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Creates a link or links between the new element and the existing ones This behavior is determined by the element merge directive of the target element that is, the one the tool was dragged onto Fires rules that update the diagram to show the new element These are determined by the shape maps, as we saw in the previous chapter The last point is important We rely on xup rules to maintain, on the screen, a presentation of what is going on in the model All the techniques in this chapter and indeed much of the custom methods you might write deal only with the domain classes and domain relationships Once we ve set up the shapes and their mappings to the domain model (as discussed in 4), we can just work with the domain model, leaving the diagrams to look after themselves

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of the displacement vector ( >) at the adjacent interfaces are applied as:

5. Move your mouse pointer to the payment column and enter $100, as shown in Figure 2-17. 6. Click the Auto Apply Payment button. QuickBooks automatically applies the payment to the outstanding invoices, oldest rst. 7. Click Save & Close to exit the window.

where linear material properties t are assumed, i.e. D{ = eiEi + Pi- Though the piezoelectric polarisation vector can have an arbitrary direction only the component along the growth direction will influence the electronic properties of a quantum well structure and therefore only this component will be considered here. For an arbitrary n-layer structure equation (7.57) gives a system of n 1 linear equations:

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The Toolbox Tools are defined in the DSL explorer under Editor\ToolboxTabs\ YourTab\Tools You need to define a tool for each item you want to appear on the toolbox (Figure 5-1) The tab name is the heading that appears above each group of tools in the toolbox By default, you have just one tab, named after your language, but you can add more tabs in the explorer if you wish

Click this button to apply payment Figure 2-18: Summary of outstanding invoices for customer Jason Burch.

which can be solved provided appropriate boundary conditions across the structure are defined. Though there are no constraints on the choice of the boundary condition, the natural choice are the 'hard wall' boundary conditions, which enforce the total

There are two kinds of tools: element tools and connection tools At runtime, you operate an element tool by dragging it from the toolbox to the diagram; for a connection tool, you click it and then drag it between the two elements you want connected (or click them in succession) The most common scheme

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Now that you have entered the transaction, you can view the applied cash payment in the Customer Register window by following these steps: 1. Make sure that you are in the Customers Navigation window. 2. Click the Customer Register icon, as shown in Figure 2-19. A list of customers will appear. Choose Jason Burch from the drop-down menu of customers. A Customer Register that shows a chronological list of all transactions for Jason Burch appears. The most recent transaction will be a $100 payment. Exit the screen by clicking the X in the upper right corner of the Customer Register (not the QuickBooks program screen).

te is used to represent the permittivity in this chapter to distinguish it from e which is the commonly accepted symbol for the components of strain.

is to provide an element tool for each class that is mapped to a shape on the diagram and a connection tool for each relationship mapped to a connector Each tool has a name, caption, tooltip, toolbox icon, and help keyword; these are set in the properties window (Figure 5-2) In addition, an element tool can have a cursor icon that shows while you are dragging it, and a connection tool can have source and target cursor icons that show while waiting for you to select the source and target of the connection

Summary

potential drop across the structure to be zero. All other possibilities would imply that the quantum well structure acts as a voltage source in the closed circuit. For a periodic structure (e.g. a superlattice) the hard wall and the periodic boundary conditions are equivalent. Knowing the boundary condition the necessary nth equation of the system is defined and reads:

where Li is the width of the i-th layer. The solution of the system gives a rather simple equation:

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