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翻訳と辞書　辞書検索 [ 開発暫定版 ] スポンサード リンク Cyclonic separation ： ウィキペディア英語版 Cyclonic separation Cyclonic separation is a method of removing particulates from an air, gas or liquid stream, without the use of filters, through vortex separation. When removing particulate matter from liquids, hydro cyclone is used while from gas, gas cyclone is used. Rotational effects and gravity are used to separate mixtures of solids and fluids. The method can also be used to separate fine droplets of liquid from a gaseous stream. A high speed rotating (air)flow is established within a cylindrical or conical container called a cyclone. Air flows in a helical pattern, beginning at the top (wide end) of the cyclone and ending at the bottom (narrow) end before exiting the cyclone in a straight stream through the center of the cyclone and out the top. Larger (denser) particles in the rotating stream have too much inertia to follow the tight curve of the stream, and strike the outside wall, then fall to the bottom of the cyclone where they can be removed. In a conical system, as the rotating flow moves towards the narrow end of the cyclone, the rotational radius of the stream is reduced, thus separating smaller and smaller particles. The cyclone geometry, together with flow rate, defines the ''cut point'' of the cyclone. This is the size of particle that will be removed from the stream with a 50% efficiency. Particles larger than the cut point will be removed with a greater efficiency, and smaller particles with a lower efficiency. An alternative cyclone design uses a secondary air flow within the cyclone to keep the collected particles from striking the walls, to protect them from abrasion. The primary air flow containing the particulates enters from the bottom of the cyclone and is forced into spiral rotation by stationary spinner vanes. The secondary air flow enters from the top of the cyclone and moves downward toward the bottom, intercepting the particulate from the primary air. The secondary air flow also allows the collector to optionally be mounted horizontally, because it pushes the particulate toward the collection area, and does not rely solely on gravity to perform this function. Large scale cyclones are used in sawmills to remove sawdust from extracted air. Cyclones are also used in oil refineries to separate oils and gases, and in the cement industry as components of kiln preheaters. Cyclones are increasingly used in the household, as the core technology in bagless types of portable vacuum cleaners and central vacuum cleaners. Cyclones are also used in industrial and professional kitchen ventilation for separating the grease from the exhaust air in extraction hoods.〔(【引用サイトリンク】author=Jeven Oy )〕 Smaller cyclones are used to separate airborne particles for analysis. Some are small enough to be worn clipped to clothing, and are used to separate respirable particles for later analysis. Similar separators are used in the oil refining industry (e.g. for Fluid catalytic cracking) to achieve fast separation of the catalyst particles from the reacting gases and vapors.〔Martin Huard, Cedric Briens, Franco Berruti, Thierry Gauthier, 2010, "A Review of Rapid Gas-Solid Separation Techniques", IJCRE, 8, R1.〕 Analogous devices for separating particles or solids from liquids are called hydrocyclones or hydroclones. These may be used to separate solid waste from water in wastewater and sewage treatment. == Cyclone theory == As the cyclone is essentially a two phase particle-fluid system, fluid mechanics and particle transport equations can be used to describe the behaviour of a cyclone. The air in a cyclone is initially introduced tangentially into the cyclone with an inlet velocity $V\_$. Assuming that the particle is spherical, a simple analysis to calculate critical separation particle sizes can be established. If one considers an isolated particle circling in the upper cylindrical component of the cyclone at a rotational radius of $r$ from the cyclone's central axis, the particle is therefore subjected to drag, centrifugal, and buoyant forces. Given that the fluid velocity is moving in a spiral the gas velocity can be broken into two component velocities: a tangential component, $V\_t$, and an outward radial velocity component $V\_r$. Assuming Stokes' law, the drag force in the outward radial direction that is opposing the outward velocity on any particle in the inlet stream is: :$F\_d\; =\; -6\; \backslash pi\; r\_p\; \backslash mu\; V\_\; .$ Using $\backslash rho\_p$ as the particles density, the centrifugal component in the outward radial direction is: :$F\_c=\; m\; \backslash frac$ ::$=\; \backslash frac\; \backslash pi\; \backslash rho\_p\; r\_p^3\; \backslash frac\; .$ The buoyant force component is in the inward radial direction. It is in the opposite direction to the particle's centrifugal force because it is on a volume of fluid that is missing compared to the surrounding fluid. Using $\backslash rho\_f$ for the density of the fluid, the buoyant force is: :$F\_b\; =\; -V\_p\backslash rho\_f\; \backslash frac$ ::$=\; -\backslash frac\; \backslash frac\backslash rho\_f\; .$ In this case, $V\_p$ is equal to the volume of the particle (as opposed to the velocity). Determining the outward radial motion of each particle is found by setting Newton's second law of motion equal to the sum of these forces: :$m\; \backslash frac\; =\; F\_d\; +\; F\_c\; +\; F\_b$ To simplify this, we can assume the particle under consideration has reached "terminal velocity", i.e., that its acceleration $\backslash frac$ is zero. This occurs when the radial velocity has caused enough drag force to counter the centrifugal and buoyancy forces. This simplification changes our equation to: $F\_d\; +\; F\_c\; +\; F\_b\; =\; 0$ Which expands to: :$-6\backslash pi\; r\_p\; \backslash mu\; V\_r\; +\; \backslash frac\backslash pi\; r\_p^3\; \backslash frac\backslash rho\_p\; -\backslash frac\backslash pi\; r\_p^3\; \backslash frac\backslash rho\_f\; =0$ Solving for $V\_r$ we have :$V\_r\; =\; \backslash frac\; \backslash frac\; \backslash frac\; (\backslash rho\; \_p\; -\; \backslash rho\; \_f)$. Notice that if the density of the fluid is greater than the density of the particle, the motion is (-), toward the center of rotation and if the particle is denser than the fluid, the motion is (+), away from the center. In most cases, this solution is used as guidance in designing a separator, while actual performance is evaluated and modified empirically. In non-equilibrium conditions when radial acceleration is not zero, the general equation from above must be solved. Rearranging terms we obtain :$\backslash frac\; +\; \backslash frac\; \backslash fracV\_r\; -\; \backslash left(1-\backslash frac\backslash right)\; \backslash frac\; =\; 0$ Since $V\_r$ is distance per time, this is a 2nd order differential equation of the form $x\text{'}\text{'}+c\_1\; x\text{'}+c\_2=0$. Experimentally it is found that the velocity component of rotational flow is proportional to $r^2$, therefore: :$V\_t\; \backslash propto\; r^2\; .$ This means that the established feed velocity controls the vortex rate inside the cyclone, and the velocity at an arbitrary radius is therefore: :$U\_r\; =\; U\_\backslash frac\{R\_\{in\}\}\; .$ Subsequently, given a value for $V\_t$, possibly based upon the injection angle, and a cutoff radius, a characteristic particle filtering radius can be estimated, above which particles will be removed from the gas stream. 抄文引用元・出典: フリー百科事典『 ウィキペディア（Wikipedia）』 ■ウィキペディアで「Cyclonic separation」の詳細全文を読む スポンサード リンク 翻訳と辞書 : 翻訳のためのインターネットリソース Copyright(C) kotoba.ne.jp 1997-2016. All Rights Reserved.