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Deck-Locking System The deck-locking system enables a helicopter to land on, and remain secured to, the desk of a heaving ship in gale force winds up to 50 knots. The principle has been in use since the early 1960s when a rudimentary system was tested by the Royal Aircraft Establishment (now the Defence Research Agency), using a Dragon y helicopter. The system allows the pilot to capture the deck, either for a nal recovery landing or to re-arm or refuel prior to an additional sortie. The deck lock system is developed and produced by Claverham now Hamilton Sundstrand and is in use for the recovery of helicopters up to 20 000 lb. Later systems under development for use with the EH 101 will enable operation with helicopters up to 30 000 lb. The ship deck has a grid into which a helicopter mounted harpoon arrangement may engage. The helicopter hovers above the deck as the pilot arms the system. This causes the decklock to be lowered from the stowage bay into an extended position. By judging the movement of the ship, the pilot elects to touchdown and activates the system by pressing a switch located on his collective lever. This enables the engagement beak and jaws to engage the deck grid and secure the helicopter to the deck. If for any reason the beak misses the grid, or encounters solid deck, the system automatically recycles and the pilot may re-attempt engagement. The engagement sequence is complete with 1.5 seconds. The deck lock system for the EH 101 is shown in Figure 9.20.



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(Fig. 2.8). Side-chain polymers are more typical, and commercially available polymer PAZO (Aldrich) was already used for LbL assembly in 1997 (Lvov et al., 1997). Both PAZO and PS-119 (Fig. 2.8) could be considered as strong polyelectrolytes being in salt form. It is important that charged group be connected to azobenzene moiety, and therefore one can expect the ionic interactions responsible for the formation of LbL structure to restrict azobenzene motion. Birefringence value of 0.09 for the 200-nm lm (dos Santos et al., 2006) was achieved for structures of PS-119 with cationic dendrimers. Interestingly, for higher dendrimer generation (with higher charge density) stronger absorption of PS-119 has been observed. That fact led to the lower values of birefringence, which is related to restriction of chromophore molecular motion. For PS-119/PAH architecture





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Our discussion up to this point has been focused on the nodal delay, ie, the delay at a single router Let us conclude our discussion by briefly considering the delay from source to destination To get a handle on this concept, suppose there are Q-1 routers between the source host and the destination host Let us also suppose that the network is uncongested (so that queuing delays are negligible), the processing delay at each router and at the source host is dproc, the transmission rate out of each router and out of the source host is R bits/sec, and the propagation delay between each pair or routers and between the source host and the first router is dprop The nodal delays accumulate and give an end-to-end delay, dendend = Q (dproc + dtrans + dprop) , where once again dtrans = L/R, where L is the packet size We leave it to the reader to generalize this formula to the case of heterogeneous delays at the nodes and to the presence of an average queuing delay at each node

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[Bertsekas 1992] D Bertsekas and R Gallager, Data Networks, 2nd Edition, Prentice Hall, Englewood Cliffs, NJ, 1992 [Daigle 1991] JN Daigle, Queuing Theory for Telecommunications, Addision-Wesley, Reading Massachusetts, 1991 [Kleinrock 1975] L Kleinrock, Queuing Systems, Volume 1, John Wiley, New York, 1975 [Kleinrock 1976] L Kleinrock, Queuing Systems, Volume 2, John Wiley, New York, 1976

Figure 2.8. Chemical formula of azobenzene-containing polyelectrolytes used for the preparation of LbL multilayers and supramolecular complexes.

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(Zucolotto et al., 2004b), the structure and charge density of cationic polyelectrolyte PAH can be governed by pH during LbL deposition, and it changes the LbL lms properties. By increasing the pH from acidic to basic, it was possible to increase the bilayer thickness by the factor of 2.4 because of the loose conformation of PAH in the LbL structure. The authors compared the lms with similar amount of azobenzene (the same optical absorption) prepared at different pH and came to the conclusion that an increase in the pH led to a slowing of kinetics of the induction of photoorientation by the factor of 4. For another similar polyelectrolyte PAZO (Fig. 2.8), the data on photoinduced orientation in LbL structures are not available. In contrast to LbL structures, the results on ionic complex of PAZO with PEI (Stumpe et al., 2006a) showed that dichroism was lower in this case compared with the neat PAZO lms (Stumpe et al., 2006b; Goldenberg et al., 2005), approximately proportional to a decrease in azobenzene loading. It seems that there is no restriction of azobenzene motion by ionic interactions with oppositely charged polyelectrolyte in this complex. This demonstrates that the layered structure of the LbL lms should be responsible for this restriction. Two other azobenzene-containing polyelectrolytes (Fig. 2.8) are copolymers. The important difference is that ionizable group (COOH) is attached not to the azobenzene but to another unit on the polymer chain. Therefore, one could expect

The means by which the FCS provides auto-stabilisation and autopilot control has already been described earlier in the chapter. Handling a large helicopter such as the EH 101 requires a great deal of effort and concentration by pilots who have other considerable demands placed upon them, for instance by Air Traf c Control or mission requirements. The need for an advanced AFCS providing a wide range of autopilot modes is paramount

[Ross 1995] KW Ross, Multiservice Loss Models for Broadband Telecommunication Networks, Springer, Berlin, 1995

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