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NIH is also the largest federal supporter of applied research in the United States. Although the relative percentage of the NIH expenditure on bioterrorism-related research and development seems small by compari son to the total budget, NIH is the lead research agency, ahead of the U.S. Department of Defense, which focuses on military rather than civilian populations. In terms of all federally funded academic research and de velopment, the NIH accounts for 60 percent, compared to 9 percent for the Department of Defense. Because of the overlap in what constitutes civilian and military bioter rorism threats, there is often cross-fertilization between civilian and mili tary departments in the government. For example, the 2003 U.S. Defense budget allotted $105 million to NIH for a new bioterrorism research lab oratory in Fort Dietrich. In the same year, the DOD proposed to spend $767 million on counterterrorism research and development as part of the U.S. Army Medical Research and Material Command (USAMRMC) at Fort Dietrich. However, the relationship between the DOD and civilian work in biotech isn t always symbiotic. For example, there are funds available to aid military physicians and other health-care workers regarding bioterror

Moisture (%) 5.00 7.50 10.0 12.5 15.0 17.5 20.0 22.5 25.0

0.33 0.8060 0.7758 0.7464 0.7092 0.6385 0.5819 0.5453 0.5220 0.4986

Length (in wavelengths) horizontal polarization 0.5 0.6 0.7 0.8 0.9 0.7918 0.7841 0.7777 0.7720 0.7671 0.7591 0.7514 0.7442 0.7377 0.7330 0.7290 0.7205 0.7132 0.7072 0.7017 0.6855 0.6743 0.6676 0.6614 0.6569 0.6088 0.5990 0.5919 0.5862 0.5758 0.5504 0.5393 0.5365 0.5248 0.5193 0.5149 0.5042 0.4961 0.4896 0.4840 0.4827 0.4925 0.4755 0.4695 0.4642 0.4678 0.4577 0.4508 0.4454 0.4409

8

1.0 0.7636 0.7286 0.6973 0.6520 0.5766 0.5149 0.4792 0.4596 0.4366

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Table 6.4.5 Computed soil emissivities at L-band. Horizontal polarization; rms height = 0.1 wavelength, observation angle = 50 degrees. Moisture (%) 5.00 7.50 10.0 12.5 15.0 17.5 20.0 22.5 25.0 Correlation Length 0.4 0.5 0.9545 0.9541 0.9410 0.9400 0.9261 0.9276 0.9024 0.8995 0.8469 0.8508 0.8104 0.8036 0.7744 0.7684 0.7412 0.7361 0.7123 0.7048 (in wavelengths) vertical polarization 0.6 0.7 0.8 0.9 0.9550 0.9563 0.9592 0.9578 0.9423 0.9439 0.9454 0.9408 0.9268 0.9284 0.9302 0.9318 0.8995 0.9006 0.9018 0.9031 0.8468 0.8480 0.8493 0.8510 0.8041 0.8054 0.8073 0.8091 0.7696 0.7716 0.7734 0.7655 0.7363 0.7382 0.7402 0.7423 0.7092 0.7113 0.7134 0.7073

0.33 0.9565 0.9437 0.9308 0.9081 0.8568 0.8202 0.7841 0.7535 0.7272

1.0 0.9603 0.9468 0.9333 0.9043 0.8524 0.8107 0.7714 0.7440 0.7130

The appcon g le for your Class Library project may appear to work This is because the setting you de ned in the Project Designer is used as the default Using application settings to store the connection string makes it easy for the application to connect to a database Any code in the DAC can reference the connection using MySettingsPTConnectionString

Table 6.4.6 Computed soil emissivities at L-band. Vertical polarization; rms height = 0.1 wavelength, observation angle = 50 degrees.

R&D Expenditure ($B)

k tZl k tpp, k U, aJ')c(N)(j)U(k' ) n tZ (12.2.58a)

NM(k iPl k iz, k ipp, k iz, aj ) cn (M)(j)U(k iz ) An NN(k n + A n tp, k tZ, k tpp, k aJ )c(N)(j)U(k tZ )

= _ Evi (_1)n e -in</J,-in7r/2S01 (k iz )

(12.2.58b)

For the Purchase Tracker sample application: Copy the connection string for the PurchaseTracker database from Server Explorer to the Clipboard, as detailed in this section Create a setting for the connection string in the data access component Class Library project (PTDAC), as detailed in this section Name the setting PTConnectionString Paste the connection string from the Clipboard to the Value column of the new setting Open the appconfig file for the data access component Class Library project (PTDAC) Copy the entire connectionStrings tag, and paste it into the appconfig file for the Windows Application project (PTWin) At this point, there is no code in your data access component yet, so there are no new features to try out

Equations (12.2.57a) and (12.2.57b) are the coupled equations for the downward-going waves of the first-order solution, and (12.2.58a) and (12.2.58b) are the coupled equations for the upward-going waves of the first-order solution. They can be solved readily. Substituting (12.2.55)-(12.2.56) into (12.2.54) gives the far-field solution of the first-order scattered field in the form as given in (12.2.6), where

[Rg A~M (k sp , k sz , kipp, -kiz , aj )c~M)(j)d( -kiz )

+ Rg A~N (k sp , k sz , kipp , -kiz, aj)e~N)(j)d(-kiZ )]

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