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A reduced-order model of the spine to study pediatric scoliosis

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Abstract

The S-shaped curvature of the spine has been hypothesized as the underlying mechanical cause of adolescent idiopathic scoliosis. In earlier work, we proposed a reduced-order model in which the spine was viewed as an S-shaped elastic rod under torsion and bending. Here, we simulate the deformation of S-shaped rods of a wide range of curvatures and inflection points under a fixed mechanical loading. Our analysis determines three distinct axial projection patterns of these S-shaped rods: two loop (in opposite directions) patterns and one Lemniscate pattern. We further identify the curve characteristics associated with each deformation pattern, showing that for rods deforming in a Loop1 shape the position of the inflection point is the highest and the curvature of the rod is smaller compared to the other two types. For rods deforming in the Loop2 shape, the position of the inflection point is the lowest (closer to the fixed base) and the curvatures are higher than the other two types. These patterns matched the common clinically observed scoliotic curves—Lenke 1 and Lenke 5. Our S-shaped elastic rod model generates deformations that are similar to those of a pediatric spine with the same sagittal curvature characteristics and it can differentiate between the clinically observed deformation patterns.

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Acknowledgements

Sunder Neelakantan and Prashant K. Purohit acknowledge partial support for this work through an NSF Grant NSF CMMI 1662101. Saba Pasha acknowledges partial support for this work through a research grant from the Scoliosis Research Society and the National Institute of Health (NIH)  R21 AR075971 01A1.

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Correspondence to Saba Pasha.

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Appendix

Appendix

We present the sagittal view of the deformed configuration of the rods presented in Fig. 8 in Fig. 11. We see that the rods bend toward the +ve y- axis, which would be the case given a -ve \(m_x(s)\) moment acting along the length of the rod.

Fig. 11
figure 11

Sagittal view of the deformed configuration of the \({37}^{\circ }\) average curve in Fig. 8

We present the equations of the surfaces and the coefficient of determination(\({\varvec{R^2}}\)) used in Fig. 3 in Tables 4 and 5. We present the equations of the loop–Lemniscate classification surfaces in Table 4. We also present the equations of the surfaces generated from the uprightness check in Table 5.

Table 4 Equations of the loop–Lemniscate classification surfaces (Fig. 3 blue surface) for the 3 cases in along with the coefficient of determination
Table 5 Equations of the uprightness condition surfaces (Fig. 3 yellow surface) for the 3 cases along with the coefficient of determination. Here, \(x = \kappa _P\), \(y = \kappa _N\) and \(S = f(x,y)\)

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Neelakantan, S., Purohit, P.K. & Pasha, S. A reduced-order model of the spine to study pediatric scoliosis. Biomech Model Mechanobiol 20, 467–480 (2021). https://doi.org/10.1007/s10237-020-01394-5

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