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3 De ne appropriate properties and methods for the class Because BindingList is a generic collection, it has the standard (Of T) syntax, where T is the speci c data type that you want it to accept In this example, the BindingList accepts only objects created from the Purchase class This ensures that only Purchase objects are added to

(8.5.28)

Japan is a densely populated group of islands with area of less than 38 mil lion hectares in which 128 million people live and work. In comparison, the state of California supports a population of 35 million people on about 42 million hectares of land. The major centers of Japanese biotech activity are located in and around Tokyo, Kobe, Kyoto, and Osaka, as illustrated in Figure 7.11. Tokyo, the site of Tokyo University and its various af liated

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The algorithm of spheroidal particle placement will be applied in the next chapter of dense media models and simulations. It is noted that S(>') is non-negative over the interval 0 :s; >. :s; 1, and vanishes at both end points when>. = 0 and 1. As .\ changes from 0 to 1, the location r(.\) will trace a path starting at rB and ending at r A. The following three situations for two ellipsoids A and B can be distinguished:

(i) A and B non-overlapping: The path r(.\) pass through the region outside both particles, where both FA and FB are greater than 1, and F(r,.\) > 1. Thus, max S(>') attains values greater than 1.

0'::::>''::::1

(ii) A and B overlapping: The minimum value of S(.\) is less than 1 inside the overlapped region oftwo particles, where both FA and FB are less than 1. This precludes the path r(>.) from entering the region outside both particles, and hence max S(.\) is less than 1.

this collection If you want to follow the Factory method design pattern introduced in the preceding chapter, add a Create method to the detail collection class In the Create method, create appropriate objects, and add them to the collection For the PurchaseList example, the Create method looks like this:

0'::::>':::;1

(iii) A and B externally tangent: At the touching point F(r, >') is equal to 1, which implies S(.\):S; 1 for all .\. This means that the path r(.\) cannot go outside both particles, so that max S(>') is equal to 1.

0'::::>':::;1

FIGURE 7.11 Major biotech activity in Japan. laboratories, is also host to numerous corporate headquarters. It s also home to the in uential National Institute of Advanced Industrial Science and Technology (AIST), as well many of the biotech-related centers that it funds. For example, Tokyo hosts the Japan Computational Biology Re search Center (JBIRC), which focuses on gene sequences, proteins, and the modeling of cellular biology. According to the Japan Statistics Bureau and Statistics Center, the pop ulation of Tokyo in 2002 was about 12.3 million, or about 10 percent of Japan s total population. As the center of commerce in Japan, the urban sprawl around Tokyo is home to many in uential companies and research centers in science and technology, including biotech. For example, Tsukuba, located at the outer edge of the Tokyo metropolitan area, is a planned community with a focus on academics and high-technology re

Based on these observations, Ferram and Wertheim [1985] proposed the contact function as given in (8.5.11). They also proved that the object function

Public Shared Function Create(ByVal custID As Integer) As _ PurchaseList Dim purchList As PurchaseList ' Create a new instance purchList = New PurchaseList ' Populate the object If custID = 1 Then purchListAdd(PurchaseCreate(1)) purchListAdd(PurchaseCreate(2)) End If Return purchList End Function

S(>') has a unique maximum in the interval 0::; >.::; 1. Various optimization methods can be applied to obtain the maximum value of S(.\). For example, Brent's method [1973], due to the concavity property of S(>'), converges quickly to the maximum. The explicit expression of the derivative of the object function S(>') is given as

(8.5.29)

Allen, M. P. and D. J. Tildesley (1989), Computer Simulation of Liquids, Oxford University Press, New York. Baxter, R J. (1968a), Percus~Yevick equation for hard spheres with surface adhesion, J. Chem. Phys., 49(6), 2770~2773. Baxter, R J. (1968b), Ornstein-Zernike relation for a disordered fluid, Aust. 1. Phys., 21,

563~569.

NOTE: The code in the Create method that hard-codes the values is temporary until the data can be retrieved from a database, as described in 8

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