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The above rule indicates that when u s dominating (absorbant) neighbor set (excluding v and w) is covered by the union of dominating (absorbant) sets of v and w, vertex u can be removed from D if the ID of u is smaller than those of v and w. Again, u and v(w) may or may not be connected. Figure 20.9 shows an example of using the extended marking process and its extensions (two rules) to identify a set of connected dominating and absorbant nodes. Figure 20.9 (a) shows the gateway nodes (nodes with double cycles) derived by the extended marking process without applying two rules. Figure 20.9 (b) shows the remaining gateway nodes after applying two rules. Assume that V * is the resultant dominating and absorbant set when Rule 1a and Rule 2a are simultaneously applied to all vertices in V . The following result shows that V * (its induced graph is D*) is still a connected dominating and absorbant set of V. The shortest path property of Proposition 3 still holds in D * for Rule 1a, but not for Rule 2a. Proposition 4: If V is a strongly connected dominating and absorbant set of D derived by using the extended marking process, then V * derived by using Rule 1a and Rule 2a on all vertices in V is still a strongly connected dominating and absorbant set of V. In addition, if V * is derived by applying Rule 1 alone, then V * still includes all intermediate vertices of at least one shortest path for any pair of vertices in V.

The ratio of distance from feed to load to dipole half-length is . All data presented here were obtained by using N = 12, which allowed loading points of 1/6, 1/3, 1/2, 2/3, and 5/6 to be considered. Results were spot checked with N = 6 and 48 to validate the runs. In principle the loading inductor functions by keeping the current distribution nearly constant from the feed to the load point, thereby increasing the current moment. Because the radiation resistance varies as current moment squared and the effective length varies with current moment, it is clear that inductive loading will improve short monopole performance (Fournier and Pomerleau, 1978). There is a value of loading reactance that allows the current to approximate a constant value out to h with a linear dropoff beyond. This value of inductance is, however, insuf cient to produce input impedance resonance. The resonant value of load produces a modest current peak just beyond h so that the current moment is increased by an additional amount over that expected from the constant current model. Figure 1.16

280 14

API (Report No CP015-97-1b), Washington, DC: 1997 37 Johnson, D, Utembe, SR, Jenkin, ME, Derwent, RG, Hayman, GD, Alfarra, MR, Coe, H and McFiggans, G Simulating regional scale secondary organic aerosol formation during the TORCH 2003 campaign in the southern UK Atmospheric Chemistry and Physics 2006; 6: 403 418 38 Pun, BK, Seigneur, C, Vijayaraghavan, K, Wu, SY, Chen, SY, Knipping, EM and Kumar, N Modeling regional haze in the BRAVO study using CMAQ-MADRID: 1 Model evaluation Journal of Geophysical Research Atmospheres 2006; 111(D6): D06302 39 O Neill, SM, Lamb, BK, Chen, J, Claiborn, C, Finn, D, Otterson, S, Figueroa, C, Bowman, C, Boyer, M, Wilson, R, Arnold, J, Aalbers, S, Stocum, J.

Public Function PPF HullWhiteLatticePrice(

You can use the do..while statement to create the same kind of loop as a while loop. In a do..while loop, the expression is evaluated at the bottom of the code block so the loop always runs at least once, as in the following:

, Swab, C, Stoll, M, Dubois, M and Anderson, M Modeling ozone and aerosol formation and transport in the paci c north-west with the community multi-scale air quality (CMAQ) modeling system Environmental Science and Technology 2006; 40(4): 1286 1299 40 Matthias-Maser, S and Jaenicke, R The size distribution of primary biological aerosol particles with radii >02 mu m in an urban rural in uenced region Atmospheric Research 1995: 39: 279 286 41 Matthias-Maser, S Primary biological aerosol particles: their signi cance, sources, sampling methods and size distribution in the atmosphere In: RM Harrison and RE van Grieken, eds Atmospheric Particles John Wiley, Chichester: 1998; pp 349 368..

The real distance is given by r and corresponds to the distance considered from the transmission time to the receiving time. Note that the transmission time should be the one at the sending time of the signal received by the receiver at the receiving time, and not the one sent at the time of reception, of course. DPropag includes all the propagation errors. Considering Equations 1 and 2, one obtains and tr trr dtr

Figure 6.19 Scheduling principle with input parameters and in uences on the overall chosen scheduling strategy.