3,267 research outputs found
Excerpt from 2024 Keynote Address by Wade Rouse
No full textAn excerpt from the show-stopping keynote address by author Wade Rouse. He received a standing ovation and a request for a reprise/sing-along of a middle school performance of Delta Dawn
Rouse, T J, WX5963
No full textThis record was harvested from a previous catalogue system and will be withdrawn in 2025. Information in this record may be superseded or incomplete. Visit this record in UMA's new catalogue at: https://archives.library.unimelb.edu.au/nodes/view/414480Surname: ROUSE. Given Name(s) or Initials: T J. Military Service Number or Last Known Location: WX5963. Missing, Wounded and Prisoner of War Enquiry Card Index Number: 44438.233827
Item: [2016.0049.46741] "Rouse, T J, WX5963
William Mac Rouse to Robert C. Byrd, 20 August 1971
No full textCarbon typed letter dated 20 August 1971 from William Mac Rouse, Special Assistant to the President, to Robert C. Byrd, re: misconduct of Superior Court Judge Harry T. Alexander; copied to Eastland.https://egrove.olemiss.edu/joecorr_f/1042/thumbnail.jp
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[Photograph of W. T. Rouse]
No full textPhotograph of W. T. Rouse. He stands to the right of a wooden fence, wearing a suit and tie
[Photograph of W. T. Rouse]
No full textPhotograph of W. T. Rouse. He stands to the right of a wooden fence, wearing a suit and tie
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
rouse (exclamation)
No full textrouse v. . . .he's tipped the boards an' down comes the horse collars, chains,breechin' an' hisself rouse! on the floor. (same usage and meaning as the exclamation _souse_ i.e. signifying a sudden loud noise, in this case caused by several large objects and a man falling from a loft onto the floor below)See Editor's Notes.YesDNE-cit JUL 1977Used IUsed IUsed
Cerium(IV) fluoride and fluoride-arsenate frameworks
No full textFive new cerium (IV) fluoride and fluoride–arsenate framework structures have been synthesised hydrothermally using CeF4 as a fluoride source. Cs[Ce2F8[F·H2O]] ( I) consists of layers, formed from linked Ce(F,O)n polyhedra cross-linked by hydrogen bonding that defines large channels containing the caesium ions. [(NH4)5(H2O)2][Ce4(AsO4)6(H2O)F3] ( II), has an open framework structure with large channels filled with NH4+ cations and H2O molecules. Ce[AsO4]F ( III) and Ce[AsO4]F[H2O] ( IV) exhibit two types of bridging (Ce–O–Ce and Ce–F–Ce) bonds between Ce(O,F)n polyhedra, and (NH4)[CeF2(AsO4)] ( V), is isostructural with the previously reported fluoride-phosphate (NH4)[CeIVF2(PO4
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
Letter re: Will Rogers' death
No full textLetter from T. L. Rouse, editor of the Vernon Times, to Amon Carter regarding the death of Will Rogers. Enclosed are some writings from Rouse
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