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27 Jan 2024: 2.3.1 The Gravitational Field 22. 2.3.2 Escape Velocity 24. 2.3.3 Inertial vs Gravitational Mass 25.

2 Jan 2024: 24, 313–358.PELLE, D.W., BROKAW, C.J., LESICH, K.A. & LINDEMANN, C.B. 2009 Mechanical properties of the.

26 Jun 2024: in (1.24) because E = (0,0,E) lies parallel to the side of the torus, not perpendicular. ... Instead, both (1.23) and (1.24) are best thought of as integrating the 2-form Fµν over.

26 Jun 2024: where. Kµ = µtr. A@A. 2i. 3AAA. (2.24). This means that, as in the Maxwell case, the theta term does not change the. ... derivative (2.24), the temporal component was K0 = 42W. For now, the key property of W(A) that we will need is.

1 Dec 2023: not always) suppress any interaction [24]. ... 24] E. Chaparian, A. Wachs, and I. A. Frigaard, Inline motion and hydrodynamic interaction of 2D particlesin a viscoplastic fluid, Phys.

21 Nov 2023: af(t) dt. b. ag(t) dt , (24). »»»»»»»». b. af(t) dt. »»»»»»»». ... 24. Taylor series for analytic functions. Zeros, Poles and Essential Singularities.

1 Dec 2023: Moreover, the onlyexisting models of freeness are semi-empirical and based on the average filter resistance of thecompacting pulp [22–24]. ... 24)The integral of Eq. (22) across the height of the solid also provides the global force balancecondition,.

13 Feb 2024: Rotletflows arise from (d) the bacterium Escherichia coli under confinement, generating flow field in (e) [24], (f)a magnetic nano stir bar [25], and (g) a macroscopic stirrer [26]. ... 23 eqs. 29-30. Stokeslet Main text eq. 24 eqs. 32-34.Rotlet Appendix

31 May 2024: S T)µ1.µp1.r1.q1.s. = Sµ1.µp1.qT1.r. 1.s (2.24). Given an (r, s) tensor T , we can also construct a tensor of lower rank (r

24 Jul 2023: δjk 12. dR̂jdŝ. dR̂kdŝ. )(ũk (R̂) ũk (ŝ). )dŝ,. (2.24). where R̂i = R̃i(ŝ). ... 3.1.1. Computation of forces and torquesUnder this parametrisation, (2.24) becomes. Ji = η̃s2. [