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19 Oct 2013: 20. Eliminate U2:. 12g(h21 h. 22) = h2. V (h2 h1).

19 Oct 2013: Then. 20. p(a+, t) = p(a, t) (bubble volume)γ (a3)γ a3γ, where γ is the ratio of specific heats.

19 Oct 2013: I don't think it needs to be 20 years and it doesn't need to be 20 years for every country on this planet.

19 Oct 2013: Transcript of British Broadcasting Corporation's "Analysis" programme of 4 November 1999: ANALYSIS ROUGH COUNTING PRESENTER: ANDREW DILNOT PRODUCER: INGRID HASSLER EDITOR: MICHAEL BLASTLAND TRANSMISSION: 4 November '99 20.30 and

5 Jun 2013: 15] [16] [17] File: PV_phillips_2.eps Graphic file (type eps) PV_phillips_2.eps [18] [19] [20] [21] [22] [23] [24] [25] [26] [27] [28] File: staircase-jets.eps

4 Nov 2013: The flow enters a new regime in which thebending stresses in (1) can be neglected almost every-where, resulting in a standard viscous gravity-currentbalance [7,20]. ... 19] L. Hocking, Q. J. Mech. Appl. Math. 36, 55 (1983).[20] H.

26 Jul 2013: FIG. 7. Energy repartition of a cy-clonic unstable normal mode obtaineby the matrix eigenvalue method fok5 20 andk5 30. ... for k5 10 andk5 20 columns 2 and 3! Anextrapolated values 0 for k5 has been calculatedcolumn4!

4 Nov 2013: The measurements of k can be fitted by an ap-proximate scaling k Ra0:4, though the data also hint at apossible decrease in the exponent for Ra > 20 000 ... 20] Counts from a plume-tracking algorithm suggest a scalingexponent of 0:96 0:05 for the rib

26 Jul 2013: sin2( φ2 )(h sinh h). h sinh h. ], (3.20). 〈ψ2〉x.

26 Jul 2013: dropping by about three orders of magnitudeto a value of approximately 20 times that of water. ... g1 =5. 144. 1. h ̄̄ ̄̄. 20. Finally, we find the first-order correction to the mechanicalenergy.