winforms pdf 417

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4. At the Select object to revolve: prompt, select the path curve object. 5. At the Select object that defines the axis of revolution: prompt, select the axis of revolution object. 6. At the Specify start angle <0>: prompt, press Enter to accept the default of 0 (zero) or type a start angle. 7. At the Specify included angle (+=ccw, -=cw) <360>: prompt, press Enter to revolve the surface 360 degrees or type a positive or negative angle. You may need to create the path curve and the axis in a different plane than the one you use when revolving them. You can draw the path curve and axis in one UCS and use REVSURF in another. If the object doesn t come out in the right direction, you can rotate the entire object when completed. Rotating objects in 3D is covered in the next chapter. REVSURF retains the original path curve and axis objects. It helps to draw them in a different layer and color so that you can easily erase them afterward. Otherwise, they re hard to distinguish from the revolved surface. Having them on a separate layer also helps if you need to redo the revolved surface you can more easily avoid erasing them when you erase the revolved surface.

Synopsis Convection heat transfer and ventilation in rotating electrical machines is poorly understood, yet thermal constraints impose limitations on the power capability of many motors and generators. CFD has the potential to provide understanding of the cooling process and aid in the design of improved machines. This chapter describes research done by The University of Nottingham in collaboration with ALSTOM Electrical Machines Limited to investigate airflow and heat transfer in an electric motor. The particular area of interest was the cooling of end windings in a large induction motor. CFD modelling was developed, using the commercial CFD code Fluent, and compared with results from an extensive programme of experimental measurements. The chapter will describe the problems that were faced in applying CFD to electrical machines in modelling: The complex geometries of the end winding coils; The interaction between the rotor and stator.

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Operating system memory requirement This is the portion of memory consumed by OS processes. Examples of UNIX processes are cron, terminal manager, sendmail, TCP port listener (inted) Volume Manager, RPC registry, route discovery daemon (in.rdisc), NFS, SNMP, and mount daemons. These processes can add up to 100 or more megabytes of memory and are provided in vendor OS documents. Kernel requirements This is the amount of memory used by the kernel and depends on tunable parameters such as Inode cache, directory lookup buffer, and so on. System Library memory requirement This component of the used memory is fairly static and is actively used by libraries. On UNIX systems, the libraries reside primarily in /usr/lib directory. Application and database requirement A large chunk of memory is used for background processes and associated with database engines and applications. This portion of the memory is initially occupied by the application and later shared by various user requests. The size of the shared memory segment is usually decided by application or database administrators as part of tunable parameters. This portion is independent of the number of users and can be sized separately.

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15.5.1. Two-wavelength Phase Measurement As long as the fringes generated at each wavelength can be resolved by the detection system, two measurement wavelengths can be used with phase-shifting techniques (Cheng and Wyant, 1984; Wyant, et al., 1984; Creath et al., 1985; Fercher et al., 1985; Creath and Wyant, 1986a; Creath and Wyant, 1986b; Wyant and Creath, 1989). These techniques are used to measure objects with height discontinuities larger than (l/4 at either of single wavelengths. By using the information from a second wavelength, the height range of the measurement can be signi cantly increased. A two-wavelength phase measurement is performed by rst taking data at one wavelength while shifting the phase in appropriate amount for that wavelength. The modulo 2p phase is then calculated for this rst wavelength. The illumination wavelength is then changed, and data are taken at the second wavelength with the appropriate phase shifts; the modulo 2p phase is then calculated for this second wavelength. These two modulo 2p phase measurements can then be combined to produce a modulo 2p phase corresponding to a long synthetic wavelength, which is the beat between the two measured wavelengths. The phase corresponding to the new synthetic wavelength can be described as l2 l1 je j1 j2 2pOPD l1 l2 2pOPD le

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