1,665 research outputs found

    Environmental Liquid Effluents, A Novel Approach For Treatment Of Industrial Waste Water

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    Nutrient enrichment or eutrophication of aquatic ecosystems can cause an increase in algae and aquatic plants, loss of component species, and loss of ecosystem function. For these reasons, numerous studies were focused on nitrogen and phosphorus removal from wastewater streams. Most of these studies were based on biological processes and different combinations of anaerobic, aerobic, and anoxic zones such as Bardenpho, A2O, UCT, and their modifications. Hence phosphate recovery from sewage is in synergy with reducing other environmental impacts and making it a long term economic resource. The aim of the novel treatment process is to highlight on studies investigated for the nutrient removal performance using Chorella-vulgaris at different nitrogen and phosphorus concentrations. The effect of ammonia nitrogen and phosphorus concentration on removal of these nutrients from synthetic wastewater by algae Chorella-vulgaris in batch cultivation have been investigated in this study and kinetic coefficients were determined. It is observed that an effluent may contain specific nutrients valuable for recovery and this observation may lead to the idea or understanding of treating an effluent from industrial source as a useful resource instead of the general idea of treating the effluent as waste products, and in the same process losing money in terms of expenses on chemicals and energy. Treatment and discharge of effluents into the receiving streams should not be an issue that will be considered as usual because there are specified standards required by the legislation, in terms of the quality and characteristic of the effluent before it is discharged into the waterways

    On the Number of Solutions of Exponential Congruences

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    For a prime pp and an integer aZa \in \Z we obtain nontrivial upper bounds on the number of solutions to the congruence xxa(modp)x^x \equiv a \pmod p, 1xp11 \le x \le p-1. We use these estimates to estimate the number of solutions to the congruence xxyy(modp)x^x \equiv y^y \pmod p, 1x,yp11 \le x,y \le p-1, which is of cryptographic relevance

    Transport in the XX chain at zero temperature: Emergence of flat magnetization profiles

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    We study the connection between magnetization transport and magnetization profiles in zero-temperature XX chains. The time evolution of the transverse magnetization, m(x,t), is calculated using an inhomogeneous initial state that is the ground state at fixed magnetization but with m reversed from -m_0 for x0. In the long-time limit, the magnetization evolves into a scaling form m(x,t)=P(x/t) and the profile develops a flat part (m=P=0) in the |x/t|1/2 while it expands with the maximum velocity, c_0=1, for m_0->0. The states emerging in the scaling limit are compared to those of a homogeneous system where the same magnetization current is driven by a bulk field, and we find that the expectation values of various quantities (energy, occupation number in the fermionic representation) agree in the two systems.Comment: RevTex, 8 pages, 3 ps figure

    Magnetization distribution in the transverse Ising chain with energy flux

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    The zero-temperature transverse Ising chain carrying an energy flux j_E is studied with the aim of determining the nonequilibrium distribution functions, P(M_z) and P(M_x), of its transverse and longitudinal magnetizations, respectively. An exact calculation reveals that P(M_z) is a Gaussian both at j_E=0 and j_E not equal 0, and the width of the distribution decreases with increasing energy flux. The distribution of the order-parameter fluctuations, P(M_x), is evaluated numerically for spin-chains of up to 20 spins. For the equilibrium case (j_E=0), we find the expected Gaussian fluctuations away from the critical point while the critical order-parameter fluctuations are shown to be non-gaussian with a scaling function Phi(x)=Phi(M_x/)=P(M_x) strongly dependent on the boundary conditions. When j_E not equal 0, the system displays long-range, oscillating correlations but P(M_x) is a Gaussian nevertheless, and the width of the Gaussian decreases with increasing j_E. In particular, we find that, at critical transverse field, the width has a j_E^(-3/8) asymptotic in the j_E -> 0 limit.Comment: 8 pages, 5 ps figure

    Formation of Liesegang patterns: Simulations using a kinetic Ising model

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    A kinetic Ising model description of Liesegang phenomena is studied using Monte Carlo simulations. The model takes into account thermal fluctuations, contains noise in the chemical reactions, and its control parameters are experimentally accessible. We find that noisy, irregular precipitation takes place in dimension d=2 while, depending on the values of the control parameters, either irregular patterns or precipitation bands satisfying the regular spacing law emerge in d=3.Comment: 7 pages, 8 ps figures, RevTe

    AdS_4/CFT_3 Construction from Collective Fields

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    We pursue the construction of higher-spin theory in AdS_4 from CFT_3 of the O(N) vector model in terms of canonical collective fields. In null plane quantization an exact map is established between the two spaces. The coordinates of the AdS_4 space-time are generated from the collective coordinates of the bi-local field. This, in the light cone gauge, provides an exact one to one reconstruction of bulk AdS_4 space-time and higher-spin fields.Comment: 17 pages, no figures; v2: references added; v3: minor change

    Matrix Model Maps and Reconstruction of AdS SUGRA Interactions

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    We consider the question of reconstructing (cubic) SUGRA interactions in AdS/CFT. The method we introduce is based on the matrix model maps (MMP) which were previously successfully employed at the linearized level. The strategy is to start with the map for 1/2 BPS configurations which is exactly known (to all orders) in the hamiltonian framework. We then use the extension of the matrix model map with the corresponding Ward identities to completely specify the interaction. A central point in this construction is the non-vanishing of off-shell interactions (even for highest-weight states).Comment: 28 page

    Non-Gaussian Resistance Noise near Electrical Breakdown in Granular Materials

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    The distribution of resistance fluctuations of conducting thin films with granular structure near electrical breakdown is studied by numerical simulations. The film is modeled as a resistor network in a steady state determined by the competition between two biased processes, breaking and recovery. Systems of different sizes and with different levels of internal disorder are considered. Sharp deviations from a Gaussian distribution are found near breakdown and the effect increases with the degree of internal disorder. However, we show that in general this non-Gaussianity is related to the finite size of the system and vanishes in the large size limit. Nevertheless, near the critical point of the conductor-insulator transition, deviations from Gaussianity persist when the size is increased and the distribution of resistance fluctuations is well fitted by the universal Bramwell-Holdsworth-Pinton distribution.Comment: 8 pages, 6 figures; accepted for publication on Physica

    Probability distribution of magnetization in the one-dimensional Ising model: Effects of boundary conditions

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    Finite-size scaling functions are investigated both for the mean-square magnetization fluctuations and for the probability distribution of the magnetization in the one-dimensional Ising model. The scaling functions are evaluated in the limit of the temperature going to zero (T -> 0), the size of the system going to infinity (N -> oo) while N[1-tanh(J/k_BT)] is kept finite (J being the nearest neighbor coupling). Exact calculations using various boundary conditions (periodic, antiperiodic, free, block) demonstrate explicitly how the scaling functions depend on the boundary conditions. We also show that the block (small part of a large system) magnetization distribution results are identical to those obtained for free boundary conditions.Comment: 8 pages, 5 figure
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