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31 Dec 2018: Unfortunately, the integrals (3.20) and (3.21) look pretty fierce. Shortly, we will start. ... this section if you’re impatient). Let’s look at the particle density (3.20),.

31 Dec 2018: G = F pV = E pV TS (4.20). This is a Legendre transform of F , this time swapping volume for pressure: G = G(T, p). ... already seen in Section 1.4.1. From its definition (4.20), we see that the Gibbs free. –

31 Dec 2018: Zvib =1. 2. Zddpe. Hvib =kBT! (2.20). The average vibrational energy of each molecule is now.

28 Dec 2018: The value of β was taken from Kang et al. [20], andthe evaporation speed was measured experimentally. ... σ. 2. (b) (c). 0. 1. 2. 3x104(a). 0 10 20 30k.

13 Dec 2018: For example, without further approximation,evaluation for a scatterer of around 220 by 20 wavelengthscan be carried out in around 100 minutes using 32processors on the SunFire machine. ... 0.05 0.05 0.2 0.6 1.0 1.4 1.8. Fig. 1 Surface current amplitudes

13 Dec 2018: 1997 Acoustical Society of America.@S0001-496697!03703-X#. PACS numbers: 43.20.Fn, 43.20.Mv, 43.30.Hw@ANN#. nsemismiceThthaceinionti-. ... An5an ,bn!, Cn5cn ,dn!, 20! wherean , bn , cn , dn are given by11!

13 Dec 2018: heightλ/20. most surface geometries, and can easily be reduced further with higher order. ... 20. 1 Introduction. 2 Formulation of equations. 2.1 Formal solution and splitting series.

13 Dec 2018: 3. The query condition is set as querying“Peak wave number” with the condition “< 20.0” througha Web form shown in Fig.

13 Dec 2018: Retaining just the first term in the iterative series (11),. ψ = L1ψinc, (20). ... height λ/20. Figure 7: Real part of surface field on waveguide at two frequencies.

13 Dec 2018: ψ̃ = (C′0 C′1)(C0 C1)1ψinc, (20). and then solving as before and comparing terms with (19).