416 research outputs found

    Fermentation of animal components in strict carnivores: a comparative study with cheetah fecal inoculum

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    The natural diet of felids contains highly digestible animal tissues but also fractions resistant to small intestinal digestion, which enter the large intestine where they may be fermented by the resident microbial population. Little information exists on the microbial degradability of animal tissues in the large intestine of felids consuming a natural diet. This study aimed to rank animal substrates in their microbial degradability by means of an in vitro study using captive cheetahs fed a strict carnivorous diet as fecal donors. Fresh cheetah fecal samples were collected, pooled, and incubated with various raw animal substrates (chicken cartilage, collagen, glucosamine-chondroitin, glucosamine, rabbit bone, rabbit hair, and rabbit skin; 4 replicates per substrate) for cumulative gas production measurement in a batch culture technique. Negative (cellulose) and positive (casein and fructo-oligosaccharides; FOS) controls were incorporated in the study. Additionally, after 72 h of incubation, short-chain fatty acids (SCFA), including branched-chain fatty acids (BCFA), and ammonia concentrations were determined for each substrate. Glucosamine and glucosamine-chondroitin yielded the greatest OM cumulative gas volume (OMCV) among animal substrates (P < 0.05), whereas total SCFA production was greatest for collagen (P < 0.05). Collagen induced an acetate production comparable to FOS and a markedly high acetate-to-propionate ratio (8.41:1) compared to all other substrates (1.67:1 to 2.97:1)

    Body Image and Cosmesis after Percutaneous Transforaminal Endoscopic Discectomy versus Conventional Open Microdiscectomy for Sciatica

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    Study Design: Randomized controlled trial Objective: Percutaneous transforaminal endoscopic discectomy (PTED) was introduced as a less invasive procedure to treat sciatica. Even though the PTED has a small scar size, it is unknown if PTED also leads to better scar-related patient-reported outcomes. Therefore, we aimed to compare scar-related outcomes between patients undergoing PTED vs open microdiscectomy. Methods: Patients with at least 6 weeks of radiating leg pain were randomized in a 1:1 ratio to PTED or open microdiscectomy. Scar-related patient-reported outcomes were measured using the Body Image Score (BIS), Cosmesis Scale (CS) and a 0-10 numeric rating scale (NRS) on scar esthetic. Results: Of the 530 included patients, 286 patients underwent PTED and 244 underwent open microdiscectomy as allocated. At 12 months of follow-up, 95% of the patients had data available. At 12 months, the BIS was 6.2 ± 1.7 in the PTED-group and 6.6 ± 1.9 in the open microdiscectomy group (between-group difference.4, 95% CI.2 to.7). CS was 21.3 ± 3.0 in the PTED-group and 18.6 ± 3.4 in the open microdiscectomy group (between-group difference −2.7, 95% CI −3.1 to −2.3). Average NRS for scar esthetic was 9.2 ± 1.3 and 7.8 ± 1.6 in the PTED and open microdiscectomy groups, respectively (between-group difference −1.4, 95% CI −1.6 to −1.2) Conclusions: PTED leads to a higher self-rated scar esthetic as compared to open microdiscectomy, while self-reported body image seems to be comparable between both groups. Therefore, from an esthetic point, PTED seems to be the preferred technique to treat sciatica.</p

    Heavy gold cluster beams production and identification

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    NIM ACCIt is shown that beams of very heavy gold clusters can be produced by a liquid metal ion source (LMIS). An experimental method is described for defining the LMIS source and the Wien filter parameters that must be set to extract and select large Aun clusters. This method is based on the acceleration of the clusters to high energy (MeV) and on the measurement, after their passage through a thin foil, of their number of constituents and velocity. Only an average mass over charge value is obtained for a given set of source and Wien filter parameters. These parameters can then be used to select heavy Aun cluster beams for applications at low energy (keV) in mass spectrometry

    Energy loss and angular distributions of gold cluster constituents

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    Heavy gold cluster beams are accelerated to high energy (hundreds of keV/atom) and break up when going through a thin foil. The energy and angular distributions of the constituents are then measured and very well reproduced by a SRIM code calculation, which takes into account atomic interactions only. These distributions do not depend on the number of constituents in the cluster and are found to be the same as those of single gold atoms at the same velocity, in the studied energy range

    Steady nearly incompressible vector fields in 2D: chain rule and renormalization

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    Given bounded vector field bcolonRRdoRRdbcolon RR^d o RR^d, scalar field ucolonRRdoRRucolon RR^d o RR and a smooth function etacolonRRoRReta colon RR o RR we study the characterization of the distribution div(eta(u)b)div(eta(u)b) in terms of divbdiv b and div(ub)div(u b). In the case of BVBV vector fields bb (and under some further assumptions) such characterization was obtained by L. Ambrosio, C. De Lellis and J. Mal'y, up to an error term which is a measure concentrated on so-called emph{tangential set} of bb. We answer some questions posed in their paper concerning the properties of this term. In particular we construct a nearly incompressible BVBV vector field bb and a bounded function uu for which this term is nonzero. For steady nearly incompressible vector fields bb (and under some further assumptions) in case when d=2d=2 we provide complete characterization of div(eta(u)b)div(eta(u) b) in terms of divbdiv b and div(ub)div(u b). Our approach relies on the structure of level sets of Lipschitz functions on RR2RR^2 obtained by G. Alberti, S. Bianchini and G. Crippa. Extending our technique we obtain new sufficient conditions when any bounded weak solution uu of dtu+bcdotablau=0d_t u + b cdot abla u=0 is emph{renormalized}, i.e. also solves dteta(u)+bcdotablaeta(u)=0d_t eta(u) + b cdot abla eta(u)=0 for any smooth function etacolonRRoRReta colonRR o RR. As a consequence we obtain new uniqueness result for this equation
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