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23 Dec 2021: toughness. and γs is the fracture surface energy of the material (11, 19,20). ... The volumetric injection rate Q0 also varied byan order of magnitude from 2.0 to 20 mL/min.

23 Dec 2021: For an inverse cone, τ ′ is given by. τ ′=20.4p1[10.049p0(p2)], (2.8). ... 5.1) becomesHT γ. 5/20 (H. 3Hx)x =0. (A 9). Dow. nloa.

23 Dec 2021: Therefore, we rewrite our expression as. p = 100a0(g′V)1/2 x3/20 t1. ... tmax = T1β1A1/2γ 5/20 , (4.2)for T1 a dimensionless constant to be determined.

23 Dec 2021: term. s. h. ttps. ://do. i.org. /10. 1017. /jfm. 201. 8.20. ... 8.20. 3. Fluid-driven cracks in brittle hydrogels 451. 100 105 1010.

23 Dec 2021: 50100150200. 3010 20 40 50 60 70 80T1.5. 2.0. 2.5. 0 2 4 6 8 10. ... The point fp(0)is both singular and finite. The distance reached by the current of a flux Q after apropagation time T is already within 20 % of the theoretical radius

23 Dec 2021: Many of these examples involve small particles and viscous fluids. However, while muchresearch has gone into studying both the conditions at which an interface can support a particle[11–20] and ... II. Theory for three-phase. systems, J. Colloid Sci. 20

23 Dec 2021: 3010 20 40 500 100. 100. 10–1 102101. 1.2. 0.4. 0.8. ... 10 cm, (c,d) xi = 15 cm, and (e,f )xi =20 cm.

23 Dec 2021: F D(h/he)=1h. h0[sDeff (h, z)]. αD dz, (2.20). and. F I(h/hT, hmax/he, hmax/hT)=1h. ... 2.31). and (2.20) and (2.21) are rewritten as. F ={F D(Bh,ΛD,αD) (r > rb)F I(δBh, Bhmax, δBhmax, δ,ΛD,ΛI,αD,αI) (r < rb).

23 Dec 2021: 3.8. 3.7. 3.6. 3.5. 3.410–6 10–4 10–2. 5.5. 5.0. 4.55 10 15 20. ... 40. 35. 30. 25. 20. 15. 10. 5. 010–4 10–2 100.

23 Dec 2021: 1H31(T). dH1(T)dT. =2P1(X, T). X2, (3.7b). and the integral equations are 1/20.