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using our numerical value for D. The ratio of D to the equilibration timescale (3.71) is D / E = 18.7R( m)2 /[Rp (1 + 6.23R( m))] (3.74) Values for this ratio covering the likely range of atmospheric aerosols with R = 1 nm 10 m and N = 102 cm 3 106 cm 3 are shown in Table 3.3 taken from Clement [5]. In the continuum limit for large R, the ratio given in (3.74) is independent of the diffusivity, D, since both timescales are then proportional to 1/D. Except for dense aerosols of very large size, the ratio is very much smaller than 1, showing that vapour diffusion in the interstitial gas between particles is much faster than condensation on the particles. This means that the vapour concentration will be kept uniform throughout the aerosol by diffusion. This result extends to the case when vapour production, P , occurs. The solution (3.69), which depends on radiusR, is invalid, and the steady-state vapour concentration is determined by the balance between the production rate and the average removal rate onto the aerosol (see Section 3.3.4 below). The same result applies to the temperature of the vapour gas mixture between particles in the aerosol. This is determined by the average heat transfer to or from the aerosol associated, respectively, with evaporation or condensation and the latent heat absorbed or released, respectively. The rates of heat transfer by conduction or from molecules at liquid surfaces are similar to those for mass transfer (see, e.g., Clement [24] and Barrett and Clement [14]). Thus there is no need to repeat the above argument with the vapour diffusivity replaced by the thermometric conductivity of the mixture. The ratio of the latter to the diffusivity is the dimensionless Lewis

, Bickman, 1987; Chen, 1990) The idea is to construct, based on local program ideas, general social science theory, or both, a kind of theoretical model of program activities, processes, and outcomes This program theory would then be used to help guide the evaluation, such as in the choice of outcome measures (eg, Bickman, 1987; Chen, 1990) Despite the potential usefulness of program theory, theory can also have some undesirable consequences (eg, Greenwald, Pratkanis, Leippe, & Baumgardner, 1986) Using theory to guide evaluation design is unlikely to be harmful if one s theory is fully correct But theories are usually only partially correct at best, and the theory-driven evaluation may exclude important outcome measures that the (imperfect) theory did not specify, ignore possible mediators other than those speci ed in the theory, and fail to search for important moderators of the program s success.

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Strong adherence to a program theory can even lead one to misinterpret results or overgeneralize conclusions (Greenwald et al, 1986) In addition, just as formal goals may sometimes be set for public.

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report that women with complete SCI experience orgasm in response to genital and nongenital stimulation Changes in heart rate, blood pressure, and arousal were monitored in 16 women with complete SCI and 5 able-bodied women Despite having complete SCIs, the women retained the ability to achieve orgasm and registered physiologic and subjective changes similar to those of the able-bodied women Post-SCI amenorrhea is a common occurrence (Charlifue et al, 1992, Comarr, 1966) and can last an average of ve months With the resumption of the ovulatory menstrual cycle, a woman s ability to conceive also returns However, Charlifue et al found that the greater the level of impairment, the likelihood of having children decreased This nding may possibly be due to women s recognition of the dif culty associated with caring for a child.

4 B Otis and J Rabaey A 300 mW 19 GHz oscillator utilizing micro-machined resonators In IEEE Proceedings of the 28th European Solid State Circuits Conference, vol 28, September 2002 5 See at http://wwwdust-inccom, 2004 6 See at http://wwwxbowcom, 2004 7 See at http://wwwxsilogycom, 2004 8 See at http://wwwembercom, 2004 9 See at http://wwwmillenialnet, 2004 10 See at http://wwwpaperpowercom, 2004 11 See at http://cymbetcom, 2004 12 J Bates, N Dudney, B Neudecker, A Ueda, and C D Evans Thin- lm lithium and lithium-ion batteries Solid State Ionics, 135:33 45, 2000 13 J N Harb, R M LaFollete, R H Selfridge, and L L Howell Mircobatteries for self-sustained hybrid micropower supplies Journal of Power Sources, 104:46 51, 2002 14 R W Hart, H S White, B Dunn, and D R Rolison 3-D microbatteries.

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