4,899 research outputs found

    Viscous to Inertial Crossover in Liquid Drop Coalescence

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    Using an electrical method and high-speed imaging we probe drop coalescence down to 10 ns after the drops touch. By varying the liquid viscosity over two decades, we conclude that at sufficiently low approach velocity where deformation is not present, the drops coalesce with an unexpectedly late crossover time between a regime dominated by viscous and one dominated by inertial effects. We argue that the late crossover, not accounted for in the theory, can be explained by an appropriate choice of length-scales present in the flow geometry.Comment: 4 pages, 4 figure

    Multiple transient memories in sheared suspensions: robustness, structure, and routes to plasticity

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    Multiple transient memories, originally discovered in charge-density-wave conductors, are a remarkable and initially counterintuitive example of how a system can store information about its driving. In this class of memories, a system can learn multiple driving inputs, nearly all of which are eventually forgotten despite their continual input. If sufficient noise is present, the system regains plasticity so that it can continue to learn new memories indefinitely. Recently, Keim & Nagel showed how multiple transient memories could be generalized to a generic driven disordered system with noise, giving as an example simulations of a simple model of a sheared non-Brownian suspension. Here, we further explore simulation models of suspensions under cyclic shear, focussing on three main themes: robustness, structure, and overdriving. We show that multiple transient memories are a robust feature independent of many details of the model. The steady-state spatial distribution of the particles is sensitive to the driving algorithm; nonetheless, the memory formation is independent of such a change in particle correlations. Finally, we demonstrate that overdriving provides another means for controlling memory formation and retention

    Multiple transient memories in experiments on sheared non-Brownian suspensions

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    A system with multiple transient memories can remember a set of inputs but subsequently forgets almost all of them, even as they are continually applied. If noise is added, the system can store all memories indefinitely. The phenomenon has recently been predicted for cyclically sheared non-Brownian suspensions. Here we present experiments on such suspensions, finding behavior consistent with multiple transient memories and showing how memories can be stabilized by noise.Comment: 5 pages, 4 figure

    Design and Analysis of the BRAE Tractor Pull Tow Vehicle

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    This senior project discusses the design and analysis of a towing vehicle for the tractor pulling team and the BRAE department. This report examines different types of existing hand operated towing vehicles and their strengths and weaknesses and how they can be modified to design a custom tow vehicle for the BRAE department. The purpose of this report was to make transporting and handling of the modified pulling tractors in the BRAE department safer for the operator and bystanders

    A Nordic Anomaly: Examining the Establishment of an Anti-Immigrant Party in Sweden

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    This thesis examines the establishment of an anti-immigrant party (AIP) in Sweden. Until recently, Sweden was known as the Nordic anomaly with no AIP in spite of high levels of immigration and high rates of right-wing violence. This has now changed, and the AIP, Sweden Democrats, are rising to popularity in high speed. I examine the causes given for the anomaly up until 2006 and show that a change in these has since created a favorable environment for an AIP to become successful. First, socio-economic cleavages have become less salient through decreasing party loyalty and increasing numbers of party switchers. Second, the immigration issue has become more politicized. I account for other complementary explanations for a Swedish AIP formation and conclude that Sweden is no longer an anomaly in the landscape of European AIPs

    The inexorable resistance of inertia determines the initial regime of drop coalescence

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    Drop coalescence is central to diverse processes involving dispersions of drops in industrial, engineering and scientific realms. During coalescence, two drops first touch and then merge as the liquid neck connecting them grows from initially microscopic scales to a size comparable to the drop diameters. The curvature of the interface is infinite at the point where the drops first make contact, and the flows that ensue as the two drops coalesce are intimately coupled to this singularity in the dynamics. Conventionally, this process has been thought to have just two dynamical regimes: a viscous and an inertial regime with a crossover region between them. We use experiments and simulations to reveal that a third regime, one that describes the initial dynamics of coalescence for all drop viscosities, has been missed. An argument based on force balance allows the construction of a new coalescence phase diagram

    Unconventional antiferromagnetic correlations of the doped Haldane gap system Y2_2BaNi1x_{1-x}Znx_xO5_5

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    We make a new proposal to describe the very low temperature susceptibility of the doped Haldane gap compound Y2_2BaNi1x_{1-x}Znx_xO5_5. We propose a new mean field model relevant for this compound. The ground state of this mean field model is unconventional because antiferromagnetism coexists with random dimers. We present new susceptibility experiments at very low temperature. We obtain a Curie-Weiss susceptibility χ(T)C/(Θ+T)\chi(T) \sim C / (\Theta+T) as expected for antiferromagnetic correlations but we do not obtain a direct signature of antiferromagnetic long range order. We explain how to obtain the ``impurity'' susceptibility χimp(T)\chi_{imp}(T) by subtracting the Haldane gap contribution to the total susceptibility. In the temperature range [1 K, 300 K] the experimental data are well fitted by Tχimp(T)=Cimp(1+Timp/T)γT \chi_{imp}(T) = C_{imp} (1 + T_{imp}/T )^{-\gamma}. In the temperature range [100 mK, 1 K] the experimental data are well fitted by Tχimp(T)=Aln(T/Tc)T \chi_{imp}(T) = A \ln{(T/T_c)}, where TcT_c increases with xx. This fit suggests the existence of a finite N\'eel temperature which is however too small to be probed directly in our experiments. We also obtain a maximum in the temperature dependence of the ac-susceptibility χ(T)\chi'(T) which suggests the existence of antiferromagnetic correlations at very low temperature.Comment: 19 pages, 17 figures, revised version (minor modifications
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