879 research outputs found

    Sex assignment in conditions affecting sex development

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    The newborn infant with atypical genitalia presents a challenging clinical scenario and requires expert input. There have been appreciable advances in our knowledge of the underlying causes that may lead to a mere difference or a more serious disorder of sex development (DSD), the natural history of conditions, as well as the short and long-term complications of these conditions themselves, together with the clinical interventions that are associated with these conditions. With this information, the DSD expert can be more confident when discussing options with the parents of the newborn infant. By working within a multidisciplinary team, the expert should be able to support the family whilst individualising the management plan so that it is also cognizant of the shifts in societal attitudes and expectations around concepts of diversity and openness. It is, therefore, likely that the practice of assigning sex, especially in those cases where sex assignment is unclear on expert assessment, will continue to show temporal, social and geographical variations. It is imperative that clinical data for rare conditions such as these are collected in a standardized format and shared through a common registry so that any evidence that is used for future shifts in practice has a stronger foundation than that which is currently available

    High order fluid model for streamer discharges. II. Numerical solution and investigation of planar fronts

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    The high order fluid model developed in the preceding paper is employed here to study the propagation of negative planar streamer fronts in pure nitrogen. The model consists of the balance equations for electron density, average electron velocity, average electron energy and average electron energy flux. These balance equations have been obtained as velocity moments of Boltzmann's equation and are here coupled to the Poisson equation for the space charge electric field. Here the results of simulations with the high order model, with a PIC/MC (Particle in cell/Monte Carlo) model and with the first order fluid model based on the hydrodynamic drift-diffusion approximation are presented and compared. The comparison with the MC model clearly validates our high order fluid model, thus supporting its correct theoretical derivation and numerical implementation. The results of the first order fluid model with local field approximation, as usually used for streamer discharges, show considerable deviations. Furthermore, we study the inaccuracies of simulation results caused by an inconsistent implementation of transport data into our high order fluid model. We also demonstrate the importance of the energy flux term in the high order model by comparing with results where this term is neglected. Finally, results with an approximation for the high order tensor in the energy flux equation is found to agree well with the PIC/MC results for reduced electric fields up to 1000 Townsend, as considered in this work.Comment: 26 pages, 11 figure

    Derivation and test of high order fluid model for streamer discharges

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    A high order fluid model for streamer dynamics is developed by closing the system after the 4th moment of the Boltzmann equation in local mean energy approximation. This is done by approximating the high order pressure tensor in the heat flux equation through the previous moments. Mathematical characteristics of the system is studied. Then planar ionization fronts for negative streamers in Nsub2 are simulated with the classical streamer model, MC-PIC particle model, and with the present higher order model

    Testicular dermoid cyst in a 14-year-old child

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    Π”Π•Π ΠœΠžΠ˜Π”ΠΠΠ― КИБВА /Π”Π˜ΠΠ“ΠΠ”Π•Π ΠœΠžΠ˜Π” /Π”Π˜ΠΠ“ΠΠ―Π˜Π§ΠšΠ˜ /Π£Π›Π¬Π’Π ΠΠ‘ΠžΠΠ”Π•Π’Π˜ΠšΠ›Π˜ΠΠ˜Π§Π•Π‘ΠšΠ˜Π• Π‘Π›Π£Π§ΠΠ˜Π’ Ρ€Π°Π±ΠΎΡ‚Π΅ прСдставлСн клиничСский случай Ρ€Π΅Π±Π΅Π½ΠΊΠ°, 14 Π»Π΅Ρ‚, с Π΄Π΅Ρ€ΠΌΠΎΠΈΠ΄Π½ΠΎΠΉ кистой ΠΏΡ€Π°Π²ΠΎΠ³ΠΎ яичка. ΠžΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ Π²ΠΏΠ΅Ρ€Π²Ρ‹Π΅ Π±Ρ‹Π»ΠΎ выявлСно ΠΏΡ€ΠΈ профилактичСском осмотрС Π² ΠΏΠΎΠ»ΠΈΠΊΠ»ΠΈΠ½ΠΈΠΊΠ΅. Π’ ΠΏΠΎΡΠ»Π΅Π΄ΡƒΡŽΡ‰Π΅ΠΌ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Ρƒ Π½Π΅ΠΎΠ΄Π½ΠΎΠΊΡ€Π°Ρ‚Π½ΠΎ ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΎΡΡŒ ΡƒΠ»ΡŒΡ‚Ρ€Π°Π·Π²ΡƒΠΊΠΎΠ²ΠΎΠ΅ исслСдованиС Π½Π°Ρ€ΡƒΠΆΠ½Ρ‹Ρ… ΠΏΠΎΠ»ΠΎΠ²Ρ‹Ρ… ΠΎΡ€Π³Π°Π½ΠΎΠ², ΠΏΡ€ΠΈ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΌ Π² Π²Π΅Ρ€Ρ…Π½Π΅ΠΌ полюсС ΠΏΡ€Π°Π²ΠΎΠ³ΠΎ яичка Π²Ρ‹ΡΠ²Π»ΡΠ»Π°ΡΡŒ нСоднородная эхоструктура Ρ€Π°Π·ΠΌΠ΅Ρ€Π°ΠΌΠΈ 14 ΠΌΠΌ, 13,7 ΠΌΠΌ ΠΈ 12 ΠΌΠΌ с Ρ‡Π΅Ρ‚ΠΊΠΈΠΌ, Ρ€ΠΎΠ²Π½Ρ‹ΠΌ ΠΊΠΎΠ½Ρ‚ΡƒΡ€ΠΎΠΌ. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΈΠΌΠΌΡƒΠ½ΠΎΡ„Π΅Ρ€ΠΌΠ΅Π½Ρ‚Π½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° ΠΊΡ€ΠΎΠ²ΠΈ Π½Π΅ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ ΡƒΠ²Π΅Π»ΠΈΡ‡Π΅Π½ΠΈΠ΅ основных ΠΌΠ°Ρ€ΠΊΠ΅Ρ€ΠΎΠ² ΠΎΠΏΡƒΡ…ΠΎΠ»Π΅Π²ΠΎΠ³ΠΎ процСсса. ΠŸΡ€ΠΈ биохимичСском тСстировании ΠΊΡ€ΠΎΠ²ΠΈ ΠΎΡ‚ΠΌΠ΅Ρ‡Π°Π»ΠΎΡΡŒ Π½Π΅Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠ΅ ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½ΠΈΠ΅ уровня прямого Π±ΠΈΠ»ΠΈΡ€ΡƒΠ±ΠΈΠ½Π° ΠΈ сывороточного ΠΆΠ΅Π»Π΅Π·Π°. Для уточнСния Π΄ΠΈΠ°Π³Π½ΠΎΠ·Π° ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½Π° ΠΌΠ°Π³Π½ΠΈΡ‚Π½ΠΎ-рСзонансная томография ΠΎΡ€Π³Π°Π½ΠΎΠ² ΠΌΠ°Π»ΠΎΠ³ΠΎ Ρ‚Π°Π·Π° с Π²Π½ΡƒΡ‚Ρ€ΠΈΠ²Π΅Π½Π½Ρ‹ΠΌ контрастированиСм. ПослС провСдСния ΡƒΠΊΠ°Π·Π°Π½Π½ΠΎΠ³ΠΎ обслСдования Π±Ρ‹Π» выставлСн Π΄ΠΈΠ°Π³Π½ΠΎΠ· "кистозноС ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΡ€Π°Π²ΠΎΠ³ΠΎ яичка". ПослС провСдСния Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΡ‹Ρ… Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… диагностичСских мСроприятий (Π£Π—Π˜ пСрифСричСских лимфатичСских ΡƒΠ·Π»ΠΎΠ², обслСдованиС Π±Ρ€ΡŽΡˆΠ½ΠΎΠΉ полости с Π²Π½ΡƒΡ‚Ρ€ΠΈΠ²Π΅Π½Π½Ρ‹ΠΌ контрастным усилСниСм) Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½Π° опСрация, Π·Π°ΠΊΠ»ΡŽΡ‡Π°Π²ΡˆΠ°ΡΡΡ Π² Ρ€Π΅Π²ΠΈΠ·ΠΈΠΈ ΠΏΡ€Π°Π²ΠΎΠΉ ΠΏΠΎΠ»ΠΎΠ²ΠΈΠ½Ρ‹ мошонки ΠΈ ΡƒΠ΄Π°Π»Π΅Π½ΠΈΠΈ образования ΠΏΡ€Π°Π²ΠΎΠ³ΠΎ яичка. Π˜Π½Ρ‚Ρ€Π°ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΎΠ½Π½ΠΎ ΠΏΠΎ Π΄Π°Π½Π½Ρ‹ΠΌ экспрСсс-биопсии Π΄ΠΈΠ°Π³Π½ΠΎΡΡ‚ΠΈΡ€ΠΎΠ²Π°Π»Π°ΡΡŒ дСрмоидная киста ΠΏΡ€Π°Π²ΠΎΠ³ΠΎ яичка, Ρ‡Ρ‚ΠΎ ΠΏΠΎΠ΄Ρ‚Π²Π΅Ρ€Π΄ΠΈΠ»ΠΎΡΡŒ ΠΏΡ€ΠΈ ΠΏΠΎΡΠ»Π΅Π΄ΡƒΡŽΡ‰Π΅ΠΌ гистологичСском исслСдовании. ΠŸΠΎΡΠ»Π΅ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΎΠ½Π½Ρ‹ΠΉ ΠΏΠ΅Ρ€ΠΈΠΎΠ΄ ΠΏΡ€ΠΎΡ‚Π΅ΠΊΠ°Π» Π³Π»Π°Π΄ΠΊΠΎ. ΠŸΠ°Ρ†ΠΈΠ΅Π½Ρ‚ выписался Π² ΡƒΠ΄ΠΎΠ²Π»Π΅Ρ‚Π²ΠΎΡ€ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΌ состоянии. Π’Π°ΠΊΠΈΠΌ ΠΎΠ±Ρ€Π°Π·ΠΎΠΌ, прСдставлСнноС клиничСскоС наблюдСниС ΠΏΠΎΠ΄Ρ‡Π΅Ρ€ΠΊΠΈΠ²Π°Π΅Ρ‚ Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎΡΡ‚ΡŒ ΠΎΠΏΡ‚ΠΈΠΌΠΈΠ·Π°Ρ†ΠΈΠΈ профилактичСской Ρ€Π°Π±ΠΎΡ‚Ρ‹ мСдицинского пСрсонала ΠΏΠ΅Ρ€Π²ΠΈΡ‡Π½ΠΎΠ³ΠΎ Π·Π²Π΅Π½Π° ΠΏΠΎ своСврСмСнной диагностикС ΠΎΠΏΡƒΡ…ΠΎΠ»Π΅Π²Ρ‹Ρ… процСссов Π½Π°Ρ€ΡƒΠΆΠ½Ρ‹Ρ… ΠΏΠΎΠ»ΠΎΠ²Ρ‹Ρ… ΠΎΡ€Π³Π°Π½ΠΎΠ², особСнно Ρƒ Π΄Π΅Ρ‚Π΅ΠΉ ΠΏΡƒΠ±Π΅Ρ€Ρ‚Π°Ρ‚Π½ΠΎΠ³ΠΎ возраста.The paper presents a clinical case of a 14-year-old child with a dermoid cyst of the right testicle. The formation was first detected during a routine check-up in the polyclinic. Then the external genitalia ultrasound examination was repeatedly performed to the patient, which revealed an inhomogeneous echostructure with dimensions of 14 mm, 13.7 mm and 12 mm with a clear, even contour in the upper pole of the right testicle. The enzyme-linked immunosorbent assay (ELISA) did not show an increase in the main tumour markers. The biochemical blood test revealed an insignificant rise in conjugated bilirubin and serum iron. To clarify the diagnosis, magnetic resonance tomography of the pelvic organs with intravenous contrast was recommended. After examination, the cystic lesion of the right testicle was diagnosed. After carrying out the necessary additional diagnostic measures (ultrasound examination of the peripheral lymphatic nodes, the abdominal cavity exploration with intravenous contrast enhancement), the child underwent an operation consisting in revising the right half of the scrotum and removing the formation of the right testicle. Intraoperatively, according to the express biopsy test, the dermoid cyst of the right testicle was diagnosed, which was confirmed by the subsequent histological examination. The postoperative period was uneventful. The patient was discharged in satisfactory state. Thus, the presented clinical observation emphasizes the need to optimize the preventive work of primary care medical personnel for timely diagnosis of tumor processes in the external genital organs, especially in children of puberty

    Intense high-order harmonic generation in giant fullerene molecule C240_{240}

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    In this work the extreme nonlinear optical response of a giant fullerene molecule C240_{240} in strong laser field is studied. The investigation of high-order harmonic generation in such quantum nanostructure is presented modeling the C240_{240} molecule and its interaction with the laser field in the scope of the tight-binding mean-field approach. Electron-electron interaction is modeled by the parametrized Ohno potentail, which takes into account long-range Coulomb interaction. The essential role of many body Coulomb interaction in determining of harmonics intensities is demonstrated. We also consider vacancy-deffected molecule C240_{240}. The presence of a single vacancy breaks the icosahedral symmetry leading to the emergence of intense even-order harmonics. We examine the dependence of moderate harmonics on laser frequency that shows the multiphoton resonant nature of high harmonics generation. The dependence of cutoff harmonics on both laser intensity and frequency are examined too.Comment: 9 pages, 10 figure

    High order fluid model for streamer discharges

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    A high order fluid model for streamer discharges is developed and used to investigate propagation of negative streamer fronts in N2 . Mo- mentum transfer theory is employed to evaluate the collision terms and close the system of moment/balance equations. The results of simulations are compared with those obtained by a PIC/MC method and by the classical first order fluid model based on the drif

    Magnetic Properties of J-J-J' Quantum Heisenberg Chains with Spin S=1/2, 1, 3/2 and 2 in a Magnetic Field

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    By means of the density matrix renormalization group (DMRG) method, the magnetic properties of the J-J-Jβ€²^{\prime} quantum Heisenberg chains with spin S=1/2S=1/2, 1, 3/2 and 2 in the ground states are investigated in the presence of a magnetic field. Two different cases are considered: (a) when JJ is antiferromagnetic and Jβ€²J^{\prime} is ferromagnetic (i.e. the AF-AF-F chain), the system is a ferrimagnet. The plateaus of the magnetization are observed. It is found that the width of the plateaus decreases with increasing the ferromagnetic coupling, and disappears when % J^{\prime}/J passes over a critical value. The saturated field is observed to be independent of the ferromagnetic coupling; (b) when JJ is ferromagnetic and Jβ€²J^{\prime} is antiferromagnetic (i.e. the F-F-AF chain), the system becomes an antiferromagnet. The plateaus of the magnetization are also seen. The width of the plateaus decreases with decreasing the antiferromagnetic coupling, and disappears when Jβ€²/JJ^{\prime}/J passes over a critical value. Though the ground state properties are quite different, the magnetization plateaus in both cases tend to disappear when the ferromagnetic coupling becomes more dominant. Besides, no fundamental difference between the systems with spin half-integer and integer has been found.Comment: 8 pages, 9 figures, to be published in J. Phys.: Condens. Matte

    Comparing plasma fluid models of different order for 1D streamer ionization fronts

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    We evaluate the performance of three plasma fluid models: the first order reaction-drift-diffusion model based on the local field approximation; the second order reaction-drift-diffusion model based on the local energy approximation and a recently developed high order fluid model by Dujko et al (2013 J. Phys. D 46 475202) We first review the fluid models: we briefly discuss their derivation, their underlying assumptions and the type of transport data they require. Then we compare these models to a particle-in-cell/Monte Carlo (PIC/MC) code, using a 1D test problem. The tests are performed in neon and nitrogen at standard temperature and pressure, over a wide range of reduced electric fields. For the fluid models, transport data generated by a multi-term Boltzmann solver are used. We analyze the observed differences in the model predictions and address some of the practical aspects when using these plasma fluid models
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