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27 Sep 2023: tangential frictional forces (stresses) across material surfaces to derive new equations formomentum conservation with new boundary conditions.

21 Nov 2023: 0.1.4 Behaviour at infinity. We can examine the behaviour of a function f(z) as z by defining anew variable ζ = 1/z and a new function g(ζ) =

1 Nov 2023: matrix A′ with respect to a new basis e′1= f′. 1= e2 and e′2 = f′2 = e1. ... Find the minimum distance from a point on Σ to the origin.[You need not find the new basis vectors explicitly.].

24 Oct 2023: Show thatthe resulting object is neither symmetric nor gauge invariant. Consider a new tensorgiven by.

3 Oct 2023: b) Write the vectors c and d in terms of the new basis set.

4 Oct 2023: Show that subsequently it evolves tobecome the new coherent state eiωt/2 |eiωtα〉.

27 Jan 2023: singularity. By introducing the new coordinates(U,V ), defined by u = tan(U/2), v = cot(V/2), obtain the maximal analytic extension of theRB metric and deduce its Penrose diagram ... The physicalmetric is g = 2ḡ. Introduce a new coordinate r = 1/ and

1 Oct 2023: A2 (t B)2 and using the new.

28 Nov 2023: ON THE EXISTENCE OF OPTIMAL MULTI-VALUED DECODERS AND THEIR ACCURACYBOUNDS FOR UNDERSAMPLED INVERSE PROBLEMS. NINA M. GOTTSCHLING, PAOLO CAMPODONICO, VEGARD ANTUN, AND ANDERS C. HANSEN. ABSTRACT. Undersampled inverse problems occur everywhere in the

23 Oct 2023: 22 p. 21 p. 22. ),. determine the new Hamiltonian H(Q,P). ... Explainwhy the theory of adiabatic invariants cannot be used to calculate the new orbit.