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9 Jan 2017 ... We got a question, and said yes. If we can do that? Yes, we can! When you get back at the office you get a cold shiver along your spine when ...

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Such materials are free from polymer chains and any restricting entanglement of the backbone The results indicate that the existence of a polymer chain is not a necessary condition for induction of anisotropy and SRG formation The bulky structure of the molecules is a necessary condition to prevent the crystallization and ensure lm-forming properties Moreover, the glass transition of the materials is rather low, leading to low stability of the photoinduced structures As in the case of polymers, the alternative use of lowmolecular-weight glasses is also restricted by their speci c design and complicated synthesis The bulky structure restricts the inducible anisotropy In addition to amorphous glasses, there is one example for low-molecular-weight liquid crystalline glass-forming material (Stracke et al, 2000) Interestingly, that anisotropy and SRG, photoinduced in the glassy state of spin-coated lms at room temperature, were ampli ed by annealing in the mesophase.



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20 Jan 2012 ... GhostScript . NET integration component - 11.7 KB · PDF conversion component - 5.4 KB. Introduction. An application I was recently working on ...

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These control laws are complex and detailed description is outside the scope of this book. Saunders (1983) gives a fuller description of these control laws and their implementation [6]. A system comprising more than one engine/FADEC may also incorporate features whereby one will be accelerated to maximum power if one of the other engines fails or the thrust drops below a predetermined level. Such a system is likely to apply power more quickly than the pilot when operating in a critical ight mode such as the hover.





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Industrial application of photoinduced anisotropy or light-induced SRG formation requires ful lling of a number of additional parameters At rst the photochromic material has to be transferred in lms of good optical quality This can be achieved using different materials as discussed above and by different methods of lm preparations, such as spin coating, doctor blading, Langmuir Blodgett, or layer-by-layer (LbL) techniques In addition to the basic effects, a number of further requirements become important, such as the easy processing and handling of the lms Especially lm-forming properties, use of good and environmental solvents, restriction of crystallization and aggregation, good optical quality of the lms before and after induction, stability of the photoinduced effects, and, of course, the price of the materials are very important requirements for any application Moreover, the matrix can introduce speci c properties such as liquid crystallinity or further functionalization.

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The Internet's network layer protocol, IP, provides a best-effort service That is to say that the Internet makes its best effort to move each datagram from source to destination as quickly as possible However, the best-effort service does not make any promises whatsoever on the extent of the endto-end delay for an individual packet, or on the extent of packet jitter and packet loss within the packet stream Real-time interactive multimedia applications, such as Internet phone and real-time video conferencing, are acutely senstive to packet delay, jitter and loss Fortunately, designers of these applications can introduce several useful mechanisms that can preserve good audio and video quality as long as delay, jitter and loss are not excessive In this section we examine some of these mechanisms To keep the discussion concrete, we discuss these mechanisms in the context of an Internet phone application, described in the paragraph below The situation is similar for real-time video conferencing applications [Bolot 1994] The speaker in our Internet phone application generates an audio signal consisting of alternating talk spurts and silent periods In order to conserve bandwidth, our Internet phone application only generates packets during talk spurts During a talk spurt the sender generates bytes at a rate of 8 Kbytes per second, and every 20 milliseconds the sender gathers bytes into chunks Thus the number of bytes in a chunk is (20 msecs)*(8 Kbytes/ sec) = 160 bytes A special header is attached to each chunk, the contents of which is discussed below The chunk along with its header are encapsulated in a UDP segment, and then the UDP datagram is sent into the socket interface Thus, during a talk spurt a UDP segment is sent every 20 msec If each packet makes it to the receiver (ie, no loss) and has a small constant end-to-end delay, then packets arrive at the receiver periodically every 20 msec during a talk spurt In these ideal conditions, the receiver can simply play back each chunk as soon as it arrives But, unfortunately, some packets can be lost and most packets will not have a fixed end-to-end delay, in even a lightly congested Internet For this reason, the receiver must take more care in (i) determining when to play back a chunk, and (ii) determining what to do with a missing chunk.

Therefore, there is still a challenge to nd low cost systems capable of effective light-induced orientation and SRG formation The supramolecular chemistry with its variety of intermolecular interactions can be seen as exactly right strategy in design of functional materials According to the broad de nition by Lehn (1995), supramolecular chemistry is chemistry beyond the molecule It is the chemistry of intermolecular bonds forming supramolecular complexes or phases It may be divided into broad, partially.

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