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Since the integrated system is constructed in a way that overlaps the execution of XGC with stability check by MHD, it is essential that the result of the stability check is available by the time it is needed by XGC, otherwise the large number (1000s) of processors running XGC will remain idle offsetting any bene t of a coupled simulation Another constraints is the overhead of the coupling framework imposed on the simulations This requires effective utilization of memory and communication buffers, specially when the volume of the coupled data is large Finally, the data transfer has to be robust and ensure that no data are lost A Prototype Coupled Fusion Simulation Using Seine Since the Fusion project is at a very early stage, the scientists involved in the project are still investigating the underlying physics and numerics, and the XGC and MHD codes are still under development.

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Figure 1.7. The symmetry characteristics of (a) s, (b) p, and (c) sp n (hybrid) atomic orbitals. The shapes of the electron distributions are similar if one ignores the phases.

However, the overall coupling behaviors of the codes is reasonably understood As a result, we use synthetic codes, which emulate the coupling behaviors of the actual codes but perform dummy computation, to develop and evaluate the coupling framework The goal is to have the coupling framework ready when the project moves to production runs The con guration of the mock simulation using the synthetic codes is shown in Figure 146 In this gure, the coupling consists of two parts, the coupling between XGC and MI and the coupling between MI and MHD..

(5.28)

-L(a)

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is huge, guaranteeing that Ethernet will be around for some time to come. There will always be improvements inserted into existing networks, but they will not cause a total dumping of the current Ethernet network.

To edit a field, double-click the field s text to open the In-Place Text Editor. Select the text, right-click, and choose Edit field. The Field dialog box opens. You edit a field in the same way that you define the field originally. When you re done, click OK. The field is reevaluated immediately. Close the In-Place Text Editor to place the edited field. By default, a field is evaluated and updated, if necessary, whenever you open, save, plot, eTransmit, or regenerate a drawing. (See 28 for information on eTransmitting a drawing.) You can change when AutoCAD updates a field by choosing Tools Options and clicking the User Preferences tab. In the Fields section, click Field Update Settings. Check or uncheck the items that you want, and then click Apply & Close. Click OK to close the Options dialog box. You can manually update a field if you want. For example, you may have an object field that displays the radius of a circle. If you resize the circle, you probably want to update the field. To update a field, double-click the field to open the In-Place Text Editor. Select the text, rightclick, and choose Update Field. Close the In-Place Text Editor to return to your drawing. Another method is to select the field and choose Tools Update Fields. You can select as many fields as you want.

350 300 N+F Avg load imbalance: 28.3994

State i is any individual conformation along the folding funnel. Q i varies between the unfolded state, U (where it has a value of 0), to a maximum value of 1 in the native state, N . Thus, this parameter is expected to increase on folding at the same time as the value of S decreases. In this representation, localized energy minima which in a pathway are designated as folding intermediates instead are represented as folding traps. In other words some proteins in the population may occupy this localized minimum but others may not. Folding traps are therefore not obligatory in the sense that intermediates in a folding pathway are. The power of this representation of protein folding is that it allows us to explain Levinthal s paradox. Distinct structures for which experimental evidence have been obtained such as molten globules, folding traps and transition states

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