2,536 research outputs found

    Topology optimized permanent magnet systems

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    Topology optimization of permanent magnet systems consisting of permanent magnets, high permeability iron and air is presented. An implementation of topology optimization for magnetostatics is discussed and three examples are considered. First, the Halbach cylinder is topology optimized with iron and an increase of 15% in magnetic efficiency is shown, albeit with an increase of 3.8 pp. in field inhomogeneity - a value compared to the inhomogeneity in a 16 segmented Halbach cylinder. Following this a topology optimized structure to concentrate a homogeneous field is shown to increase the magnitude of the field by 111% for the chosen dimensions. Finally, a permanent magnet with alternating high and low field regions is considered. Here a Λcool\Lambda_\mathrm{cool} figure of merit of 0.472 is reached, which is an increase of 100% compared to a previous optimized design.Comment: 10 pages, 10 figure

    The efficiency and the demagnetization field of a general Halbach cylinder

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    The maximum magnetic efficiency of a general multipole Halbach cylinder of order pp is found as function of pp. The efficiency is shown to decrease for increasing absolute value of pp. The optimal ratio between the inner and outer radius, i.e. the ratio resulting in the most efficient design, is also found as function of pp and is shown to tend towards smaller and smaller magnet sizes. Finally, the demagnetizing field in a general pp-Halbach cylinder is calculated, and it is shown that demagnetization is largest either at cos2pϕ=1\cos 2p\phi=1 or cos2pϕ=1\cos 2p\phi=-1. For the common case of a p=1p=1 Halbach cylinder the maximum values of the demagnetizing field is either at ϕ=0,π\phi = 0,\pi at the outer radius, where the field is always equal to the remanence, or at ϕ=±π/2\phi = \pm \pi/2 at the inner radius, where it is the magnitude of the field in the bore. Thus to avoid demagnetization the coercivity of the magnets must be larger than these values.Comment: 5 pages, 5 figure

    The lifetime cost of a magnetic refrigerator

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    The total cost of a 25 W average load magnetic refrigerator using commercial grade Gd is calculated using a numerical model. The price of magnetocaloric material, magnet material and cost of operation are considered, and all influence the total cost. The lowest combined total cost with a device lifetime of 15 years is found to be in the range \150$400dependingonthepriceofthemagnetocaloricandmagnetmaterial.Thecostofthemagnetislargest,followedcloselybythecostofoperation,whilethecostofthemagnetocaloricmaterialisalmostnegligible.Forthelowestcostdevice,theoptimalmagneticfieldisabout1.4T,theparticlesizeis0.23mm,thelengthoftheregeneratoris4050mmandtheutilizationisabout0.2,foralldevicelifetimesandmaterialandmagnetprices,whiletheoperatingfrequencyvaryasfunctionofdevicelifetime.TheconsideredperformancecharacteristicsarebasedontheperformanceofaconventionalA150-\$400 depending on the price of the magnetocaloric and magnet material. The cost of the magnet is largest, followed closely by the cost of operation, while the cost of the magnetocaloric material is almost negligible. For the lowest cost device, the optimal magnetic field is about 1.4 T, the particle size is 0.23 mm, the length of the regenerator is 40-50 mm and the utilization is about 0.2, for all device lifetimes and material and magnet prices, while the operating frequency vary as function of device lifetime. The considered performance characteristics are based on the performance of a conventional A^{+++}$ refrigeration unit. In a rough life time cost comparison between the magnetic refrigeration device and such a unit we find similar costs, the former being slightly cheaper, assuming the cost of the magnet can be recuperated at end of life.Comment: 17 pages, 17 figure

    Brillouin Cooling

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    We analyze how to exploit Brillouin scattering for the purpose of cooling opto-mechanical devices and present a quantum-mechanical theory for Brillouin cooling. Our analysis shows that significant cooling ratios can be obtained with standard experimental parameters. A further improvement of cooling efficiency is possible by increasing the dissipation of the optical anti-Stokes resonance.Comment: 4 pages 3 figure

    Phylogeny of Rosellinia capetribulensis sp. nov. and its allies (Xylariaceae)

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    A new Rosellinia species, R. capetribulensis isolated from Calamus sp. in Australia is described. R. capetribulensis is characterized by perithecia immersed within a carbonaceous stroma surrounded by subiculum-like hyphae, asci with large, barrel-shaped amyloid apical apparatus and large dark brown spores. Morphologically, R. capetribulensis appears to be similar to R. bunodes, R. markhamiae and R. megalospora. To gain further insights into the phylogeny of this new taxon we analyzed the ITS-5.8S rDNA using maximum parsimony and likelihood methods. In addition, a morphological dataset also was analyzed phylogenetically to investigate possible affinities. ITS rDNA based phylogenies reveal that R. capetribulensis is closely related to other Rosellinia species showing closest affinity to R. arcuata, R. necatrix and R. pepo. However, analysis of R. capetribulensis forms an unsupported branch sister to these taxa. Results from the morphological matrix indicate a close morphological affinity to members of Rosellinia subgenus Rosellinia. Despite that ITS rDNA and morphological analyses present difficulties in constructing a proper phylogenetic framework among Rosellinia and allied genera, there is sufficient evidence to support the establishment of the new taxon in the genus Rosellinia. The morphological similarities and differences between R. capetribulensis and allied genera such as Astrocystis and Entoleuca are also briefly discussed.published_or_final_versio

    Does A Food Exemption Lead to A Higher State Sales Tax Rate?

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