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The key piece of code in the data access layer is the DAC The DAC is de ned as a separate project in the solution because it is independent of any business logic The DAC is composed of one or more classes that provide access to the database by calling SQL statements, stored procedures, or other queries (such as QueryDefs) To create the DAC: 1 Create a project for the data access layer, as described in 3, Building Projects 2 Open the Project Designer for the DAC Class Library project Right-click the project in Solution Explorer and select Properties from the context menu, or select Project | Properties from the main menu bar, or double-click on the My Project folder under the project in Solution Explorer to open the Project Designer 3 Select the References tab 4 Ensure that there is a reference to SystemData, as shown in Figure 816 If not, use the Add button to add the reference To make the classes in this library easier to use in the code, check SystemData in the Imported Namespaces list, as shown in Figure 816

The first term in (12.2.49) is due to Go, and the second term in (12.2.49) is due to the reflected Green's function G re !.

Step iv: To obtain self-consistent multiple scattering equations, we express the exciting field of cylinder l as follows:

(12.2.50)

+ a~N) (kz)Rg N n(kop , k z , r - r l )]

Agency Department of Homeland Security (DHS) U.S. Department of Justice (DOJ)

Figure 816 The References tab in the Project Designer for the DAC de nes the references to the NET Framework database libraries

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In matching the coefficients to scattered field from cylinder j, a problem exists. That is, the reflected term in (12.2.49) is integration of dk p from 0 to 00 while that of (12.2.50) is dk z from -00 to 00. This is because in the reflected term, if dk p integration is performed in the complex kp-plane, it will have to include a contribution of a branch cut of kl z = (kr - k~)1/2 of the bottom half-space E1 as well as possibly a Zenneck surface wave pole [Kong, 2000]. However, when we examine the exponential terms, dependence involving k oz in the reflected term of (12.2.48), we find that, with Zj =

-d + L j /2,

Zj)) = exp (ikoz(Z' + d)) (12.2.51) The sine ((k oz + k~)Lj/2) shows the conical pattern with k oz close to -k~ which is real, while ZI in (12.2.51) is from -d to -d + L j . Thus the contribution of evanescent waves in dk p integration will be small. Hence we approximate the second term in (12.2.49) as follows. exp(2ikoz (zj z dk z (12.2.52) - kk o 0 k 0 0 op Integration is only over dk z from 0 to k for reflected term. Once the approximation is made, the exciting field coefficients a~M)(I) and a~N)(I) can be equated to the sum of incident, reflected, and scattered fields. We obtain the following self-consistent Foldy-Lax multiple scattering equations in equating the exciting field of cylinder l to its internal field as represented by (1.6.75) and (1.6.76). Thus, for -00 < k z < 00, l = 1,2, ... ,N, we obtain

+ d)) exp(-ikoz L j /2) exp (ikoAz' -

aU'vI)(I)(k z ) =AMM(kop, k z, k pp, k z, a l"n )c(M)(I)(kz ) n n + A~N (k op , k z , k pp , k z , al)c~'V)(I)(kz)

8

+~ N (

L ) 2;

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00 00 ( -00

H(l)

At this point, decide which data provider you will use in your DAC and import its associated library using the Imported Namespaces list shown in Figure 816 The common data providers and their associated libraries are:

n-n'

[e~~)(j) (k~)Rg A~M (k op , k z , k~p, k~, aj)

t( ;:) n,r;=l: -'

U(k z - k))

For SQL Server, import the SystemDataSqlClient namespace For Access using OleDb, import the SystemDataOleDb namespace For any ODBC data source, import the SystemDataOdbc namespace To support any data source from any data provider, import the SystemDataCommon namespace

dk;sinc ( (k;

,,2ik, ("

Department of Energy (DOE)

In-n,(kop!Pj - Pll)e-i(n-n') PjPI-ikz(ZJ-ZI) ROl(k z )

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