, whereas Hsp40 seems to induce it. Thus, Hsp40 and Hsp70, both closely associated in their chaperone function, seem to act contrary to each other in regulating viral gene expression. It seems that Hsp70 favors the host by inhibiting viral replication, whereas Hsp40 works in favor of the virus by inducing its replication. Thus, differential expression of Hsp40 and Hsp70 reciprocally regulates viral gene expression and replication in HIV-1 infection

    Measurement of the branching fractions for Cabibbo-suppressed decays D+K+Kπ+π0D^{+}\to K^{+} K^{-}\pi^{+}\pi^{0} and D(s)+K+ππ+π0D_{(s)}^{+}\to K^{+}\pi^{-}\pi^{+}\pi^{0} at Belle

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    International audienceWe present measurements of the branching fractions for the singly Cabibbo-suppressed decays D+K+Kπ+π0D^+\to K^{+}K^{-}\pi^{+}\pi^{0} and Ds+K+ππ+π0D_s^{+}\to K^{+}\pi^{-}\pi^{+}\pi^{0}, and the doubly Cabibbo-suppressed decay D+K+ππ+π0D^{+}\to K^{+}\pi^{-}\pi^{+}\pi^{0}, based on 980 fb1{\rm fb}^{-1} of data recorded by the Belle experiment at the KEKB e+ee^{+}e^{-} collider. We measure these modes relative to the Cabibbo-favored modes D+Kπ+π+π0D^{+}\to K^{-}\pi^{+}\pi^{+}\pi^{0} and Ds+K+Kπ+π0D_s^{+}\to K^{+}K^{-}\pi^{+}\pi^{0}. Our results for the ratios of branching fractions are B(D+K+Kπ+π0)/B(D+Kπ+π+π0)=(11.32±0.13±0.26)%B(D^{+}\to K^{+}K^{-}\pi^{+}\pi^{0})/B(D^{+}\to K^{-}\pi^{+}\pi^{+}\pi^{0}) = (11.32 \pm 0.13 \pm 0.26)\%, B(D+K+ππ+π0)/B(D+Kπ+π+π0)=(1.68±0.11±0.03)%B(D^{+}\to K^{+}\pi^{-}\pi^{+}\pi^{0})/B(D^{+}\to K^{-}\pi^{+}\pi^{+}\pi^{0}) = (1.68 \pm 0.11\pm 0.03)\%, and B(Ds+K+ππ+π0)/B(Ds+K+Kπ+π0)=(17.13±0.62±0.51)%B(D_s^{+}\to K^{+}\pi^{-}\pi^{+}\pi^{0})/B(D_s^{+}\to K^{+}K^{-}\pi^{+}\pi^{0}) = (17.13 \pm 0.62 \pm 0.51)\%, where the uncertainties are statistical and systematic, respectively. The second value corresponds to (5.83±0.42)×tan4θC(5.83\pm 0.42)\times\tan^4\theta_C, where θC\theta_C is the Cabibbo angle; this value is larger than other measured ratios of branching fractions for a doubly Cabibbo-suppressed charm decay to a Cabibbo-favored decay. Multiplying these results by world average values for B(D+Kπ+π+π0)B(D^{+}\to K^{-}\pi^{+}\pi^{+}\pi^{0}) and B(Ds+K+Kπ+π0)B(D_s^{+}\to K^{+}K^{-}\pi^{+}\pi^{0}) yields B(D+K+Kπ+π0)=(7.08±0.08±0.16±0.20)×103B(D^{+}\to K^{+}K^{-}\pi^{+}\pi^{0})= (7.08\pm 0.08\pm 0.16\pm 0.20)\times10^{-3}, B(D+K+ππ+π0)=(1.05±0.07±0.02±0.03)×103B(D^{+}\to K^{+}\pi^{-}\pi^{+}\pi^{0})= (1.05\pm 0.07\pm 0.02\pm 0.03)\times10^{-3}, and B(Ds+K+ππ+π0)=(9.44±0.34±0.28±0.32)×103B(D_s^{+}\to K^{+}\pi^{-}\pi^{+}\pi^{0}) = (9.44\pm 0.34\pm 0.28\pm 0.32)\times10^{-3}, where the third uncertainty is due to the branching fraction of the normalization mode. The first two results are consistent with, but more precise than, the current world averages. The last result is the first measurement of this branching fraction

    Measurement of branching fractions of Λc+pKS0KS0\Lambda_c^+\to{}pK_S^0K_S^0 and Λc+pKS0η\Lambda_c^+\to{}pK_S^0\eta at Belle

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    We present a study of a singly Cabibbo-suppressed decay Λc+pKS0KS0\Lambda_c^+\to{}pK_S^0K_S^0 and a Cabibbo-favored decay Λc+pKS0η\Lambda_c^+\to{}pK_S^0\eta based on 980 fb1\rm fb^{-1} of data collected by the Belle detector, operating at the KEKB energy-asymmetric e+ee^+e^- collider. We measure their branching fractions relative to Λc+pKS0\Lambda_c^+\to{}pK_S^0: B(Λc+pKS0KS0)/B(Λc+pKS0)=(1.48±0.08±0.04)×102\mathcal{B}(\Lambda_c^+\to{}pK_S^0K_S^0)/\mathcal{B}(\Lambda_c^+\to{}pK_S^0)={(1.48 \pm 0.08 \pm 0.04)\times 10^{-2}} and B(Λc+pKS0η)/B(Λc+pKS0)=(2.73±0.06±0.13)×101\mathcal{B}(\Lambda_c^+\to{}pK_S^0\eta)/\mathcal{B}(\Lambda_c^+\to{}pK_S^0)={(2.73\pm 0.06\pm 0.13)\times 10^{-1}}. Combining with the world average B(Λc+pKS0)\mathcal{B}(\Lambda_c^+\to{}pK_S^0), we have the absolute branching fractions: B(Λc+pKS0KS0)=(2.35±0.12±0.07±0.12)×104\mathcal{B}(\Lambda_c^+\to{}pK_S^0K_S^0) = {(2.35\pm 0.12\pm 0.07 \pm 0.12 )\times 10^{-4}} and B(Λc+pKS0η)=(4.35±0.10±0.20±0.22)×103\mathcal{B}(\Lambda_c^+\to{}pK_S^0\eta) = {(4.35\pm 0.10\pm 0.20 \pm 0.22 )\times 10^{-3}}. The first and second uncertainties are statistical and systematic, respectively, while the third ones arise from the uncertainty on B(Λc+pKS0)\mathcal{B}(\Lambda_c^+\to{}pK_S^0). The mode Λc+pKS0KS0\Lambda_c^+\to{}pK_S^0K_S^0 is observed for the first time and has a statistical significance of > ⁣10σ>\!10\sigma. The branching fraction of Λc+pKS0η\Lambda_c^+\to{}pK_S^0\eta has been measured with a threefold improvement in precision over previous results and is found to be consistent with the world average
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