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Zwaneveld (1997) also studied a routing problem for train units over railway infrastructure. In this problem, one is looking for a set of routes for trains in a 1-hour period where arrival and departure times are xed. He develops a solution approach based on state of the art techniques from the eld of Operations Research. This approach is applied to a number of railway stations in the Netherlands. Compared to the problem of Zwaneveld, our problem is complicated by the exible start and end times, the fact that infrastructure can already be reserved for certain time intervals for (for example) through-trains, the splitting and recombining of train units, and a different planning period (typically 24 hours instead of 1 hour). 15.3. SOLUTION APPROACH For practical instances, the TUSP becomes far too large to be solved as one integrated optimization problem. Therefore, the problem is decomposed in four parts, and we developed a four-step algorithmic solution approach that assists planners in creating parts of the shunt plan. The decomposed approach enables planners to view and possibly modify partial solutions between the steps. The four steps are: Step Step Step Step 1. 2. 3. 4. Matching arriving to departing train units Estimating routing costs of train units Parking of train units on shunt tracks Routing of train units

of feedback are applied without any ltering in the external feedback path; Figure 9.15a shows the multimode of the freely running laser; Figure 9.15b shows the single-mode operation of the laser when feedback is applied; Figures 9.15c g reveal the deterioration of the spatial pro le, the spectral broadening, and the mode hopping of the laser output as the amount of external feedback is increased. The spatial pro le is changed from an almost diffraction-limited spot in Fig. 9.15a to a radiation pattern in Fig. 9.15g that is far from the diffraction limit, which corresponds to several spatial modes emitted from the laser diode array. The increase of the external feedback also leads to slow temporal alternations (on the order of minutes) of the output. At a given level of external feedback the laser diode array is forced out of single-mode operation. This occurs slowly over 10 15 minutes or immediately after the external feedback is applied, depending on the intensity and the feedback angle. In all the experiments the feedback has been optimized by adjusting the external mirror (M2). However, due to diffraction loss, and so on, it is dif cult to determine the absolute amount of re ected light that enters the laser diode array. The response to a certain amount of external feedback radiation is seen to vary from measurement to measurement. We believe that this is due to the fact that the feedback is coupled into different array modes. It is possible to alter the spatial

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//.. Other Imports //JPA Imports ... import javax.persistence.Entity; @Entity @Inheritance(strategy=InheritanceType.JOINED) public class PixUser { @Id private String userName; private String firstName; private String lastName; private String email; private String password; //... remaining fields

Quickkey is an expanded replacement for acad.pgp that supports commands with their options, such as ZOOM Previous. Look in \Software\Chap29\Quickkey.

Figure 9-11: Using the CHANGE command on one line. If you select more than one line, CHANGE works differently: it moves the nearest endpoints of all of the lines to the change point so that all of the lines meet at one point, as shown in Figure 9-12. Figure 9-12: Using the CHANGE command on several lines. The original lines are shown as continuous. The new lines, after using the CHANGE command, are dashed.

where Ig is the gate current, and K1 , K2 and K3 are functions of resistances and capacitances [87, 88]; their expressions are given in Appendix A.2. As in the previous case, not all equations have been considered: the Z11 parameter does not usually yield reliable results. Plotting the measured data versus frequency, a suitable frequency range is identi ed for the extraction of the parameter; for example, the real part of the Z12 parameter is better evaluated at relatively high frequency (Figure 3.49). The extracted value depends on the value of the gate current Ig : the corresponding term can be eliminated by repeating the measurement for several current values and extrapolating to Ig 0 (Figure 3.50). From this bias condition, the source and drain inductances are found, and two equations in the three unknown resistances Rs , Rd and Rchannel are found. The third cold bias condition is somehow in between the other two: the channel is open, and controlled by the gate source voltage. The equations relative to the impedance Z-parameters are

Figure 3.27 Color Doppler ultrasound of blood ow showing convergent pulmonary vein in ow. (Courtesy of Siemens Medical Imaging Systems) http://www.siemensmedical.com/webapp/wcs/stores/servlet/PSProductImageDisplay productId=17966&storeId=10001&langId=-1&catalogId=-1&catTree=100001,12805,12761*559299136.

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