189,971 research outputs found
Interview with Charlie Rouse / interviewed by Felix Grant, November 21, 1979
No full textCharlie Rouse discusses his career with interviewer and radio host Felix Grant. Rouse is featured on excerpts from recordings selected by Grant.Made available in DSpace on 2012-10-09T17:42:40Z (GMT). No. of bitstreams: 2
rouse_charlie.rm: 11784497 bytes, checksum: 7fde547e79f00060485c177241d3f338 (MD5)
manifest.xml: 3419 bytes, checksum: 5578a8973808fc4431fcae438e4e3971 (MD5)Reflectory / P. Adams (04:39-07:08) -- Who's bossa now / B. Bailey (09:48-12:04) -- Let me go / F. Pauer (13:42-14:30)Charlie Rouse interviewed by Felix Grant on WMAL. Recorded November 21, 1979. Reproduction of radio interview produced at Washington, D.C. Station WMAL for broadcast on The Album Sound. Forms part of the Felix Grant Collection at the Felix E. Grant Jazz Archives. Original format: 1 sound tape reel (16 min.) : analog, 7 1/2 ips., full track mono; 7 in
Critical behaviour of the Rouse model for gelling polymers
No full textIt is shown that the traditionally accepted 'Rouse values' for the critical exponents at the gelation transition do not arise from the Rouse model for gelling polymers. The true critical behaviour of the Rouse model for gelling polymers is obtained from spectral properties of the connectivity matrix of the fractal clusters that are formed by the molecules. The required spectral properties are related to the return probability of a 'blind-ant' random walk on the critical percolating cluster. The resulting scaling relations express the critical exponents of the shear-stress-relaxation function, and hence those of the shear viscosity and of the first normal stress coefficient, in terms of the spectral dimension d(s) of the critical percolating cluster and the exponents or and tau of the cluster-size distribution
Catoptometridae Taylor, Messing and Rouse 2023, new family
No full textCatoptometridae Taylor, Messing and Rouse, 2023, new family <p> <b>Type genus:</b> <i>Catoptometra</i> AH Clark, 1908c</p> <p> <b>Diagnosis</b>: Himerometroidea lacking any aboral cirral spines; IBr2 syzygies extremely brittle. Adoral centrodorsal surface smooth, with no radial depressions or furrows. Distal margins of division series and arm brachials bearing strong spines.</p> <p> <b>Remarks</b>: This diagnosis is the same as for the genus <i>Catoptometra</i> (A. H. Clark, 1915 a, 1931, 1941; Hess & Messing, 2011).</p>Published as part of <i>Taylor, Kristian H., Rouse, Greg W. & Messing, Charles G., 2023, Phylogeny and taxonomy of Himerometroidea (Echinodermata: Crinoidea), pp. 149-164 in Zootaxa 5277 (1)</i> on page 160, DOI: 10.11646/zootaxa.5277.1.7, <a href="http://zenodo.org/record/7893112">http://zenodo.org/record/7893112</a>
rouse chocks
No full textrouse nThe 'Service' . . . is a piece of brin or canvas which was wrapped around the rope at the point where it passes through the "rouse chocks"DNE-cit [see other side for diagram](shown in diagram 1A and diagram No. 32) (see appendix) see other side for diagramG. M. Story FEB 1973 JH FEB 1973Used IUsed IUsed IReverse of card at R_1485
Introduction : Utopian Longing, Ludic Aesthetics, and Exchange
No full textEditor: Konstmuseet i Skövde/Skövde Art MuseumCo-Editors: Lars Kristensen & Rebecca Rouse at University of SkövdeAuthors: Thomas Oldrell, Rebecca Rouse, Lars Kristensen, Sharon Clark, Jack Hardiker, Hedvig Jalhed, Mattias Rylander, Kristoffer Åberg, David Hornwall, Katariina Poikela, WU Mingmin, Nea Landin, Gabriel Widing, Scott Cazan, Jamie Fawcus, Susanne Hansson, Anna Granath, Lisa Sjögren, Charlotta Grimfjord Cederblad, Erik Dahl & Claes SvenssonLudoKonst 2023 was carried out with support from Västra Götaland Region and it was a collaboration between the University of Skövde, Skövde Art Museum and Folkteatern Gothenburg.</p
Simulational Tests of the Rouse Model
No full textAn extensive review of literature simulations of quiescent polymer melts is given, considering results that test aspects of the Rouse model in the melt. We focus on Rouse model predictions for the mean-square amplitudes ⟨(Xp(0))2⟩ and time correlation functions ⟨Xp(0)Xp(t)⟩ of the Rouse mode Xp(t). The simulations conclusively demonstrate that the Rouse model is invalid in polymer melts. In particular, and contrary to the Rouse model, (i) mean-square Rouse mode amplitudes ⟨(Xp(0))2⟩ do not scale as sin−2(pπ/2N), N being the number of beads in the polymer. For small p (say, p≤3) ⟨(Xp(0))2⟩ scales with p as p−2; for larger p, it scales as p−3. (ii) Rouse mode time correlation functions ⟨Xp(t)Xp(0)⟩ do not decay with time as exponentials; they instead decay as stretched exponentials exp(−αtβ). β depends on p, typically with a minimum near N/2 or N/4. (iii) Polymer bead displacements are not described by independent Gaussian random processes. (iv) For p≠q, ⟨Xp(t)Xq(0)⟩ is sometimes non-zero. (v) The response of a polymer coil to a shear flow is a rotation, not the affine deformation predicted by Rouse. We also briefly consider the Kirkwood–Riseman polymer model
Coil-to-globule collapse of active polymers: a Rouse perspective
No full textWe derive an effective Rouse model for tangentially active polymers, characterised by a constant active force tangent to their backbone. In particular, we show that, once extended to account for finite bending rigidity, such active Rouse model captures the reduction in the gyration radius, or coil-to-globule-like transition, that has been observed numerically in the literature for such active filaments. Interestingly, our analysis identifies the proper definition of the Peclet number, that allows to collapse all numerical data onto a master curve
rouse chocks
No full textrouse n_Diagram_ #32 Fore _Rouse_ chock Aft _rouse_ chock Groove - about 4 inches bottom - " 8 " width - " 2 "[check] [check]179Used IUsed INot usedReverse side of R_14852. Diagram include
Mesomyzostoma lanterbecqae Summers, Al-Hakim & Rouse, 2014, n. sp.
No full text<i>Mesomyzostoma lanterbecqae</i> n. sp. Summers & Rouse <p>Fig. 2 I–L</p> <p> <b>Holotype:</b> SIO-BIC A3651 <b>hologenophore</b> (1 spm: ½—in 70% ethanol after formalin fixation; ½—95% ethanol). Padoz Reef, Madang Harbor, Papua New Guinea (5° 9' 34.8006"S, 145° 48' 46.2096"W), 5– 20 m. Collected using scuba on 27 November 2012 by MMS and GWR. Genbank (COI—KM014176).</p> <p> <b>Host.</b> <i>Clarkcomanthus alternans</i> (Carpenter) (Comatulidae, Comatulida, Crinoidea). MNHN-IE-2013-8114 (dried voucher); SIO-BIC E5879 (tissue subsample in 95% ethanol). Genbank (COI—KM491773).</p> <p> <i>Paratypes:</i> SIO-BIC A3652 <b>syngenophores</b> (3 spms: 2—in 70% ethanol after formalin fixation; 2—95% ethanol). Same location as holotype. Genbank (COI—KM491743). Host: <i>Clarkcomanthus mirabilis</i> (Rowe et al.), MNHN-IE-2013-8174 (dried voucher) & SIO-BIC E5880 (tissue subsample in 95% ethanol); Genbank (COI—KM491774). SIO-BIC A3653 <b>syngenophores</b> (2 spms: 95% ethanol). South Padoz Reef, Madang Harbor, Papua New Guinea (5° 9' 43.1994"S, 145° 48' 59.3922"W), 5– 20 m. Collected using scuba on 1 December 2012. Genbank (COI—KM491744). Host: <i>Comatella nigra</i> (Carpenter), MNHN-IE-2013-8064 (dried voucher) & SIO- BIC E5891 (tissue subsample in 95% ethanol); Genbank (COI—KM491775).</p> <p> <b>Etymology.</b> Named for Deborah Lanterbecq, who first sequenced DNA from a <i>Mesomyzostoma</i> and led the work resulting in the first molecular phylogeny for myzostomids (Lanterbecq <i>et al.</i> 2006).</p> <p> <b>Diagnosis and description.</b> Located within host’s coelom. Holotype body thin and elongate. Length ~ 2.5 mm following fixation (specimen cut and curled) [paratypes 2–4 mm]. Body margin acirrate. Mouth and cloaca terminal. Five pairs of small parapodia, with large hooks (Fig. 2 L). Color cream in life, white in preservative.</p> <p> <b>Remarks.</b> There are nine other species of <i>Mesomyzostoma</i> —two described, <i>Mesomyzostoma katoi</i> Okada, 1933 and <i>Mesomyzostoma reichenspergeri</i> Remscheid, 1918, and four currently being described Eeckhaut <i>et al.</i> (<i>in prep</i>) and three undescribed species in Summers & Rouse (2014). All of these species have a similar body form and occupy the coelom and/or gonads of feather star crinoids. The species are best distinguished by molecular data, followed by host use. This is likely a highly undersampled lifestyle due to the requirement of dissection.</p>Published as part of <i>Summers, Mindi M., Al-Hakim, Iin Inayat & Rouse, Greg W., 2014, Turbo-taxonomy: 21 new species of Myzostomida (Annelida), pp. 301-344 in Zootaxa 3873 (4)</i> on page 306, DOI: 10.11646/zootaxa.3873.4.1, <a href="http://zenodo.org/record/252208">http://zenodo.org/record/252208</a>
Review: Simulational Tests of the Rouse Model
No full textThe file is a Chapter from my review volume Polymer Physics: Phenomenology of Polymeric Fluid Simulations . The chapter treats literature tests of the Rouse model, which is widely invoked as a description of polymer motion in melts. In summary: The literature conclusively demonstrates that the Rouse model does not describe polymer motion in melts. Simulations find that the temporal autocorrelation function of a single Rouse amplitude is a stretched exponential in time, not the pure exponential predicted by the Rouse model. Also, the mean-square amplitude of the Rouse modes deviates from the model\u27s prediction, at least for p > 3. Furthermore, the relaxation time of depends on p, but not as predicted by the Rouse model. According to the Rouse model, bead displacements are driven by independent Gaussian random processes. Accordingly, the intermediate structure factor g(q,t) is predicted to be accurately described by the Gaussian approximation. Doob\u27s theorem then guarantees that g(q,t) decays as a single exponential in time. Simulations show that these predictions of the Rouse model are incorrect.38 pages, 81 references, 12 figure
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