Euler Buckling as a Model for the Curvature and Flexion of the Human Lumbar Spine
The upright thoraco-lumbar spine resembles an Euler column buckled in the second mode (n = 2) when viewed in the sagittal plane. An advantage of n = 2 buckling is that further load can be carried without adopting a stooped posture. Flexion of the spine is considered as the first quarter cycle of an...
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Published in | Proceedings of the Royal Society. B, Biological sciences Vol. 263; no. 1375; pp. 1383 - 1387 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
London
The Royal Society
22.10.1996
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Subjects | |
Online Access | Get full text |
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Summary: | The upright thoraco-lumbar spine resembles an Euler column buckled in the second mode (n = 2) when viewed in the sagittal plane. An advantage of n = 2 buckling is that further load can be carried without adopting a stooped posture. Flexion of the spine is considered as the first quarter cycle of an Euler pendulum. This is possible if the antagonistic muscles which control movement increase the bending stiffness, El, to a value of about 15 N m2. If the muscles are incapable of increasing El sufficiently to support the weight of the body, or any excess load, the spine will be dynamically unstable. This conclusion is consistent with a static model which considers spinal instability as 'loss of stiffness’ and a dynamic model which suggests that it arises from ineffective adaptive control. The flexed spine resembles an n = 1 buckled column. |
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Bibliography: | istex:5AFCA82650BD67B61CE0FD6D0E62057C12D6D0C7 ark:/67375/V84-42404KNS-N This text was harvested from a scanned image of the original document using optical character recognition (OCR) software. As such, it may contain errors. Please contact the Royal Society if you find an error you would like to see corrected. Mathematical notations produced through Infty OCR. ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
ISSN: | 0962-8452 1471-2954 |
DOI: | 10.1098/rspb.1996.0202 |