Screw Compressors, 1st Edition by Ahmed Kovacevic, Nikola Stosic, Ian Smith (auth.)

By Ahmed Kovacevic, Nikola Stosic, Ian Smith (auth.)

This e-book - the authors' moment ebook on screw compressors – offers the result of the hottest equipment of 3-dimensional modeling of the fluid dymanics and the solid-fluid interplay inside those machines, that are nonetheless being constructed. by means of together with them within the layout technique, it truly is attainable, not just to foretell stream styles extra adequately, and consequently increase the layout of the serious parts, but in addition to figure out how the strain and temperature distribution in the compressor distorts the rotors and casing and the way this, in flip, has an interactive influence at the performance.

Such calculating amenities are specially worthwhile for oil loose machines, within which temperature adjustments are a lot higher and hence make thermal distortion results extra major. in spite of the fact that, it confers merits in all situations, as better desktop instruments let production tolerances to be diminished and accordingly compressors might be outfitted with smaller clearances. 4 examples define the scope of the utilized mathematical version for 3 dimensional calculation of fluid stream and stresses within the stable components of the screw machine.

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Extra info for Screw Compressors, 1st Edition

Example text

50) can be found in Cengel and Boles (1989). The specific heat at constant pressure is a fluid property needed to calculate the specific enthalpy of the mixture. 52) where D0, D1, D2 and D3 are constants which vary for different fluids. Their values can be found in Sonntag and Borgnakke (2001). 51) gives the specific heat of the mixture. Even if the concentration of the liquid phase in the working chamber is equal to zero, this equation can be used to express the specific heat of the working fluid, which in this case is vapour.

If implicit time integration is employed, these prescribed values at time t0 are sufficient for the calculation. If, however, the three time level implicit scheme is used, values at the time t1  t0   t0 must be given. They are set at the same value as those at time t0 . 67) j 1 where index 0 determines the control volume in which the variable is calculated and index j defines the neighbouring cells. Symbol ni represents a number of internal cell faces between the calculating cell and its neighbouring cells.

The screw machine rotor geometry is described by the boundary and internal points in a sequence of rotor cross sections. A 3-D numerical mesh is then formed by connecting these points in consecutive cross sections. Preferably, the entire numerical mesh is formed of hexahedral control volumes with a righthand definition in which eight grid points form a right-handed coordinate system as in Figure 3-8. However, if hexahedral cells are not attainable, the numerical cells may degenerate to form either a prism, a pyramid or a tetrahedron, as shown in Figure 3-9.

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