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A billing statement (or statement, as the term is used by QuickBooks) is another document that identi es charges to a customer. A statement always re ects past charges that a customer has accumulated over a period of time. For example, a law rm might issue a statement for services performed in the past month. QuickBooks presumes that you will use invoices, rather than statements, when sales taxes or discounts are applied. Service companies such as doctors, dentists, and consultants primarily use statements, because sales taxes are not generally imposed on such services. You might also opt to use a combination of invoices and statements for billing your customers. For example, you may issue an invoice at the outset of the transaction to memorialize contractual terms quantity, price, time and place of delivery, and payment. You may follow up by sending the customer reminder statements as to invoiced items provided in the past. QuickBooks automatically tracks the information necessary to create reminder statements. Table 14-1 provides a useful summary of considerations for deciding whether you should use invoices or statements.

which do not make this imposition (parameterisation) within them all of the electron states, within both the conduction and valence band can be derived from the constant free electron mass. Therefore the kinetic energy operator remains

Partial Classes Partial classes are the feature of NET languages that allows the methods of one class to be compiled from several different les All the generated classes are partial, allowing you not only to add methods of your own to a class in a separate le, but also to add overrides of methods de ned in

236 Part III Preferences and Data Management Table 14-1 When to Use an Invoice versus a Statement

and hence the boundary conditions are set as continuity in both wave function and derivative note wave function, and not envelope Junction. Such methods are the subject of later chapters, for example, 11. However within the auspices of this very successful model of semiconductor band structure, allowance has to be made for the additional complication of variable mass. As discussed in Section 2.6, this can be achieved with the original Schrodinger equation applied to each region, taken together with boundary conditions for matching solutions at the heterojunctions between the regions of different effective mass. However, fundamentally both of these conditions can be incorporated within one Hamiltonian which is valid throughout all space at once. Its construction derives from the cornerstones of quantum mechanics all physical observables can be represented by linear Hermitian operators [12], With this aim consider the classical (non-relativistic) kinetic energy: