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. 2019 Dec 4;19(3):1015–1034. doi: 10.1007/s10237-019-01268-5

Table 7.

Laplace law

Fibers R (mm) T (mm) Vwall (cm3) V0 (ml) Vinfl (ml) Vcont (ml) IF (%) EF (%) σ¯infl1st (kPa) σ¯cont1st (kPa) σ¯inflcirc (kPa) σ¯contcirc (kPa) σinflLa (kPa) σcontLa (kPa)
isotropic 20 0.5 2.6 33.5 59.7 58.6 178.0 1.8 53.3 52.8 46. 4 45.9 46. 6 46.6
tr. iso. 20 0.5 2.6 33.5 57.0 43.7 170.2 23.4 52.8 42.8 48. 4 40.8 44. 6 44.7
ortho. 20 0.5 2.6 33.5 56.0 49.9 167.3 11.0 50.5 44.8 44. 0 39.0 43. 8 43.9
incomp. 20 0.5 2.6 33.5 55.9 50.5 166.9 9.6 50.4 47.0 43. 9 41.0 43. 7 43.8
isotropic 20 2.5 14.2 33.5 48.6 47.7 145.0 1.7 8.7 7.9 7. 5 6.7 7. 1 7.2
tr. iso. 20 2.5 14.2 33.5 46.3 22.9 138.2 50.5 8.5 12.8 7. 7 8.6 6. 8 7.1
ortho. 20 2.5 14.2 33.5 45.5 22.0 136.0 51.7 8.1 5.1 7. 0 3.2 6. 7 7.0
isotropic 20 5.0 31.9 33.5 44.5 43.8 133.0 1.6 4.0 3.1 3. 4 2.5 3. 1 3.1
tr. iso. 20 5.0 31.9 33.5 42.5 21.7 126.9 48.9 3.9 13.0 3. 5 4.2 2. 9 3.2
ortho. 20 5.0 31.9 33.5 41.8 20.7 124.8 50.5 3.7 4.3 3. 1 − 1.1 2. 9 3.1
isotropic 25 0.5 4.0 65.4 119.9 117.7 183.2 1.8 68.5 68.0 59. 7 59.2 60. 2 60.2
tr. iso. 25 0.5 4.0 65.4 114.5 98.4 175.0 14.1 67.9 60.7 62. 3 57.5 57. 5 57.5
ortho. 25 0.5 4.0 65.4 112.4 104.2 171.7 7.3 64.9 60.1 56. 5 52.3 56. 4 56.5
incomp. 25 0.5 4.0 65.4 112.0 104.8 171.2 6.4 64.8 61.9 56. 4 54.0 56. 3 56.3
isotropic 25 2.5 21.7 65.4 97.5 95.8 149.0 1.7 11.1 10.3 9. 7 8.8 9. 3 9.3
tr. iso. 25 2.5 21.7 65.4 93.0 45.7 142.2 50.8 10.9 13.3 10. 0 10.3 8. 9 9.2
ortho. 25 2.5 21.7 65.4 91.5 43.9 139.9 52.1 10.5 5.8 9. 0 4.6 8. 8 9.1
isotropic 25 5.0 47.6 65.4 89.5 87.0 136.8 1.7 5.1 4.2 4. 4 3.5 4. 1 4.1
tr. iso. 25 5.0 47.6 65.4 85.3 43.0 130.4 49.5 5.0 12.7 4. 5 5.5 3. 9 4.1
ortho. 25 5.0 47.6 65.4 83.8 41.2 128.2 50.8 4.7 4.5 4. 0 0.3 3. 8 4.1
isotropic 30 0.5 5.8 113.1 212.1 208.3 187.5 1.8 84.0 83.7 73. 2 72.9 74. 1 74.1
tr. iso. 30 0.5 5.8 113.1 202.3 183.3 178.9 9.4 83.4 78.0 76. 6 73.7 70. 7 70.7
ortho. 30 0.5 5.8 113.1 198.3 187.5 175.3 5.4 79.5 75.2 69. 3 65.5 69. 3 69.3
incomp. 30 0.5 5.8 113.1 197.5 188.2 174.7 4.7 79.5 76.9 69. 2 67.0 69. 0 69.1
isotropic 30 2.5 30.7 113.0 172.2 169.2 152.4 1.8 13.7 12.9 11. 9 11.0 11. 5 11.5
tr. iso. 30 2.5 30.7 113.0 164.4 80.9 145.5 50.8 13.4 14.1 12. 2 11.9 11. 0 11.3
ortho. 30 2.5 30.7 113.0 161.9 77.3 143.2 52.3 12.9 6.9 11. 1 5.9 10. 9 11.2
isotropic 30 5.0 66.5 113.0 158.2 155.5 139.9 1.7 6.3 5.4 5. 4 4.5 5. 1 5.1
tr. iso. 30 5.0 66.5 113.0 150.7 75.4 133.3 50.0 6.1 12.6 5. 5 6.6 4. 8 5.1
ortho. 30 5.0 66.5 113.0 148.2 72.3 131.1 51.2 5.8 4.7 5. 0 1.4 4. 8 5.0

Comparison of FE-based mean principal stresses (σ¯infl1st, σ¯cont1st) and mean circumferential fiber stresses (σ¯inflcirc, σ¯contcirc) with Laplace estimations (σinflLa, σcontLa) for the inflated (infl.) and the fully contracted (cont.) state. Radius (R), which is the inverse of curvature C, and thickness (T) of the spheres are varied. Three different fiber laws are applied to each of the resulting spheres: isotropic, transversely isotropic (tr. iso.), and orthotropic (ortho.). For the thinnest spheres, (T=0.5mm) a fully incompressible (incomp.) case is included. Additionally, wall volume Vwall, initial cavity volume V0, inflated cavity volume Vinfl and cavity volume at contracted state Vcont are given as well as inflation fraction (IF) and ejection fraction (EF)

In bold are the circumferential fiber stresses and Laplace estimations for the inflated state; in these cases the Laplace laws are known to be almost exact