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Protected Const CN_LastUpdateUser As String = "LastUpdateUser" Protected Const CN_RowState As String = "RowState"

(12.3.45)

"2)

(12.3.46)

-TE( _ _ d ] TE(p) w lm RgH n kpl,kzl,P-Pq,z "2)

The constants are de ned with the Protected modi er, so they can be used in any class that inherits from the base business object class When the constants (or resource strings) are in place, the business object can call the ExecuteDataTable method to retrieve the DataTable and populate each business object property with its associated column value:

(12.3.47)

Thus we get the Foldy-Lax multiple scattering equations, similar to 9,

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+2: 2:

(12348) . .

TE(q)

Public Shared Function Create(ByVal prodID As Integer) As Product Dim prod As Product ' Populate the object Dim dt As DataTable dt = DACExecuteDataTable( _ MyResourcesSP_ProductRetrieveByID, _ DACParameter(CN_ProductID, prodID)) ' Create a new instance prod = New Product() With dtRows(0) prodProductID = CType(Item(CN_ProductID), Integer) prodProductName = Item(CN_ProductName)ToString

TE(q)

+2: 2:

(12349) ..

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where a'fnM(q) , a'fnE(q) are incident field of the current source onto cylinder q. The equations are basically identical to that of (9.3.74) and (9.3.75) in 9. This is because there is no coupling between different l because each l corresponds to a specific k z . Neither is there coupling between TE and TM waves because the cylinders are perfect electric conductors as shown in (9.3.51)-(9.3.60) of 9. This is particularly important when one considers the dimension of the matrix equation associated with Foldy-Lax multiple scattering equations. The decoupling reduces significantly the dimension of the matrix equation, as one needs only to solve Foldy-Lax equation for each waveguide mode separately. This decoupling is useful when multiple waveguide modes are excited for waveguides of moderate thickness. For such cases, if discretization in the z-direction is done using subsectional basis functions, a large number of basis functions are required and they are all coupled in multiple scattering. To determine a'fnM(q) , afnE(q) , we use the results of the primary Green's function of the previous section. Note that the primary Green's function is translational invariant in the horizontal plane.

prodProductNumber = Item(CN_ProductNumber)ToString prodPrice = CType(Item(CN_Price), Decimal) prodDescription = Item(CN_Description)ToString prodProductType = CType(Item(CN_ProductType), Integer) prodStockType = Item(CN_StockType)ToString End With ' Reset the state to unchanged prodDataStateChanged(EntityStateEnumUnchanged) Return prod End Function

Gp (15, z, 15', z') . It = Gp (15 -

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z, 15'

(12.3.50)

Thus the incident field from the magnetic surface current sOurce M s onto cylinder q for 115 - pql < 115' - pql is, from (12.3.32) and (12.3.34),

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