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Giulio Del Zanna - Publications
www.damtp.cam.ac.uk/user/astro/gd232/publications.html21 Apr 2004: 5th SOHO workshop Oslo, 17-20 June 1997. Bromage, B.J.I., G. Del Zanna, C. ... Pike, 1997: GIS calibration study with a plasma diagnostic method 5th SOHO workshop Oslo, 17-20 June 1997. -
Selected and Recent Publications
www.damtp.cam.ac.uk/user/bioguest/selected_pubs.html21 Apr 2004: Respir. Physiol. 15: 1-38, 1972. 20. -
Worked ExampleElectrostatics: Using the Integral Solution of…
www.damtp.cam.ac.uk/user/reh10/lectures/nst-mmii-handout9.pdf2 Mar 2004: 4π0. LL. dzx20 y. 20 (z z0)2. =µ. 4π0. [sinh1. z z0x20 y. ... 20. }. This is true for arbitrary locations x0, so replacing x0 by x we obtain. -
F21 MATHEMATICAL TRIPOS PART IIB Prof E.J. Hinch‘Waves in ...
www.damtp.cam.ac.uk/user/hinch/teaching/B21d.pdf27 Apr 2004: c20. (. ρ3/20. ρ̃)). = 0 ,. where ρ̃(x, t) is the density perturbation, ρ0(z) is the unperturbed density, and c0(z) isthe local speed of sound. ... γ. (. 1. k. 1. (k2 20)1/2. ). ,. and. (b) y =N. -
Geophysical and Environmental Fluid Dynamics:Some useful numbers…
www.damtp.cam.ac.uk/user/mem/GEFD-SUMMER-numbers.pdf1 Oct 2004: g = (9.78032 0.005172 sin2 ϕ 0.00006 sin2 2ϕ)(1 z/a)2. Mean surface value, ḡ = π/20. ... 25 298 ” 3.820 293 ” 4.20 273 ” 5.2. -30 243 ” 8.4. -
Evolution of vortex rings after the collapse of ultrasound ...
www.damtp.cam.ac.uk/user/ngb23/publications/bubbleQFS.pdf20 Jul 2004: For a > 20 the energy depends on theradius as E 1.65 a2.9. ... 10. 15. 20. a. -. -. -. --. 0.7 0.8 0.9 1 1.1b. -
CATAM Lecture NotesComplexity We often have a choice of ...
www.damtp.cam.ac.uk/user/reh10/lectures/complexity.pdf10 Mar 2004: Suppose that the former requires 12 n. 2 operations and the latter 10n; thenthe first algorithm is quicker for n < 20. -
F19 MATHEMATICAL TRIPOS PART IIB Prof. E.J. Hinch‘Waves in ...
www.damtp.cam.ac.uk/user/hinch/teaching/B21b.pdf27 Apr 2004: Typical values of E (in units of 1010 Nm2) and ν for materials at 20 are:E ν E ν. -
VOLUME 93, NUMBER 9 P H Y S I ...
www.damtp.cam.ac.uk/user/ngb23/publications/bubble.pdf17 Sep 2004: 0 20 40 60 80 1000. 1. 2. 3. 0 20 40 60 80 1002. ... 1.5. 1. 0.5. 0. 0.5. 1. 0 20 40 60 80 100. -
INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS A: MATHEMATICAL ...
www.damtp.cam.ac.uk/user/ngb23/publications/motionX2.pdf19 Nov 2004: We performed numerical integrations of (20) with the time derivative 2it restoredto the left-hand side. ... 20. )v0. 2[2H v0 u20v0 2U zu0] O( 4) = 0, (B.5). -
Interactions of vortices with rarefaction solitary waves in a ...
www.damtp.cam.ac.uk/user/ngb23/publications/interact2.pdf25 Jun 2004: p / 4) is shown in Fig. 3. Initially the center of the rarefactionpulse is 20[Fig. ... rarefactionpulses and the straight-line vortex att = 35 that are initially a dis-tance of 20 healing lengths apart. -
IserlesNorsett1.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2004_03.pdf26 Jan 2004: 0. 0.002. 0.004. 0.006. 0.008. 20 40 60 80 100. omega. ... omega. 2e–06. 3e–06. 4e–06. 5e–06. 20 40 60 80 100. omega. -
Capture of an impurity by a vortex line in ...
www.damtp.cam.ac.uk/user/ngb23/publications/capture.pdf25 Jun 2004: Gross, NuovoCimento 20, 454 1961! 4 C.A. Jones and P.H. Roberts, J. ... Acad. Sci., Ser. III 325, 195. 1997!20 W.H. Raymond and H.L. -
Evolution of rarefaction pulses into vortex rings Natalia G. ...
www.damtp.cam.ac.uk/user/ngb23/publications/evolution.pdf25 Jun 2004: is l 5 20. The solutions starting with the thirdpanel possess vorticity and evolve into equally spaced vortex rings. ... In these computationswe use e 5 0.3 and l 5 60,30,20,15. -
INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS A: MATHEMATICAL ...
www.damtp.cam.ac.uk/user/ngb23/publications/pair.pdf19 Jan 2004: 20 10 0 10 2020. 10. 0. 10. 20. 20 10 0 10 2020. ... 10. 20. 20. 010. 20. 10 20. 0. 0.25. 0.5. 0.75. -
INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS A: MATHEMATICAL ...
www.damtp.cam.ac.uk/user/ngb23/publications/motionIX.pdf8 Oct 2004: 20). Here γ 0.577216 is Euler’s constant. When we approximate (19) for kh 1, we obtain(18). ... Phys. A: Math. Gen. 4 55[19] Saffman P G 1992 Vortex Dynamics (Cambridge: Cambridge University Press)[20] Schwarz K W 1988 Phys. -
vtalk.dvi
www.damtp.cam.ac.uk/user/tong/talks/vsvs.pdf29 Nov 2004: The mass of the kink is given by. Mkink = r(χ+ χ) = r(mj mi) (20). ... The 4d theory contains dyons. The 2d theory also contains dyonic kink objects, asfirst noted 10 years ago by Abraham and Townsend [20]. -
Scenario of strongly nonequilibrated Bose-Einstein condensation…
www.damtp.cam.ac.uk/user/ngb23/publications/svist1.pdf25 Jun 2004: Gross,Nuovo Cimento 20, 454 1961!; L.P. Pitaevskii, Sov. Phys.JETP 13, 451 1961! ... 20# C.W. Gardiner et al., Phys. Rev. Lett. 81, 5266 1998!; M.J.Davis, C.W. -
EXPONENTIAL BROWNIAN MOTION AND DIVIDED DIFFERENCES B. J. C. ...
www.damtp.cam.ac.uk/user/na/NA_papers/NA2004_06.pdf14 Jul 2004: obtain. (4.20) r(z) = u[z0] u[z0,. , zn](z z0) (z zn).We obtain (4.17) by equating the coefficients of zn in (4.20) and the product of -
Reconstruction Algorithms for PositronEmission Tomography and Single…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2004_07.pdf11 Oct 2004: 20] B.F. Hutton, Cardiac Single–Photon Emission Tomography: Is Attenuation Correc-tion Enough? ... Prob. 20, 175 (2004). [31] T. Hebert, R. Leahy, M. Singh, Fast MLE for SPECT using an Intermediate PolarRepresentation and a Stopping Criterion, IEEE -
Paper1.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2004_04.pdf25 Mar 2004: . . . 0 0 0 20 0 2 00 2 0 02 0 0 0. -
Introduction E.J. Hinch D.A.M.T.P. Cambridge University Mobile…
www.damtp.cam.ac.uk/user/hinch/teaching/mobile.pdf23 Apr 2004: In long drums (some of the model experimentshave been with very short drums which permit just a monolayer of particles), Fauvredescribes in chapter 20 an axial instability which leads to a ... For thin layers of grains,Fauvre shows in chapter 20 that air -
NA2004_08.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2004_08.pdf14 Nov 2004: . . . . (4.20). The technique of the previous paragraph is employed only if at least one ofthe signs sk, k = 1, 2,. , ... We. 20. write t instead of MOVE, in order to retain the notation of Section 4. -
report.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2004_01.pdf7 Jan 2004: 2eTt H et = 1 αβ τ2. Hence, by. taking determinants of the matrix equation (2.20), we obtain the condition. ... 20. defined by formula (2.12), where α = eTt Het and σ = αβ τ2, the value of σ being. -
Appendix I: Rossby-wave propagation and shear instability M. E. ...
www.damtp.cam.ac.uk/user/mem/GEFD-SUMMER-shear-instability.pdf30 Sep 2004: Batchelor’s textbook, eq. (7.1.20)). The fact that small Kmeans radian wavelength k1 À 2b suggests that the disturbance should see the whole shear layeras being thin; i.e. ... Rev. Fluid Mech., 20, especially pages381–384. 9. Suppression of shear -
IserlesNorsett2.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2004_05.pdf17 Jun 2004: ω. 500480400. 20. 10. 440420. 30. 40. Figure 2.1: The error for QA1 (bottom) and three different Filon-type methodsQF1 (from the second plot up), scaled by ω. -
Chapter 2 Poisson’s Equation 2.1 Physical Origins Poisson’s equation, …
www.damtp.cam.ac.uk/user/reh10/lectures/nst-mmii-chapter2.pdf8 Mar 2004: 2=. e2. 20. (G. x. )2,. and we calculate G/x as in the worked example in the next section. ... e2. 20. x20. 4π2(x20 (y y0)2 (z z0)2. )3 dy dz = = e216π0x20.
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