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29 Jan 2013: modes, corresponding to radial deformations Ũr cos nθ; (b) in-plane ex-tensional ring modes, corresponding to tangential deformations Ũθ sin nθ;and (c) out-of-plane flexural ring modes, corresponding ... to longitudinaldeformations Ũz cos nθ.

4 Nov 2013: sin. 4)(cos. 22 I. b. bI. ... σωσ cos. 24. 2. 22. = , (35). respectively. The mid-span back face deflection and velocity are given by Eqs.

19 Oct 2013: Further detailsof the method used can be found in appendix B and inN88. ... 4, and (b) that when judged by comparison withthe reinitialized primitive equation integration, the nor-.

19 Oct 2013: where θ is the polar angle and where the outward normal n̂ now has Cartesiancomponents (cos θ, sin θ). ... Then, noting that the Cartesian components of U atr = b are ( sin θ, cos θ)Γ /(2bπ), we can easily evaluate the integral.

5 Oct 2013: As is evident, the quantity cos (θn,n) is exponentially small in n. ... 100. 106. 1010. (a) (b) (c). Figure 1: (a): cos(θn,n) against n.

10 Jan 2013: terminus of the protein) in COS-7 cells (where the protein is not. ... RBL?2H3 cell line), B cells and macrophages (Figure 1 and datanot shown).

21 Mar 2013: from the start of the alphabet (e.g, a,b,c,. ) take values 1,. ... dx , as before (we note here that A, B, C and D, defined by (2.9).

27 Jan 2013: B Thomas Algorithm 159. C Green’s Functions for a Layered Halfspace 161. ... a) Wheel flat (b) Uneven rail joint. Figure 2.2: Examples of wheel and rail discontinuities.