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8 Mar 2024: 39. Cambridge Educational Research e-Journal | Vol. 10 | 2023. Note: From top to bottom: Excerpt 1 (BF_005-B-B), Excerpt 2 (IS_079-B-B), Excerpt 3 ... Cambridge Educational Research e-Journal | Vol. 10 | 2023. Note: From top to bottom: Excerpt 12

12 Jun 2024: ferentiation, in the sense that. Zb. a. dxdf. dx= f(b) f(a). ... equation tells us that. µ0I =. Z. C. B dx =. Z 2. 0. d b() =) B(x) =µ0I. 2( sin , cos , 0).

19 Jun 2024: distributions of nodes from A and B in the embedding space(to have |UA||A|. ... Group AGroup BGroup AGroup B. (b) The fractions of influencednodes in the two groups.

27 Apr 2024: magnetic fields through the Lorentz force law,. F = q(E ṙ B) (1.2). ... field causes a particle to move in circles in the plane perpendicular to B.

19 Jun 2024: Wethen multiply the sum by b/n > 2m. As long as b, b/n(and thus also n/b) can be represented with sufficient preci-sion, which is the case in ... Details about parameters and thealgorithm can be found in Section B in the appendix.

19 Jun 2024: Z. (b). X. Y. Z. 12 / 26. D-separation (“directed separation”) in Bayesian networks. ... over A,B,C :. p(D) =a,b,c. p(A = a,B = b,C = c,D). 28 / 26.

20 Mar 2024: fields, E(x,t) and B(x,t). Both of these fields are spatial 3-vectors. ... tand B = A (1.2). which ensure that two of Maxwell’s equations, B = 0 and dB/dt = E, holdimmediately as identities.

26 Jun 2024: eigenvector (T A0)b actually vanishes. Indeed, this is clearly the case if 0 = 0. ... Each of these generators gives a unique eigenstate (R)b, and hence a massless mode.

19 Jun 2024: 142. B.2.3 Some frustrated K4 structures (treewidth 3). 145. B.3 Discussion. ... i,j) E and a,b B, which we term the edge or pairwise potentials.

19 Jun 2024: over A,B,C :. p(D) =. a,b,c. p(A = a,B = b,C = c,D). 8 / 32. ... c. b. a. p(D | c)p(c | b)p(b | a)p(a).