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Like the Java Editor, Spring IDE s XML Editor provides content assist proposals on request. The content assist can be triggered on elements of the Spring DTD and XSDs, including elements defined in Spring 2.0 extension namespaces. Content assists are available on the following elements: Bean class name: Spring IDE provides a list of all classes and packages that match the prefix given by the user. Bean property name: Displays all JavaBean property names that are defined on the bean s class. The bean class needs to be specified for that content assist to work. Lifecycle method: For methods like factory-method, init-method and destroy-method, Spring IDE lists all available methods of the bean class that match the requirements of the Spring Container for a certain type of lifecycle method. Bean references: All bean definitions of the current Beans Config and all associated Beans Config Sets are listed.

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Within ALSTOM Electrical Machines Limited, CFD is finding a place right at the heart of the development process. New and untested developments, components with particularly complex geometry (strip on edge field winding) or which are located in areas of extreme turbulence (field winding supports) have an obvious affinity with the CFD approach. Some structures, such as end-windings have proved to be beyond any previous predictive capability and yet are more suited to CFD methods.

If you change tools in a toolbar and open a context menu, the menu options change to reflect choices with that particular tool. Likewise, a context menu opened on a palette offers menu options respective to the palette, as shown in Figure 1.15. FIGURE 1.15

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53 A Elwalid, D Mitra, and R Wentworth, A new approach for allocating buffers and bandwidth to heterogeneous, regulated traffic in an ATM node, IEEE J Select Areas Commun, vol 13, no 6, pp 1115 1127, Aug 1995 54 L He and A Wong, Connection admission control design for Globeview-2000 ATM core switches, Bell Labs Tech J, pp 94 111, Jan Mar 1998 55 F Lo Presti, Z-L Zhang, J Kurose, and D Towsley, Source time scale and optimal bufferrbandwidth trade-off for regulated traffic in an ATM node, IEEE Infocom 97, pp 676 683, Mar 1997 56 B Jamoussi, S Rabie, and O Aboul-Magd, Performance evaluation of connection admission control techniques in ATM networks, IEEE Globecom 96, pp 659 664, Nov 1996 57 G Ramamurthy and Qiang Ren, Multi-class connection admission control policy for high speed ATM switches, IEEE Infocom 97, pp 965 974, Mar 1997 58.

l,, 1 = 1, ...,L , have the same pdf, so we drop the subscript 1 to Clearly, all G,,, simplify the notation. From (6.9) to (6.12), we arrive at the pdf of,S , ,

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Figure 5.2. The SHMO orbitals of allyl, butadiene, and pentadienyl. The vertical scale is energy in units of j j, relative to . Coe cients not speci ed may be obtained by symmetry.

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B T Doshi, Deterministic rule based traffic descriptors for broadband ISDN: worst case behavior and connection acceptance control, IEEE Globecom 93, pp 1759 1764, Nov 1993 59 D Mitra and J A Morrison, Independent regulated processes to a shared unbuffered resource which maximize the loss probability, unpublished manuscript, 1994 60 T Worster, Modeling deterministic queues: the leaky bucket as an arrival process, Proc ITC-14, J Labetoulle and J W Roberts, Eds, Elsevier, New York, pp 581 590, 1994 61 N Yamanaka, Y Sato, and K I Sato, Performance limitations of leaky bucket algorithm for usage parameter control of bandwidth allocation methods, IEICE Trans Commun, vol E75-B, no 2, pp 82 86, 1992 62 S Rajagopal, M Reisslein, and K W Ross, Packet multiplexers with adversarial regulated traffic, IEEE Infocom 98, pp 347 355, Mar 1998 63 J Song and R.

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The simulated solutions based on these methods appear in Fig. 10.9. As expected, the fourth-order method is much more accurate than Heun s method. The plot in Fig. 10.9 was generated using MATLAB, and the code for this appears in Appendix 10.A as an example. (Of course, previous plots were also produced by MATLAB codes similar to that in Appendix 10.A.)

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Fig. 10.9 Vertical force predictions for vehicle underbody shapes It is interesting to observe that Fig. 10.8(a) displays both the shock wave, at the circular extremity of the high-pressure region, and the blast wind continuing to emanate from the source. Figure 10.9 shows that the angled underbody experiences a lower peak force, approximately 37 per cent of that experienced by the flat underbody. The angled underbody reduces the reflected component of the blast and therefore reduces the developed underbody pressures. In addition, the duration of the angled body force is less than that of the flat underbody, as there is less repeated reflection between the ground and the vehicle. The angled underbody therefore receives a much lower momentum transfer from the blast, thereby potentially reducing the structural damage and potential injury to the vehicle occupants.

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