505 research outputs found

    Measuring device Patent

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    Expulsion and measuring device for determining quantity of liquid in tank under conditions of weightlessnes

    Financial Distress Predicted by Cash Flow and Leverage with Capital Intensity as Moderating

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    The level of financial distress is a condition where the company\u27s finances are in an unhealthy state or crisis. This study aims to examine the effect of cash flow and leverage in predicting the level of financial distress which is moderated by capital intensity at PT. Indah Karya (Persero). The research method used is descriptive verification with a quantitative approach. To assess this research, the 2013-2017 Quarterly Financial Report is used. The results showed that cash flows has a negative and significant influence in predicting the level of financial distress, leverage (debt to asset ratio) has a positive and insignificant influence in predicting the level of financial distress, capital intensity has a negative and insignificant effect in moderating the effect of cash flows on the level of financial difficulty and capital intensity has a positive and insignificant influence in moderating the influence of leverage in predicting the level of financial distress. Simultaneously cash flow and leverage in predicting the level of financial distress which is moderated by capital intensity together - have a significant effect on the condition of the level of financial distress of PT. Indah Karya (Persero). Another result found in this study is that the capital intensity variable in moderating leverage has the strongest influence in predicting the level of corporate financial distress which is seen by using an assessment of total assets to sales and debt to asset ratio. With these results, the company can use it as an early detection in the face of financial distress. Keywords: CashFlow, Leverage, Capital Intensity, Financial distres

    Harmonic Systems With Bulk Noises

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    We consider a harmonic chain in contact with thermal reservoirs at different temperatures and subject to bulk noises of different types: velocity flips or self-consistent reservoirs. While both systems have the same covariances in the nonequilibrium stationary state (NESS) the measures are very different. We study hydrodynamical scaling, large deviations, fluctuations, and long range correlations in both systems. Some of our results extend to higher dimensions

    Anomalous diffusion for a class of systems with two conserved quantities

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    We introduce a class of one dimensional deterministic models of energy-volume conserving interfaces. Numerical simulations show that these dynamics are genuinely super-diffusive. We then modify the dynamics by adding a conservative stochastic noise so that it becomes ergodic. System of conservation laws are derived as hydrodynamic limits of the modified dynamics. Numerical evidence shows these models are still super-diffusive. This is proven rigorously for harmonic potentials

    Conservative interacting particles system with anomalous rate of ergodicity

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    We analyze certain conservative interacting particle system and establish ergodicity of the system for a family of invariant measures. Furthermore, we show that convergence rate to equilibrium is exponential. This result is of interest because it presents counterexample to the standard assumption of physicists that conservative system implies polynomial rate of convergence.Comment: 16 pages; In the previous version there was a mistake in the proof of uniqueness of weak Leray solution. Uniqueness had been claimed in a space of solutions which was too large (see remark 2.6 for more details). Now the mistake is corrected by introducing a new class of moderate solutions (see definition 2.10) where we have both existence and uniquenes

    Localization Recall Precision (LRP): A New Performance Metric for Object Detection

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    Average precision (AP), the area under the recall-precision (RP) curve, is the standard performance measure for object detection. Despite its wide acceptance, it has a number of shortcomings, the most important of which are (i) the inability to distinguish very different RP curves, and (ii) the lack of directly measuring bounding box localization accuracy. In this paper, we propose 'Localization Recall Precision (LRP) Error', a new metric which we specifically designed for object detection. LRP Error is composed of three components related to localization, false negative (FN) rate and false positive (FP) rate. Based on LRP, we introduce the 'Optimal LRP', the minimum achievable LRP error representing the best achievable configuration of the detector in terms of recall-precision and the tightness of the boxes. In contrast to AP, which considers precisions over the entire recall domain, Optimal LRP determines the 'best' confidence score threshold for a class, which balances the trade-off between localization and recall-precision. In our experiments, we show that, for state-of-the-art object (SOTA) detectors, Optimal LRP provides richer and more discriminative information than AP. We also demonstrate that the best confidence score thresholds vary significantly among classes and detectors. Moreover, we present LRP results of a simple online video object detector which uses a SOTA still image object detector and show that the class-specific optimized thresholds increase the accuracy against the common approach of using a general threshold for all classes. At https://github.com/cancam/LRP we provide the source code that can compute LRP for the PASCAL VOC and MSCOCO datasets. Our source code can easily be adapted to other datasets as well.Comment: to appear in ECCV 201

    IMECE2009-12660 MECHANICAL DESIGN AND VIBRO-ACOUSTIC TESTING OF ULTRATHIN CARBON FOILS FOR A SPACECRAFT INSTRUMENT

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    ABSTRACT IBEX-Hi is an electrostatic analyzer spacecraft instrument designed to measure the energy and flux distribution of energetic neutral atoms (ENAs) emanating from the interaction zone between the Earth's solar system and the Milky Way galaxy. A key element to this electro-optic instrument is an array of fourteen carbon foils that are used to ionize the ENAs. The foils are comprised of an ultrathin (50-100Å thick) layer of carbon suspended across the surface of an electroformed Nickel wire screen, which in turn is held taught by a metal frame holder. The electroformed orthogonal screen has square wire elements, 12.7 m thick, with a pitch of 131.1 wires/cm. Each foil holder has an open aperture approximately 5 cm by 2.5 cm. Designing and implementing foil holders with such a large surface area has not been attempted for spaceflight in the past and has proven to be extremely challenging. The delicate carbon foils are subject to fatigue failure from the large acoustic and vibration loads that they will be exposed to during launch of the spacecraft. This paper describes the evolution of the foil holder design from previous space instrument applications to a flight-like IBEX-Hi prototype. Vibro-acoustic qualification tests of the IBEX-Hi prototype instrument and the resulting failure of several foils are summarized. This is followed by a discussion of iterative foil holder design modifications and laser vibrometer modal testing to support future fatigue failure analyses. The results of these activities indicate that there is no strong dependency of the natural frequencies or transmissibilities of the foils on the different foil holder and screen configurations. However, for all foil holder designs, the natural frequencies of the foils were observed to decrease noticeably from exposure to acoustic testing. These test results, when combined with foil holder assembly considerations, suggest that the welded frame and integrated screen designs should be incorporated into the architecture of the IBEX-Hi flight instrument. INTRODUCTION The IBEX-Hi spacecraft instrument, shown in As discussed in [1] and [2], the mechanical design of the IBEX-Hi instrument proved to be quite challenging. Harsh environmental conditions imposed by the IBEX mission, combined with the need for delicate, high precision, and stable mechanical features, required that detailed structural and thermal analyses be combined with extensive environmental testing to qualify the mechanical design. In references [1] and [2], the mechanical design, thermal and structural analyses, an

    On the Fibonacci universality classes in nonlinear fluctuating hydrodynamics

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    We present a lattice gas model that without fine tuning of parameters is expected to exhibit the so far elusive modified Kardar-Parisi-Zhang (KPZ) universality class. To this end, we review briefly how non-linear fluctuating hydrodynamics in one dimension predicts that all dynamical universality classes in its range of applicability belong to an infinite discrete family which we call Fibonacci family since their dynamical exponents are the Kepler ratios zi=Fi+1/Fiz_i = F_{i+1}/F_{i} of neighbouring Fibonacci numbers FiF_i, including diffusion (z2=2z_2=2), KPZ (z3=3/2z_3=3/2), and the limiting ratio which is the golden mean z∞=(1+5)/2z_\infty=(1+\sqrt{5})/2. Then we revisit the case of two conservation laws to which the modified KPZ model belongs. We also derive criteria on the macroscopic currents to lead to other non-KPZ universality classes.Comment: 17 page

    t1/3t^{1/3} Superdiffusivity of Finite-Range Asymmetric Exclusion Processes on Z\mathbb Z

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    We consider finite-range asymmetric exclusion processes on Z\mathbb Z with non-zero drift. The diffusivity D(t)D(t) is expected to be of O(t1/3){\mathcal O}(t^{1/3}). We prove that D(t)≄Ct1/3D(t)\ge Ct^{1/3} in the weak (Tauberian) sense that ∫0∞e−λttD(t)dt≄Cλ−7/3\int_0^\infty e^{-\lambda t}tD(t)dt \ge C\lambda^{-7/3} as λ→0\lambda\to 0. The proof employs the resolvent method to make a direct comparison with the totally asymmetric simple exclusion process, for which the result is a consequence of the scaling limit for the two-point function recently obtained by Ferrari and Spohn. In the nearest neighbor case, we show further that tD(t)tD(t) is monotone, and hence we can conclude that D(t)≄Ct1/3(log⁥t)−7/3D(t)\ge Ct^{1/3}(\log t)^{-7/3} in the usual sense.Comment: Version 3. Statement of Theorem 3 is correcte
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