Environmental and Waste Management in Iron and Steel Industry

The Indian Iron and Steel scenario has changed considerably after the announcement of Government Policy on de-control and liberalization. Several new entrepreneurs have entered the steel industry. It is heartening to see that the steel industry is set to carve a niche for itself in the domestic and foreign market. The rapid progress of steel industry has aggravated environmental and waste management problems. This has led to increasing pressure from Government and the public to speed up action plan for effective industrial waste management. The waste management in steel industry is an emerging complex issue and can be implemented after regulating through monitoring, analysis, legalization , addition of infra-structural facilities for enforcement, waste auditing , change of process technology etc. The paper reviews current knowledge of waste management in Indian Steel Industry, approaches to environmental improvement and examines various options to environmental management plan keeping in view of the importance of sustainable endurance of environment and other natural resources

Environmental and waste management in iron and steel industry

The Indian Iron and Steel scenario has changed considerably after the announcement of Government Policy on de-control and liberalization. Several new entrepreneurs have entered the steel industry. It is heartening to see that the steel industry is set to carve a niche for itself in the domestic and foreign market. The rapid progress of steel industry has aggravated environmental and waste management problems. This has led to increasing pressurefrom Government and the public to speed up action plan for effective industrial waste management. The waste management in steel industry is an emerging complex issue and can be implemented after regulating through monitoring, analysis, legalization, addition of infra-structural facilities for enforcement, waste auditing, change of process technology etc. The paper reviews current knowledge of waste management in Indian Steel Industry, approaches to environmental improvement and examines various options to environmental man-agement plan keeping in view of the importance of sustainable endurance of environment and other natural resources

Role of CA 125 in predicting pathological response and recurrence in advanced stage non mucinous epithelial ovarian cancer

Background: Ovarian cancer is the most common gynaecological malignancy. Neo adjuvant chemotherapy (NAC) followed by interval cytoreduction is proven to be non-inferior to primary debulking surgery in advanced stage epithelial ovarian cancers (EOC). The data about patterns of reduction of CA125, its cut off value to predict chemotherapy response and recurrence in patients who receive NAC is heterogeneous with varying cut offs. This study aims to evaluate the role of CA125 as a predictive marker of pathological response and recurrence in cases of advanced EOC and to determine cut off for the same.Methods: This is a prospective study conducted in department of medical oncology, from December 2019 to May 2021. Patients of advanced stage EOC who are on NAC with carboplatin and paclitaxel combination were included (n=33). CA125 values before treatment, after each cycle of chemotherapy, post-surgery, during the course of adjuvant chemotherapy and every 2 months post treatment were noted. As the patient undergoes interval cytoreduction, histopathology reports were followed for chemotherapy response score (CRS). Imaging was done to detect recurrence during follow up, if CA 125 value increases.Results: The level of CA125 after third cycle of NAC showed significant correlation with chemotherapy response score and DFS in all the patients who were operable at the end of NAC. Patients with normal CA125 value (i.e. <35 U/ml) post 3 cycles chemotherapy had increased chance of having CRS 3 and longer DFS in patients with high grade serous carcinoma. Decline in CA125 value to less than 10 IU/ml post interval cytoreduction also correlates with DFS.Conclusions: Our study shows that CA125 levels before cytoreductive surgery predicts CRS and DFS of women undergoing NAC for advanced stage EOC

Active Vibration Control of a Smart Cantilever Beam on General Purpose Operating System

All mechanical systems suffer from undesirable vibrations during their operations. Their occurrence is uncontrollable as it depends on various factors. However, for efficient operation of the system, these vibrations have to be controlled within the specified limits. Light weight, rapid and multi-mode control of the vibrating structure is possible by the use of piezoelectric sensors and actuators and feedback control algorithms. In this paper, direct output feedback based active vibration control has been implemented on a cantilever beam using Lead Zirconate-Titanate (PZT) sensors and actuators. Three PZT patches were used, one as the sensor, one as the exciter providing the forced vibrations and the third acting as the actuator that provides an equal but opposite phase vibration/force signal to that of sensed so as to damp out the vibrations. The designed algorithm is implemented on Lab VIEW 2010 on Windows 7 Platform.Defence Science Journal, 2013, 63(4), pp.413-417, DOI:http://dx.doi.org/10.14429/dsj.63.486

Observation of charge-dependent azimuthal correlations and possible local strong parity violation in heavy ion collisions

Parity-odd domains, corresponding to non-trivial topological solutions of the QCD vacuum, might be created during relativistic heavy-ion collisions. These domains are predicted to lead to charge separation of quarks along the orbital momentum of the system created in non-central collisions. To study this effect, we investigate a three particle mixed harmonics azimuthal correlator which is a \P-even observable, but directly sensitive to the charge separation effect. We report measurements of this observable using the STAR detector in Au+Au and Cu+Cu collisions at $\sqrt{s_{NN}}$=200 and 62~GeV. The results are presented as a function of collision centrality, particle separation in rapidity, and particle transverse momentum. A signal consistent with several of the theoretical expectations is detected in all four data sets. We compare our results to the predictions of existing event generators, and discuss in detail possible contributions from other effects that are not related to parity violation.Comment: 17 pages, 14 figures, as accepted for publication in Physical Review C

Longitudinal Spin Transfer to Λ\Lambda and Λˉ\bar{\Lambda} Hyperons in Polarized Proton-Proton Collisions at s\sqrt{s} = 200 GeV

The longitudinal spin transfer, $D_{LL}$, from high energy polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons has been measured for the first time in proton-proton collisions at $\sqrt{s} = 200 \mathrm{GeV}$ with the STAR detector at RHIC. The measurements cover pseudorapidity, $\eta$, in the range $|\eta| < 1.2$ and transverse momenta, $p_\mathrm{T}$, up to $4 \mathrm{GeV}/c$. The longitudinal spin transfer is found to be $D_{LL}= -0.03\pm 0.13(\mathrm{stat}) \pm 0.04(\mathrm{syst})$ for inclusive $\Lambda$ and $D_{LL} = -0.12 \pm 0.08(\mathrm{stat}) \pm 0.03(\mathrm{syst})$ for inclusive $\bar{\Lambda}$ hyperons with $= 0.5$ and $= 3.7 \mathrm{GeV}/c$. The dependence on $\eta$ and $p_\mathrm{T}$ is presented.Comment: 5 pages, 4 figure

System-Size Independence of Directed Flow Measured at the BNL Relativistic Heavy-Ion Collider

We measure directed flow (ν_1) for charged particles in Au+Au and Cu+Cu collisions at √S_(NN)=200 and 62.4 GeV, as a function of pseudorapidity (η), transverse momentum (p_t), and collision centrality, based on data from the STAR experiment. We find that the directed flow depends on the incident energy but, contrary to all available model implementations, not on the size of the colliding system at a given centrality. We extend the validity of the limiting fragmentation concept to ν_1 in different collision systems, and investigate possible explanations for the observed sign change in ν_1(p_t)

Measurements of ϕ\phi meson production in relativistic heavy-ion collisions at RHIC

We present results for the measurement of $\phi$ meson production via its charged kaon decay channel $\phi \to K^+K^-$ in Au+Au collisions at $\sqrt{s_{_{NN}}}=62.4$, 130, and 200 GeV, and in $p+p$ and $d$+Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV from the STAR experiment at the BNL Relativistic Heavy Ion Collider (RHIC). The midrapidity ($|y|<0.5$) $\phi$ meson transverse momentum ($p_{T}$) spectra in central Au+Au collisions are found to be well described by a single exponential distribution. On the other hand, the $p_{T}$ spectra from $p+p$, $d$+Au and peripheral Au+Au collisions show power-law tails at intermediate and high $p_{T}$ and are described better by Levy distributions. The constant $\phi/K^-$ yield ratio vs beam species, collision centrality and colliding energy is in contradiction with expectations from models having kaon coalescence as the dominant mechanism for $\phi$ production at RHIC. The $\Omega/\phi$ yield ratio as a function of $p_{T}$ is consistent with a model based on the recombination of thermal $s$ quarks up to $p_{T}\sim 4$ GeV/$c$, but disagrees at higher transverse momenta. The measured nuclear modification factor, $R_{dAu}$, for the $\phi$ meson increases above unity at intermediate $p_{T}$, similar to that for pions and protons, while $R_{AA}$ is suppressed due to the energy loss effect in central Au+Au collisions. Number of constituent quark scaling of both $R_{cp}$ and $v_{2}$ for the $\phi$ meson with respect to other hadrons in Au+Au collisions at $\sqrt{s_{_{NN}}}$=200 GeV at intermediate $p_{T}$ is observed. These observations support quark coalescence as being the dominant mechanism of hadronization in the intermediate $p_{T}$ region at RHIC.Comment: 22 pages, 21 figures, 4 table

Systematic Measurements of Identified Particle Spectra in pp, d+Au and Au+Au Collisions from STAR

Identified charged particle spectra of $\pi^{\pm}$, $K^{\pm}$, $p$ and \pbar at mid-rapidity ($|y|<0.1$) measured by the \dedx method in the STAR-TPC are reported for $pp$ and d+Au collisions at \snn = 200 GeV and for Au+Au collisions at 62.4 GeV, 130 GeV, and 200 GeV. ... [Shortened for arXiv list. Full abstract in manuscript.]Comment: 58 pages, 46 figures, 37 table

Spin alignment measurements of the K∗0(892)K^{*0}(892) and ϕ(1020)\phi(1020) vector mesons at RHIC

We present the first spin alignment measurements for the $K^{*0}(892)$ and $\phi(1020)$ vector mesons produced at mid-rapidity with transverse momenta up to 5 GeV/c at $\sqrt{s_{NN}}$ = 200 GeV at RHIC. The diagonal spin density matrix elements with respect to the reaction plane in Au+Au collisions are $\rho_{00}$ = 0.32 $\pm$ 0.04 (stat) $\pm$ 0.09 (syst) for the $K^{*0}$ ($0.8<p_T<5.0$ GeV/c) and $\rho_{00}$ = 0.34 $\pm$ 0.02 (stat) $\pm$ 0.03 (syst) for the $\phi$ ($0.4<p_T<5.0$ GeV/c), and are constant with transverse momentum and collision centrality. The data are consistent with the unpolarized expectation of 1/3 and thus no evidence is found for the transfer of the orbital angular momentum of the colliding system to the vector meson spins. Spin alignments for $K^{*0}$ and $\phi$ in Au+Au collisions were also measured with respect to the particle's production plane. The $\phi$ result, $\rho_{00}$ = 0.41 $\pm$ 0.02 (stat) $\pm$ 0.04 (syst), is consistent with that in p+p collisions, $\rho_{00}$ = 0.39 $\pm$ 0.03 (stat) $\pm$ 0.06 (syst), also measured in this work. The measurements thus constrain the possible size of polarization phenomena in the production dynamics of vector mesons.Comment: 7 pages, 4 figures. fig.1 updated; one more reference added, one typo corrected, published in PRC.77.06190