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81 present in a given volume at a site of lower concentration have a lower probability to come to the same volume at a site of higher concentration than in the opposite case, where the particles at a site of higher concentration come to the site of lower concentration. 2. Heat conduction the transport of energy resulting from temperature gradients in the system or difference in temperature, between the system and its surroundings. Heat conduction arises from the fact that, while the number of particles per volume unit is identical at various sites in the system, they have different impulses. 3. Convection the transport of mass or energy as a result of streaming in the system produced by the action of external forces. These include mechanical forces {forced convection) or gravitation, if there are density gradients in the system {natural or free convection). 4. Conduction of electric current transport of charge and mass as the result of the motion of elecrically charged particles in an electric field. Chemical reactions in the system are irreversible processes, affecting transport processes, as they result in the formation and disappearance of components of the system and in the release or consumption of thermal energy. The rate of a chemical reaction (the 'chemical flux'), / ch , in contrast to the above processes, is a scalar quantity and, according to the Curie principle, cannot be coupled with vector fluxes corresponding to transport phenomena, provided that the chemical reaction occurs in an isotropic medium. Otherwise (see 6, page 450), chemical flux can be treated in the same way as the other fluxes.



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Dest. Prefix 10.10.2.0/30 10.10.3.0/30 192.168.10.20/32 192.168.20.30/32 172.16.2.0/24 Next-hop Local Local 10.10.2.1 10.10.3.1 Local Metric 0 0 2 2 0

References De Groot, S. R., and P. Mazur, Non-equilibrium Thermodynamics, Interscience, New York, 1962. Denbigh, K. G., Thermodynamics of the Steady State, Methuen, London, 1951. Glansdorff, P., and I. Prigogine, Structure, Stability and Fluctuations, John Wiley & Sons, New York, 1971. Onsager, L., Phys. Rev., 31, 405, 2265 (1931). Prigogine, I., Introduction to Thermodynamics of Irreversible Processes, John Wiley & Sons, New York, 1967. Yao, Y. L., Irreversible Thermodynamics, Science Press, Beijing and Van NostrandReinhold, New York, 1981. 2.2 Common Properties of the Fluxes of Thermodynamic Quantities





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6.19 While hiking in the Grand Canyon, I came upon this lizard that was darting in You don t need any other special and out of the shade of trees. With a little equipment to take stunning macro patience and making slow, stalking shots with your PowerShot G11 like movements to get into position and ll the frame, I was able to make this detailed you do with larger dSLRs it comes portrait. Taken in Macro mode at ISO 400, ready to go, right out of the box. f/3.5, 1/100 second with a 13mm lens DSLRs require extension tubes or setting. close-up lters to get you into the close-up range that the G11 handles with ease. Macro photography can be a great avenue for learning about light and the world around you, but be warned it can be very habit forming. The more you do it, the more you begin to see macro possibilities everywhere.

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3. The longest entry matching the destination is found, and the next-hop IP address is examined. The local interface corresponding to the next-hop IP address is then determined by re-examining the R1 forwarding table. 4. The IP packet is then forwarded to the corresponding local interface and out of Router R1 to its next-hop R3. 5. The IP packet enters Router R3. 6. R3 examines its routing table to find a matching destination for the IP address. It determines that the network is local and that it does not need to forward the packet to any other routers. 7. R3 puts the correct L2 header on the IP packet and forwards it to the destination device. These procedures are actually the result of two separate functions that routers perform. One function of routers is simply to forward packets as we have described. The other function is to use routing protocols to build routing tables so that the forwarding process has the information it needs to operate correctly. The terms control plane and data plane are often used when referring to these routing update and packet forwarding processes.

Consider a linear tube with cross-section A and length /, filled with a material, and assume that changes in the considered thermodynamic quantity can occur only along the length of the tube (i.e. the 'mantle' of the tube is insulated, the ends being permeable for the thermodynamic quantities). Flux / is a function of coordinate x (see Fig. 2.1).

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