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Note The relationship between the move grip tool and the UCS icon is significant. In any 3D visual style, the X axis of the UCS icon is red, the Y axis is green, and the Z axis is blue. The rotate grip tool uses the same colors to indicate the same directions.

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Compared to a value of unity for CO2 , the global warming potential (over a period of 100 years), GWP, of CH4 = 23 and that of N2 O = 296 The comparable GWP value for CFC-11 and CFC-12 would be 4000 and 8500! The Table A1 below shows data on the global warming potential of common greenhouse gases and chloro uorocarbons relative to that of carbon.

Figure 7-4

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2 The magnitude of interaction, heL e hAB a eLUMO eHOMO , depends inversely on the orbital energy di erences and directly on the square of the intrinsic interaction matrix element, which in turn is approximately proportional to the overlap of the two orbitals. The LUMO energies of methyl and allyl are the same. The di erence in reactivity, as measured by heL does not arise from the orbital energy di erences, but rather from the magnitude of hAB e kSAB . Since the nucleophile's HOMO can only overlap with one p orbital of the LUMO in each case, the overlap with the allyl LUMO will be smaller because the magnitude of the coe cient (0.707) is smaller (it is 1.0 in the case of methyl).

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Connelly, P.R. (1994) Acquisition and use of calorimetric data for prediction of the thermodynamics of ligand-binding and folding reactions of proteins. Current Opinion in Biotechnology, 5, 381 8. Review of use of calorimetric measurements in study of processes such as protein folding and ligand binding. Janin, J. (1997) Angstroms and calories. Structure, 5, 473 9. A thought-provoking exploration of the relationship between calorimetric measurements and structure in biomacromolecules. Jelesarov, I. and Bosshard, H.R. (1999) Isothermal titration

contaminant proteins (e.g. large differences in Mr or hydrophobicity).

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Results for a reference antenna ( o = i = 0) are shown for comparison. Note that the embedded slots in the ground plane have very small effects on the feed position dp for achieving good impedance matching of the prototypes; dp was chosen to be 5 mm. For the reference antenna, the fundamental resonant mode is excited at 2387 MHz with a 10-dB return-loss bandwidth of 2.0%. For increasing slot length i , it is seen that the fundamental resonant frequency is quickly lowered. For antenna 4 ( i = 14 mm), the resonant frequency f r is 1587 MHz, which is about 0.66 times that of the reference antenna. This suggests that an antenna size reduction as large as about 56% can be achieved for the proposed antenna operated at a xed frequency. Moreover, it is clearly seen that the impedance bandwidths of the prototypes (antennas 1 4) are all greater than that of the reference antenna. This behavior is largely owing to the meandering slots embedded in the antenna s ground plane, which effectively lower the quality factor of the proposed antenna.

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In his view, planning is performed by recursively decomposing goals into subgoals, until a subgoal can be reached by elementary actions As was explained in s 3 and 4, this paradigm is contradicted by Hayes-Roth and Hayes-Roth (1979) In their line of reasoning, they say that planning processes operate in a two-dimensional planning space de ned on time and abstraction (op cit, p 312) In these terms, successive re nement would always work top-down from high to low abstraction and forward in the timeframe of the plan Thinking aloud protocols from different subjects that perform planning tasks show that this is not always the case Hayes-Roth and Hayes-Roth found planning actions that they call opportunistic planning The subjects do not work solely linear but appear to switch in levels of abstraction and move both forward and backward in time in successive reasoning steps.

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