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28 Dec 2013: 28 September 2013, 2:30 pm. Peter Warlock: Capriol. Franz Schubert: Variations in A flat major, Op 35 / D 813.

5 Oct 2013: Our approach is modeled on the abstractStetter-Lindberg-Skeel error analysis [15, 12, 14], which treats the initial value problem (IVP) as an op-erator equation approximated by a discrete operator

27 Feb 2013: perpendicular to OP , find the equation of the orbit under the assumptions. ... dicular to OP , where v2 < k/a2. Use the orbit equation to prove that P spirals in.

5 Oct 2013: as op-posed to an mm section).

26 Jul 2013: In addi-tion, the parameter space is vast with many interactingvariables—geometry, material properties, kinematics.The environment is constantly changing hence evolvingorganisms are “chasing a moving target” making op-timization studies

19 Oct 2013: Section 7 shows how the PV inversion op-erators can be made Galilean invariant in an appropriatesense, and section 8 presents concluding remarks onconservation and related issues. ... Attention is restricted first of all to PV inversion op-erators for

26 Jul 2013: c same as b but for dimers pointing in the op-posite direction; note the change in the sign of the dimer-dimereffective interaction.

26 Jul 2013: Thecost function J must weigh together the state x, thecontrol u, and the noise w; moreover, since the GL op-erator is time invariant, one can apply the control theoryfor infinite

5 Oct 2013: as op-posed to an mm section).

26 Jul 2013: The op-timization is performed numerically as before, but includingthe constraint that = 0 for 1. ... For a given aspect ratio, the maximal efficiency mustnot increase as the body becomes less porous, since the op-timal profile for a more porous body

27 Aug 2013: On a cylindrical shell, the gradient op-erator reads. = eθ1R. θ.

26 Jul 2013: a more traditional measure of locomotion cost themechanical work of the crawling organism, we find the op-posite result.

5 Oct 2013: In the finite-dimensional case every self-adjoint matrix is tridiagonalizable.This is not the case in infinite dimensions, however, it is well known that if a self-adjoint op-erator ... The problem is that our op-erator may not have a cyclic vector,

19 Oct 2013: British Higher Education Policy in the last Twenty Years: The Murder of a Profession. Richard F. Gombrich. Tokyo, January 2000. Preamble. This is the text of a lecture I gave on 7 January 2000 in Tokyo at the Graduate Institute of Policy Studies

5 Oct 2013: In the finite-dimensional case every self-adjoint matrix is tridiagonalizable.This is not the case in infinite dimensions, however, it is well known that if a self-adjoint op-erator ... The problem is that our op-erator may not have a cyclic vector,

19 Oct 2013: The reported conference discussion (Jeffreys, op.cit., pp. 210–11) illustrates that in 1933 no-one, not even Jeffreys, had the faintest idea ofwhat kind of fluid dynamics might be involved.

5 Oct 2013: Our approach is modeled on the abstractStetter-Lindberg-Skeel error analysis [15, 12, 14], which treats the initial value problem (IVP) as an op-erator equation approximated by a discrete operator

26 Jul 2013: The optimal elastic flagellumSaverio E. Spagnoliea and Eric Laugab. Department of Mechanical and Aerospace Engineering, University of California, San Diego,9500 Gilman Drive, La Jolla, California 92093-0411, USA. Received 25 September 2009; accepted

19 Oct 2013: already alluded to. In any case, the work of Lindzen and Tsay (op.

5 Oct 2013: exponential convergence whenevern = O (. m). We note that the use of polynomial least squares for overcoming the Gibbs phenomenon, as op-posed to the Runge phenomenon, is far less well known.