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Even so, the price of coal also increased sharply and rapidly in 2008 The CIF price of steam coal reached around 300 US $/toe in July, falling back to around 200 US $/toe in September 2008 (compared with 600 US $/toe for natural gas and 700 US $/toe for oil at the same time) In China, the rapid increase in demand has led to a very ambitious planning of renewal and growth of the power generation capacity in the years to come China plans around 1 GW of additional capacity each week over 20 years The additional capacity in China amounted to 50 GW in 2004, 70 GW in 2005 and 102 GW in 2006 China aims to install an overall capacity of power generation between 1200 GW and 1300 GW by 2030 [87].

How can you make sure that the string only matches if the digits and colon are at the start The answer is that you can use an anchor (also known as an assertion), as follows:

Figure 24-17: These solids are the basis for the model. 5. To create the central tube, choose Subtract from the Solids Editing toolbar. Follow the prompts:

v.,/V ,,,,.

Finally, the directory handle is closed:

As mentioned in the XML Schema-based support section earlier in the chapter, advice parameters can be matched by name as well as by type. With the @AspectJ support, this same solution of parameter name and type matching still applies. However, with @AspectJ support there is more available.

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the necessity to have long coherence length of the self-intersecting wave for the dynamic gratings completing the cavity to be effectively induced. Note that the single longitudinal mode operation of the scheme does not contradict the frequency shift of the interacting waves necessary for the self-starting oscillations. Indeed, the required frequency shift can be about t21 * 4 kHz, which is R much less than the estimated frequency bandwidth of the generated mode ( *MHz). In turn, the frequency shift of about 4 kHz is easily achieved by noised vibrations of the mirror mounting. 10.3.3.2 Experiments with thermal dynamic gratings in the NLC cell In the second series of our experiments, NLC cells with the homeotropic orientation were used. This orientation of the NLC layer permits propagation of ordinary optical waves. The self-starting generation was observed when ampli cation exceeded some threshold level (Fig. 10.23). Threshold gains of the nonlinear generation were considerably lower than those of the generation without NLC or due to diffuse scattering without a second pass through the NLC layer. The generation pulse energy did not depend on the repetition rate, so the relaxation time of the thermal grating was much less than 30 ms. Such temporal behavior corresponds to thermal nonlinearity of the NLC. The threshold of the self-starting generation decreased and the energy increased when the NLC was changed from 5CB with the nematic isotropic transition temperature of about 368C to a mixture of cyanobiphenyls with the nematic isotropic transition temperature of about 598C (Fig. 10.23). This fact

The world consumption of steam coal for power generation might therefore increase from 1500 Mtoe in 2000 to 2500 Mtoe in 2030 Coal ensures around 40 % of power generation, which amounts to around twothirds of the worldwide coal consumption Furthermore, if, in the future, it becomes dif cult to satisfy the demand for engine fuels by deriving them only from oil supplies, the production of synthetic liquid fuels from coal will increase rapidly The yield of such a transformation is unfortunately comparatively low: an amount of 25 toe of coal is needed to replace 1 toe of oil Large emissions of CO2 therefore result from such a transformation Synthetic fuels can also be produced from natural gas or biomass and the future outlook for these synthetic fuels is discussed in the next section.

As shown in Figure 7.9 a., the feedback signal 1. arriving at time o s g t ny1 , t n x indicates that x kq1 s y . s Bkq1 . The data to be received at node k q 1 from s y to t n , whose number is denoted by A kq1 s y , t n . wsee 7.2.x, were previously sent by node k in s y 2 , t n y x, denoted by D k s y 2 , t n y . wsee 7.1.x. The data dispatched by the model queue according to 7.16. is R t n y s q . during s y , t n x. Thus from the queue evolution equation 7.6.,

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