Kim, Diana H.; Bautista, Sana A.; Mehta, Sonul; Briceño, César A., E-mail: Cesar.Briceno@pennmedicine.upenn.edu2023
AbstractAbstract
[en] A 53-year-old man with a 3-day history of periorbital swelling and vision loss in the left eye was found to have septic cavernous sinus thrombosis with bilateral orbital vein involvement causing congestive orbitopathy. He was treated with an emergent canthotomy and cantholysis, intraocular pressure-lowering drops, antibiotics, anticoagulation, and serial examinations. Optical coherence tomography ultimately revealed diffuse ischemic destruction of both layers of the retina, which suggested occlusion of the ophthalmic artery or the short posterior ciliary arteries and central retinal artery without intracavernous internal carotid artery involvement. The patient remained without light perception in the left eye after treatment. (author)
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Available from: https://www.scielo.br/j/abo/a/9t4YwxZMqkZRd3DCCjVvJ7m/?format=pdf& lang=en
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Journal Article
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Arquivos Brasileiros de Oftalmologia (Online); ISSN 1678-2925; ; v. 86(1); p. 79-82
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ANEMIAS, BACTERIA, BLOOD VESSELS, BODY, CARDIOVASCULAR DISEASES, CARDIOVASCULAR SYSTEM, DIAGNOSTIC TECHNIQUES, DISEASES, EYES, FACE, HEAD, HEMIC DISEASES, MEDICINE, MICROORGANISMS, NUCLEAR MEDICINE, ORGANS, PATHOLOGICAL CHANGES, RADIOLOGY, RESONANCE, SENSE ORGANS, SYMPTOMS, TOMOGRAPHY, VASCULAR DISEASES
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AbstractAbstract
[en] The propagation of thermal and magnetohydrodynamic (MHD) waves in a heat-conducting, hydrogen plasma, threaded by an external uniform magnetic field (B) and in which photoionization and photorecombination [H++e-<-->H+hν(χ)] processes are progressing, is investigated here using linear analysis. The resulting dispersion equation is solved analytically for varied strength (β<<1 and ∼1) and orientation of the magnetic field, where β denotes the ratio of plasma to magnetic pressures. Application of this model to the interstellar medium shows that heat conduction governs the propagation of thermal waves only at relatively high frequencies regardless of the plasma temperature, strength, and orientation of the magnetic field. When the direction of wave propagation is held perpendicular to B (i.e., k perpendicular B), the magnetosonic phase velocity is closely Alfvenic for β<<1, while for β∼1 both the hydrostatic and magnetic pressures determine the wave velocity. As long as k parallel B, the fast (transverse) magnetosonic wave becomes an Alfven wave for all frequencies independent of the plasma temperature and field strength, while the slow (longitudinal) magnetosonic wave becomes a pure sound wave. Amplification of thermal and MHD waves always occur at low frequencies and preferentially at temperatures for which the plasma is either weakly or partially ionized. Compared to previous analysis for the same hydrogen plasma model with B=0, the presence of the magnetic field makes the functional dependence of the physical quantities span a longer range of frequencies, which becomes progressively longer as the field strength is increased
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(c) 2004 American Institute of Physics.; Country of input: International Atomic Energy Agency (IAEA)
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