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Another approach to detecting airborne biologicals with high selectiv ity is to use pathogen-speci c DNA probes on a chip. One of the most promising technologies is under development by the Northwestern Insti tute for Nanotechnology, which has a chip that can quickly indicate the presence of a speci c biological in the atmosphere. A major limitation of this technology is that chip processing can require several hours. An alter native to the DNA detector chip technology is to use an antibody-based de tection system that circumvents the time and complexity associated with processing DNA. An example of a system that uses real-time detection is RAPTOR, which is under development at the United States Naval Re search Laboratory. In the area of containing the spread of disease following the expo sure of a population to a biological, a number of experimental informa tion systems, such as the U.S. Air Force s Lightweight Epidemiology Advanced Detection and Emergency Response System (LEADERS), are under development. LEADERS is a Web-based system designed to em power medical personnel to track symptom outbreaks as they are re ported by hospitals in real time. In the event of a biological attack, it is intended to allow public health of cials to map geographic regions where outbreaks are occurring and to determine the response capabili ties of various medical facilities.

t=1 1=1

(8.3.6)

Click the Preview tab to con rm the results When you obtain the desired results, save the code snippet The code snippet is automatically added to the Code Snippet Manager in the de ned folder, so it is immediately ready for your use in the Code Editor Any time you nd yourself typing the same set of code or looking up some syntax you do not use very often, consider building a snippet for that code As you build your code snippet library, the code for many of your coding tasks will be at your ngertips Your code snippets are yours Modify them, reorganize them, and create your own so that you can build a very ef cient, personalized snippets library

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On the other hand, if the particles were totally uncorrelated, the average number of particles of size aj in the spherical shell surrounding a particle of size ai at a distance r away would be nj (Nj - Oij) 2 (Cij(r))unc = N 41fr dr (8.3.7) where unc stands for uncorrelated, 41fr 2dr is the volume of a spherical shell of thickness dr, and Oij is the Kronecker delta function which corrects the inability of the tagged particle to be in the spherical shell. The pair distribution functions gij(r) are then calculated from (8.3.6) and (8.3.7) by means of the relation

(Cij(r)) = Nj ~ ~ cIt (8.3.8) (C(r)) une TNn(N-J)(41fr2dr)DD ZJ ZJ t J J ZJ t=l 1=1 Generally, a pair of particles is considered to be uncorrelatcd when their separation is greater than 5Rij , and the values of pair distribution functions gij (r) are taken to be unity for r > 5Rij . The pair distribution functions vanish, gij (r) = 0 for r < Rij, due to the non-interpenetrable characteristic of macroscopic spheres. gi' r =

The simulation of random distribution of particles using sequential addition method is different from the Metropolis technique in that the realizations of discrete random media are constructed by depositing spheres one by one into the box subject to the same condition of no overlap with all other particles. Thus, in the sequential addition method the particles do not move, and there is no shuffling of particles. The procedures adopted are as follows.

Step 1: Generate a random test site to accommodate a new particle. The x, y, and z coordinates of this trial position within the cube are determined by three independent random number generators as

For the Purchase Tracker sample application: If desired, build a code snippet that inserts the Property statement structure that includes all the code that calls the DataStateChanged method You can then use this snippet to create properties that include the majority of their required code

(8.3.9)

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