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reaches nine, but the for-loop processes from the starting number through the end number. When the counter reaches nine, it is still less than or equal to the end value and, therefore, processes the loop once again. The next time through the loop, the counter is incremented to ten and then fails the test. Upon failure, control passes to the next line immediately following the for loop block. In our code, myAverage = mySum/10.0 is executed. After this statement is processed, we then have the average of the closing prices for the past ten days. In EasyLanguage, you can have for loops that loop from lower numbers to higher numbers or vice versa. If you loop from a higher number to a lower number, you must use the keyword downto or the program will not loop properly.

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To further increase transmission speeds, the 80216e standard specifies MIMO (multiple input multiple output) techniques for the network and the client devices This is especially the case in urban environments, where a signal is often split into several transmission paths due to reflection and refraction caused by objects in the direct line of sight between the transmitter and the receiver As the transmission paths have different lengths, each copy of the signal arrives at a slightly different time at the receiver as shown in Figure 519 For traditional GSM receivers, this phenomenon causes multipath fading due to the quickly changing paths and the resulting changes in interference of the different paths with each other In systems such as UMTS, rake receivers are used to combine the signal energy received from different paths (see 3).

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where [S] represents the eigenvector matrix3 of [Z] with the eigenvectors as columns and [ ] is a diagonal matrix with the eigenvalues as diagonal elements. The above identity can be proven directly from the definition of the eigenvector of [Z]. Thus, we need to determine the eigenvectors and the eigenvalues of the impedance matrix. Toward that end we choose the phase difference between the adjacent elements as x /2 and y /2, respectively, along x- and y-directions with uniform amplitudes. This particular selection of phase and amplitude distributions among the elements will allow us to treat the entire array as an infinite periodic structure of cell size a/2 b/2 radiating in the ( )-direction under Floquet excitation. In other words, the subarray grouping would not have any influence on the field solutions. For such an excitation all the elements inside a subarray (for that matter, all the elements of the entire array) have identical impedances, equal to the Floquet impedance corresponding to the scan angle ( ). This type of subarray excitation can be regarded as an eigenvector excitation, because the input voltage vector (of four dimensions because of the four elements in a subarray) and the input current vector are parallel. This voltage (or current) vector is one of the eigenvectors

1 A CCESS TO P HARMACEUTICALS Lack of access to drugs often leads to declines in health status (Lurie et al, 1984) This decline is explained by increased ambulatory care visits to obtain medications and the shifting of care to provider settings, such as hospitals and nursing homes, where prescription drug reimbursement is available (McCombs et al, 1994) The cost of prescription drugs and drug utilization vary considerably among individuals (Doonan, 2001) The poor, uninsured, and elderly have reduced access to drugs and rely on safety net providers for pharmaceuticals (Committee on the Changing Market Managed Care and the Future Viability of Safety Net Providers, 1999) With few exceptions, Medicare does not cover outpatient prescription costs Consequently, older Americans spend three times as much of their income on drugs as the general population.

In OnClickCalc(), each Cartesian point to be plotted is represented by the coordinates (xC,yC). The values of (xC,yC) are initially obtained from (X[j],Y[j]) at each end of the segment Sj(x). These coordinates are converted to the Windows coordinates Point.x and Point.y using Equations (5.1a) and (5.1b), respectively. It is not necessary to use an array for Point in this case as the coordinates are just temporary variables needed only for plotting the points on the curve. The last function in this application is ComputeCSpline(). This function gets input from the interpolating points that have been converted to the Cartesian coordinates earlier in the function OnLButtonClicked(). The function ComputeCSpline() produces the values of a[j], b[j], c[j], and d[j] for Equation (5.4) to generate the cubic spline based on the cubic spline algorithm discussed earlier. The following code fragment shows the function:

which is equal to the mutual impedance between two elements in an infinite array environment as deduced in 3. 5.9 Deduce the relations in (5.39). Obtain the reflection coefficient at the input port of the power divider in terms of the scattering matrices of the power divider network and the subarray.

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