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Print setup allows the user to de ne the printer and other print settings before printing In some applications, the Print menu option provides this feature and the user must view this dialog every time printing is required In this example, the features are separated to give the user an easy way to print to the default printer without accessing the setup dialog Either way you prefer, this feature is easy to implement because it uses the same PrintDocument control and associated code required to implement the Print feature To implement a Print Setup feature: 1 Ensure that there is a way for the user to select a Print Setup This is most logically de ned near the Print option In some cases, the setup is handled in the Print option, and a separate Print Setup option is not desired 2 Add the PrintDialog control to the form from which the user initiates the Print Setup process This is normally the same form containing the PrintDocument control Give the control a logical name, such as PTPrintDialog 3 In the event handler for the control that initiates the Print Setup, write the code required to display the Print dialog The code involves associating the appropriate PrintDocument control with the Print dialog, displaying the Print dialog, and then, if the user clicked OK, printing the document as follows:

Effective Permittivity Scattering Attenuation and Coherent Propagation Constant Coherent Reflection and Incoherent Scattering From a Half-Space of Scatterers A Simple Dense Media Radiative Transfer Theory

2.1 2.2 2.3 2.4

496 500 505 510

3.1 3.2 3.3

4

512 514 518

Multiple Scattering Equations Computational Considerations Results and Comparisons with Analytic Theory Simulation of Absorption Coefficient

4.1 4.2 4.3 4.4

533 541 545 547

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For example, monoclonal antibody therapy, which is based largely on research con ducted by an Argentinean-born British molecular biologist and a Ger man immunologist in 1975, was rst exploited commercially in the United States Furthermore, the trajectory of that commercialization il lustrates many of the challenges inherent in realizing practical bene ts from theoretical studies in biotech The rst rm to commercialize monoclonal antibodies, Hybritech, was founded in 1978 in the United States Hybritech s track record also high lights many of the challenges faced by next-generation biotech rms Scien tists at Hybritech, like investors on Wall Street, assumed that monoclonal antibodies, which are proteins normally produced by the body in response to a foreign protein, were the magic bullets that could cure cancer and other diseases.

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PTPrintDialogDocument = PTPrintDocument Dim oResult As DialogResult = PTPrintDialogShowDialog If oResult = WindowsFormsDialogResultOK Then PTPrintDocumentPrint() End If

In scattering of waves by densely packed media, the particles do not scatter independently. The correlated scattering between particles has to be taken into account. This was verified by controlled experiments [Ishimaru and Kuga, 1982; Mandt et al. 1992; West et al. 1994]. In Volume III, we study extensively the analytic theory of dense media scattering. These include the Feynman diagrammatic methods leading to the Dyson equatiou and the Bethe-Salpeter equation. To make analytic theory numerically tractable, approximations have to be made on the mass and intensity operators. In Volume III, we study the quasi-crystalline approximation (QCA), the quasicrystalline approximation with coherent potential (QCA-CP), the correlated ladder approximation and the dense media radiative transfer theory (DMRT). These approaches take into account the pair-distribution functions of particle positions for which we have used the Percus-Yevick pairdistribution functions as illustrated in 8. Near-field coherent wave interactions are also included. In this chapter, we study Monte Carlo simulations of three-dimensional dense media. In Section 2, we first formulate a simple analytic model for scattering by dense media. In Section 3, we use a volume integral equation approach for Monte Carlo simulations of spheres and spheroids. In Section 4, we use the T-matrix approach. Scattering simulations include up to 5000 particles. We simulate the extinction rates and the phase matrices. The scattering results compare well with dense media analytic theory for the case of spheres. However, for complicated cases of densely packed media such as densely packed nonspherical particles, numerical simulations of Maxwell's equations become mOre attractive.

only applies to non-near field interaction. For near field interaction, Green's functions G 1 and G 2 have similar rate of variations. Thus we separate out a distance, say lA, outside of which G 2 is much more rapidly varying spatially than G 1 . Based on the observations above, we decompose the upper medium Green's function into near field and non-near field interactions

(6.4.28)

S 2':

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