| 영문 | coagulation time | 한글 | 응고시간 |
|---|---|---|---|
| 설명 | 혈액응고란 지혈의 한 과정으로 섬유소란 물질을 만들어 내는 과정이다. 이 섬유소란 물질은 손상된 혈관의 부위에 작용하여 여러 가지 세포들을 얽어 묶는 역할을 하여 결국 손상된 혈관에서 혈액의 소실을 막는다. 혈액응고는 다음과 같은 3단계로 이루어진다. 첫번째 단계는 혈관손상에 의해서 prothrombin activator라는 것이 만들어지는 단계이다. 두번째 단계는 이 prothrombin activator라는 물질에 의해서 혈액속에 있는 프로트롬빈이라는 물질이 트롬빈이라는 물질로 바뀌는 단계이다. 세번째 단계는 트롬빈이라는 물질에 의해서 섬유소원이라는 물질이 섬유소으로 바뀌는 단계이다. 응고작용은 크게 2가지로 나뉘는데, 외인성 응고인자와 내인성 응고인자가 그것이다. 외인성 응고인자와 내인성 응고인자는 각기 별개로 작용하지만, 결국은 마지막 과정에서 하나로 만나서 섬유소원을 섬유소(응고작용의 마지막 단계에 생성되며 단단하고 풀리지 않는 매듭을 형성하여 지혈작용을 완성한다)으로 만들어 응고작용을 나타낸다. |
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| 영문 | bleeding time | 한글 | 출혈시간 |
|---|---|---|---|
| 설명 | 몸에 상처가 나서 출혈이 있었을 경우에 피가 멎는데 까지 걸리는 시간을 출혈시간이라고 한다. 사람의 몸에 상처가 나서 출혈이 있을 경우에 이것을 막고 피를 더이상 나지 않게 하는 것을 지혈이라고 한다. 지혈의 과정에는 크게 두 가지 단계가 있다. 첫번째 단계는 혈소판들이 상처가 나서 손상된 혈관의 부위를 막는 것이다. 이렇게 하면 우선 혈관의 손상부위로부터 피가 나오는 것을 막을 수가 있다. 다음의 단계는 상처를 막고 있는 혈소판위에 여러 가지 물질들이 작용해서 더욱 단단하게 하여 상처가 난 혈관에서 피가 새는 것을 영구히 막는 것이다. 쉽게 말하면 혈소판은 벽돌에 해당하는 것이고 두번째 과정에 참여하는 물질들은 시멘트에 해당하는 것이다. 이 두 과정이 완전할 경우에 지혈이 순조롭게 일어난다. 출혈시간은 위에서 설명한 지혈의 두가지 과정 중에서 첫번째 과정에 의해서만 영향을 받는다. 즉 손상된 혈관을 막아주는 벽돌에 해당하는 혈소판의 기능만 정상일 경우에 출혈시간은 정상으로 나온다. 만약 혈소판의 기능에 이상이 있는 경우에는 자연히 출혈시간이 길어진다. |
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| 영문 | prothrombin time | 한글 | 프로트롬빈시간 |
|---|---|---|---|
| 설명 | 프로트롬빈은 간에서 합성되는 비타민 K 의존성 응고단백질의 하나이며, 프로트롬빈시간은 외인계 응고활성을 종합적으로 특정하는 검사의 하나이다. 피검혈장에 칼슘이온과 조직트롬보플라스틴(제III 응고인자)을 가해, 섬유소가 나타날 때까지의 시간으 측정한다. |
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| CT | calcitonin; calf testis; cardiac tamponade; cardiothoracic [ratio]; carotid tracing; carpal tunnel; ... |
|---|---|
| PTT | partial thromboplastin time; particle transport time; posterior tibial tendon (transfer); prothrombi... |
| AGD | agar gel diffusion; agarose diffusion; alpha-ketoglutarate dehydrogenase |
| DP | data processing; deep pulse; definitive procedure; degradation product; degree of polymerization; de... |
| ST | esotropia; scala tympani; scaphotrapezoid; sclerotherapy; sedimentation time; semitendinosus; sensor... |
| ADC | Apparent Diffusion Coefficient |
|---|---|
| ADC | Apparent diffusion coefficient of water |
| DC | Diffusion Chambers |
| DTI | Diffusion Tensor Imaging |
| DWI | Diffusion Weighted Imaging |
mucosal bleeding (점막 출혈
| ambipolar diffusion | <radiobiology> Diffusion process in which buildup of spatial charge creates electric fields which cause electrons and ions to leave the plasma at the same rate. (Such electric fields are self-generated by the plasma and act to preserve charge neutrality.) (09 Oct 1997) |
|---|---|
| anomalous diffusion | <radiobiology> Diffusion in most plasma devices, particularly tokamaks, is higher than what one would predict from understood causes. The observed, typical diffusion is referred to as anomalous because it has not yet been explained. Anomalous diffusion includes all diffusion which is not due to collisions and geometric effects. While such effects were not understood when the term was coined, and most still are not, diffusion due to well-understood wave phenomena is still 'anomalous'. Classical diffusion and Neo-classical diffusion are the two well-understood diffusion theories, although neither is adequate to fully explain the observed anomalous diffusion. See: entries for classical diffusion and neoclassical diffusion. Anomalous resistivity (09 Oct 1997) |
| bohm diffusion | <radiobiology> A rapid loss of plasma across magnetic field lines caused by microinstabilities. Theory formulated by the physicist David Bohm. Semiempirical formula for the diffusion coefficient given by Bohm in 1946 (noted by Bohm, Burhop, and Massey, who were developing a magnetic arc for use in uranium isotope separation). Bohm diffusion was proposed (not derived from first principles) to scale as 1/B rather than the 1/B^2 scaling predicted by classical diffusion. A 1/B scaling results from assuming that particles diffuse across field lines at an optimum rate (effective collision frequency=cyclotron frequency). The 1/B scaling is observed (approximately) in most reactors. See: diffusion, microinstabilities, field lines. (09 Oct 1997) |
| gel diffusion | Diffusion in a gel, as in the case of gel diffusion precipitin tests in which the immune reactants diffuse in agar. See: immunodiffusion. (05 Mar 2000) |
| gel diffusion precipitin tests | Precipitin test's in which the immune precipitate forms in a gel medium (usually agar) into which one or both reactants have diffused; generally classified in two types, in one dimension, and in two dimensions. Synonym: gel diffusion reactions. (05 Mar 2000) |
| gel diffusion precipitin tests in one dimension | Precipitin test's in which antigen solution and antibody incorporated in agar are layered in tubes, permitting effective diffusion in the vertical dimension; the antibody-containing agar may be overlaid directly with antigen solution (single (gel) diffusion in one dimension). (05 Mar 2000) |
| gel diffusion precipitin tests in two dimensions | Precipitin test's made in a layer of agar that permits radial diffusion, in both of the horizontal dimensions, of one or both reactants. Double (gel) diffusion in two dimensions (Ouchterlony test, technique, or method) incorporates antigen and antibody solutions placed in separate wells in a sheet of plain agar, permitting radial diffusion of both reactants; this method is widely used to determine antigenic relationships; the bands of precipitate that form where the reactants meet in optimal concentration are of three patterns, referred to as reaction of identity, reaction of partial identity (cross-reaction), and reaction of nonidentity. (05 Mar 2000) |
| gel diffusion reactions | Precipitin test's in which the immune precipitate forms in a gel medium (usually agar) into which one or both reactants have diffused; generally classified in two types, in one dimension, and in two dimensions. Synonym: gel diffusion reactions. (05 Mar 2000) |
| passive diffusion | See: facilitated transport. (05 Mar 2000) |
| classical diffusion | <radiobiology> In plasma physics, diffusion due solely to scattering (collisions) of charged particles (with unlike charges) via electrical (Coulomb) interactions. (See also diffusion.) (09 Oct 1997) |
| population diffusion coefficient | <cell biology> Coefficient that describes the tendency of a population of motile cells to diffuse through the environment. Its use presupposes that the cells move in a random walk. (18 Nov 1997) |
| neoclassical diffusion | <radiobiology> In a magnetised plasma, _classical_ diffusion refers to transport of particles due to Coulomb collisions, taking the spiral orbits in the magnetic field into account. In a toroidal magnetic field, the actual rate of diffusive transport is much higher due to slow changes in the positions of the centres of the spirals, known as banana orbits. This faster transport is called _neo-classical_. With very few exceptions the transport in toroidal devices is observed to be 10-100 times larger still, presumably due to small-scale turbulence. The observed transport is called _anomalous_ (although it actually is the normal state). (09 Oct 1997) |
| diffusion | The process of becoming diffused or widely spread, the spontaneous movement of molecules or other particles in solution, owing to their random thermal motion, to reach a uniform concentration throughout the solvent, a process requiring no addition of energy to the system. (18 Nov 1997) |
| diffusion anoxia | Diffusion hypoxia severe enough to result in the absence of oxygen in alveolar gas. (05 Mar 2000) |
| diffusion chambers, culture | Devices used in a technique by which cells or tissues are grown in vitro or, by implantation, in vivo within chambers permeable to diffusion of solutes across the chamber walls. The chambers are used for studies of drug effects, osmotic responses, cytogenic and immunologic phenomena, metabolism, etc., and include tissue cages. (12 Dec 1998) |
제품명 |
판매사 |
보험코드 | 성분/함량 | 구분/보험급여 |
|---|
제품명 |
판매사 |
보험코드 | 성분/함량 | 구분/보험급여 |
|---|