Добавил:
kiopkiopkiop18@yandex.ru t.me/Prokururor I Вовсе не секретарь, но почту проверяю Опубликованный материал нарушает ваши авторские права? Сообщите нам.
Вуз: Предмет: Файл:
Ординатура / Хирургия / Библиотека им академика М.И. Перельмана / Книга_6012_Библиотеки_им_академика_М_И_Перельмана.pdf
Скачиваний:
0
Добавлен:
29.08.2026
Размер:
93 Мб
Скачать
Chapter 6 Biomechanics of the Spinal Motion Segment 113
Level
Load (N)
Compressive loads
A
B
FIG. 6.25 (A) Sagittal view of computational model and (B) stress distributions following total articial disc
placement at L5–S1. (From Knapik GG, Mendel E, Marras WS. Use of a personalized hybrid biomechanical model to assess change in lumbar spine function with a TDR compared to an intact spine. Eur Spine J. 2012;21[suppl 5]:S641-S652.)
SECTION
I
L1–L2 SUP
L1–L2 INF
L2–L3 SUP
L2–L3 INF
L3–L4 SUP
L3–L4 INF
L4–L5 SUP
L4–L5 INF
L5–S1 SUP
L5–S1 INF
0
–500
–1000
–1500
–2000
–2500
–3000
FIG. 6.26 Average of the peak compression loads on the lumbar spine endplates as a function of intact spine
versus total articial disc replacement (TDR) spine and external loading condition (bending while unloaded 0 kg, lifting 9.5 kg, lifting 19 kg). INF, inferior; SUP, superior. (From Knapik GG, Mendel E, Marras WS. Use of a personalized hybrid biomechanical model to assess change in lumbar spine function with a TDR compared to an intact spine. Eur Spine J. 2012;21[suppl 5]:S641-S652.)
–3500
–4000
–4500
T12–L1 SUP
T12–L1 INF
0 kg Intact
0 kg TDR
9.5 kg Intact
9.5 kg TDR
19 kg Intact
19 kg TDR
114 BASIC SCIENCE
Sagittal range of motion
Level
Range of motion (degrees)
16
14
12
10
8
6
4
2
0
L5–S1 L4–L5 L3–L4 L2–L3 L1–L2 T12–L1
FIG. 6.27 Mean sagittal plane range of motion at each lumbar level as
a function of intact spine versus total articial disc replacement (TDR) spine and external loading condition (bending while unloaded 0 kg, lifting
9.5 kg, lifting 19 kg). (From Knapik GG, Mendel E, Marras WS. Use of a personalized hybrid biomechanical model to assess change in lumbar spine function with a TDR compared to an intact spine. Eur Spine J. 2012;21[suppl 5]:S641-S652.)
0 kg Intact
0 kg TDR
9.5 kg Intact
9.5 kg TDR
19 kg Intact
19 kg TDR
is alteration could change the kinematic signature of the spine.
Finally, a narrowed disc space could compromise the protection of the nerve root because there is less space for the nerve root to pass through the intervertebral foramen. A compromise of the disc could lead to load transmission irregularities, instability, motion restrictions, and a compro­mise of the nerve root. is is just one example of how inter­related the components of the spine are from a biomechanical perspective.
As can be seen from this discussion, biomechanics of the spine not only can inuence the various dimensions of the biomechanical system, but it also can inuence the biochemi­cal behavior of the system. Because biomechanical consider­ations provide an understanding of the forces that are generated on the system, some authors are beginning to consider the spine as a mechanobiologic system.

Summary

By nature, the spine is a complex structure that provides protection for the spinal cord and a structure to support loads in numerous postures and positions. In addition, the healthy spine limits physiologic movement to conditions that protect the structures of the spine. With trauma and degeneration, the spine loses its ability to achieve these functions adequately.
Biomechanics provides a means to characterize and assess the status of the spine quantitatively and precisely. Quantica­tion provides a rationale for one to determine “how much is too much” exposure to the physical conditions that might damage the spinal system. is chapter has systematically summarized and characterized the capacity of the spinal motion segments in terms of kinematic capacity and load tolerance.
e spinal structures themselves are physiologically unique, and have evolved in such a manner that their functions are
unique. Although this chapter has examined the capacity of the individual motion segments, this evaluation should make it clear that the spine is truly a system of components that act collectively and interactively to achieve the functions of motion and load support. e kinematic and load support capacities of the motion segment vary signicantly as a func-
tion of spinal level, direction of motion, direction of load application, and temporal exposure characteristics.
Although presented as basic information, this information should be considered the fundamental scientic foundation for understanding how the spine functions, how disorders and pain might occur in the spine, how exposure to ADLs and occupational conditions might aect the spine status, and what functions need to be restored clinically. Biomechanical features and function change throughout life. Aging alone alters the biomechanical properties of the spine. It has also been well established, however, that various exposures can greatly accelerate the degenerative process and the biome­chanical functioning of the spine.
As knowledge of the spine increases, it is clear that a bio­mechanical foundation is essential for prevention and treat­ment of spinal disorders. A better understanding of spine function can be achieved through a better quantication of physical attributes, yielding improved sensitivity and specic­ity of functional understanding and interventions.

KEY REFERENCES

1. Adams MA, Bogduk N, Burton AK, Dolan P. The Biomechanics of
Back Pain. Edinburgh: Elsevier; 2013.
2.
White AA 3rd, Panjabi MM. Clinical Biomechanics of the Spine.
Philadelphia: Lippincott-Raven; 1990.
3.
Marras WS. The Working Back: A Systems View. Hoboken, NJ: John
Wiley and Sons; 2008.
4.
McGill S. Ultimate Back Fitness and Performance. Waterloo,
Canada: Wabuno Publishers; 2004.
5.
National Research Council & Institute of Medicine [NRC-IOM].
Musculoskeletal Disorders and the Workplace: Low Back and Upper
Extremities. Washington, DC: National Academy Press; 2001.

REFERENCES

1. Bernhardt M, White AA, Panjabi MM. Biomechanical considerations of spinal stability. In: Herkowitz HN, Garn SR, Eismont FJ, eds. Rothman-Simeone e Spine. Philadelphia: WB Saunders; 2006.
2. White AA, Panjabi MM. Clinical Biomechanics of the Spine. Philadelphia: Lippincott-Raven; 1990.
3. Quint U, Wilke HJ, Shirazi-Adl A, et al. Importance of the intersegmental trunk muscles for the stability of the lumbar spine: a biomechanical study in vitro. Spine. 1998;23:1937-1945.
4. Cholewicki J, McGill S. Mechanical stability of the in vivo lumbar spine: implications of injury and chronic low back pain. Clin Biomech (Bristol, Avon). 1996;11:1-15.
5. Farfan HF, Gracovetsky S. e nature of instability. Spine. 1984;9:714-719.
6. Granata KP, Marras WS. Cost-benet of muscle cocontraction in protecting against spinal instability. Spine. 2000;25:1398-1404.
7. Panjabi MM. Clinical spinal instability and low back pain. J Electromyogr Kinesiol. 2003;13:371-379.
Chapter 6 Biomechanics of the Spinal Motion Segment 115
8. Reeves NP, Narendra KS, Cholewicki J. Spine stability: the six blind men and the elephant. Clin Biomech (Bristol, Avon). 2007;22:266-274.
9. Marras WS. e Working Back: A Systems View. Hoboken, NJ: John Wiley & Sons; 2008.
10. Lee CK. Accelerated degeneration of the segment adjacent to a lumbar fusion. Spine. 1988;13:375-377.
11. Ghiselli G, Wang JC, Bhatia NN, et al. Adjacent segment degeneration in the lumbar spine. J Bone Joint Surg Am. 2004;86:1497-1503.
12. van Ooij A, Oner FC, Verbout AJ. Complications of articial disc replacement: a report of 27 patients with the SB Charite disc. J Spinal Disord Tech. 2003;16:369-383.
13. Dooris AP, Goel VK, Grosland NM, et al. Load-sharing between anterior and posterior elements in a lumbar motion segment implanted with an articial disc. Spine. 2001;26:E122-E129.
14. Brinkmann P, Biggermann M, Hilweg D. Prediction of the compressive strength of human lumbar vertebrae. Clin Biomech (Bristol, Avon). 1989;4:S1-S27.
15. Yoganandan N, Larson SJ, Gallagher M, et al. Correlation of microtrauma in the lumbar spine with intraosseous pressures. Spine. 1994;19:435-440.
16. Reinhold M, Audigé L, Schnake KJ, et al. AO spine injury classication system: a revision proposal for the thoracic and lumbar spine. Eur Spine J. 2013;22(10):2184-2201.
17. Haughton VM, Schmidt TA, Keele K, et al. Flexibility of lumbar spinal motion segments correlated to type of tears in the annulus brosus. J Neurosurg. 2000;92:81-86.
18. Adams MA, Bogduk N, Burton AK, et al. e Biomechanics of Back Pain. Edinburgh: Churchill Livingstone; 2013.
19. Gertzbein SD, et al. Centrode patterns and segmental instability in degenerative disc disease. Spine. 1985;10:257-261.
20. Zhao F, Pollintine P, Hole BD, et al. Discogenic origins of spinal instability. Spine. 2005;30:2621-2630.
21. Adams MA, Hutton WC. e relevance of torsion to the mechanical derangement of the lumbar spine. Spine. 1981;6:241-248.
22. Moroney SP, Schultz AB, Miller JA, et al. Load-displacement properties of lower cervical spine motion segments. J Biomech. 1988;21:769-779.
23. Panjabi MM, Brand RA, White AA. ree-dimensional exibility and stiness properties of the human thoracic spine. J Biomech. 1976;9:185-192.
24. Bogduk N. Clinical Anatomy of the Lumbar Spine and Sacrum. Edinburgh: Churchill Livingstone; 2005.
25. Pearcy MJ, Tibrewal SB. Axial rotation and lateral bending in the normal lumbar spine measured by three-dimensional radiography. Spine. 1984;9:582-587.
26. Cholewicki J, Crisco JJ, Oxland TR, et al. Eects of posture and structure on three-dimensional coupled rotations in the lumbar spine: a biomechanical analysis. Spine. 1996;21:2421-2428.
27. Pearcy M, Portek I, Shepherd J. ree-dimensional x-ray analysis of normal movement in the lumbar spine. Spine. 1984;9:294-297.
28. Panjabi M, et al. ree-dimensional movements of the upper cervical spine. Spine. 1988;13:726-730.
29. Yamamoto I, Panjabi MM, Crisco T, et al. ree-dimensional movements of the whole lumbar spine and lumbosacral joint. Spine. 1989;14:1256-1260.
30. Mimura M, et al. Disc degeneration aects the multidirectional exibility of the lumbar spine. Spine. 1994;19:1371-1380.
31. Oxland TR, Panjabi MM. e onset and progression of spinal injury: a demonstration of neutral zone sensitivity. J Biomech. 1992;25:1165-1172.
32. Panjabi MM. e stabilizing system of the spine. Part II: neutral zone and instability hypothesis. J Spinal Disord. 1992;5:390-396.
33. Yoganandan N. Biomechanical identication of injury to an
intervertebral joint. Clin Biomech (Bristol, Avon). 1986;1:149.
34. Hoy MG, Zajac FE, Gordon ME. A musculoskeletal model of the human lower extremity: the eect of muscle, tendon, and moment arm on the moment-angle relationship of musculotendon actuators at the hip, knee, and ankle. J Biomech. 1990;23:157-169.
35. Nordin M, Frankel V. Basic Biomechanics of the Musculoskeletal System. Philadelphia: Lea & Febiger; 1989.
36. Solomonow M. Ligaments: a source of work-related musculoskeletal disorders. J Electromyogr Kinesiol. 2004;14:49-60.
37. Solomonow M, Zhou BH, Baratta RV, et al. Biomechanics of increased exposure to lumbar injury caused by cyclic loading. Part 1: loss of reexive muscular stabilization. Spine. 1999;24:2426-2434.
38. Solomonow M, Zhou BH, Harris M, et al. e ligamento-muscular stabilizing system of the spine. Spine. 1998;23:2552-2562.
39. Stubbs M, et al. Ligamento-muscular protective reex in the lumbar spine of the feline. J Electromyogr Kinesiol. 1998;8:197-204.
40. Gedalia U, et al. Biomechanics of increased exposure to lumbar injury caused by cyclic loading. Part 2: recovery of reexive muscular stability with rest. Spine. 1999;24:2461-2467.
41. Wang JL, Parnianpour M, Shirazi-Adl A, et al. Viscoelastic nite-element analysis of a lumbar motion segment in combined compression and sagittal exion: eect of loading rate. Spine. 2000;25:310-318.
42. Solomonow M, Zhou B, Baratta RV, et al. Neuromuscular disorders associated with static lumbar exion: a feline model. J Electromyogr Kinesiol. 2002;12:81-90.
43. Solomonow M, et al. Biexponential recovery model of lumbar viscoelastic laxity and reexive muscular activity aer prolonged cyclic loading. Clin Biomech (Bristol, Avon). 2000;15:167-175.
44. Solomonow M, Eversull E, He Zhou B, et al. Neuromuscular neutral zones associated with viscoelastic hysteresis during cyclic lumbar exion. Spine. 2001;26:E314-E324.
45. Jager M, Luttmann A. Compressive strength of lumbar spine elements related to age, gender, and other inuences. J Electromyogr Kinesiol. 1991;1:291-294.
46. Jager M, Luttmann A, Laurig W. Lumbar load during one-hand bricklaying. Int J Indust Ergo. 1991;8: 261-277.
47. Gallagher S, Marras WS, Litsky AS, et al. Torso exion loads and the fatigue failure of human lumbosacral motion segments. Spine. 2005;30:2265-2273.
48. Brinkmann P, Biggermann M, Hilweg D. Fatigue fracture of human lumbar vertebrae. Clin Biomech (Bristol, Avon). 1988;3:S1-S23.
49. Gallagher S, Marras WS, Litsky AS, et al. An exploratory study of loading and morphometric factors associated with specic failure modes in fatigue testing of lumbar motion segments. Clin Biomech (Bristol, Avon). 2006;21:228-234.
SECTION
I
116 BASIC SCIENCE
50. Cyron BM, Hutton WC. e behaviour of the lumbar intervertebral disc under repetitive forces. Int Orthop. 1981;5:203-207.
51. Cyron BM, Hutton WC, Troup JD. Spondylolytic fractures. J Bone Joint Surg Br. 1976;58:462-466.
52. Lamy C, Bazergui A, Kraus H, et al. e strength of the neural arch and the etiology of spondylolysis. Orthop Clin North Am. 1975;6:215-231.
53. Weiss EB. Stress at the lumbosacral junction. Orthop Clin North Am. 1975;66:83.
54. McGill S. Low Back Disorders: Evidence-Based Prevention and Rehabilitation. Champaign, IL: Human Kinetics; 2002.
55. Marras WS. Occupational low back disorder causation and control. Ergonomics. 2000;43:880-902.
56. National Research Council & Institute of Medicine [NRC­IOM]. Musculoskeletal Disorders and the Workplace: Low Back and Upper Extremities. Washington, DC: National Academy Press; 2001.
57. Yingling VR, McGill SM. Anterior shear of spinal motion segments: kinematics, kinetics, and resultant injuries observed in a porcine model. Spine. 1999;24:1882-1889.
58. Yingling VR, McGill SM. Mechanical properties and failure mechanics of the spine under posterior shear load: observations from a porcine model. J Spinal Disord. 1999;12(6):501-508.
59. Gallagher S, Marras WS. Tolerance of the lumbar spine to shear: a review and recommended exposure limits. Clin Biomech (Bristol, Avon). 2012;27(10):973-978.
60. Adams MA, Dolan P. Spine biomechanics. J Biomech. 2005;38:1972-1983.
61. Oxland TR, Crisco JJ, Panjabi MM, et al. e eect of injury on rotational coupling at the lumbosacral joint: a biomechanical investigation. Spine. 1992;17:74-80.
62. Oxland TR, et al. e relative importance of vertebral bone density and disc degeneration in spinal exibility and interbody implant performance: an in vitro study. Spine. 1996;21:2558-2569.
63. Oxland TR, Grant JP, Dvorak MF, et al. Eects of endplate removal on the structural properties of the lower lumbar vertebral bodies. Spine. 2003;28:771-777.
64. Adams MA, Dolan P, Hutton WC. e lumbar spine in backward bending. Spine. 1988;13:1019-1026.
65. Green TP, Allvey JC, Adams MA. Spondylolysis: bending of the inferior articular processes of lumbar vertebrae during simulated spinal movements. Spine. 1994;19:2683-2691.
66. Adams MA, Dolan P. A technique for quantifying the bending moment acting on the lumbar spine in vivo. J Biomech. 1991;24:117-126.
67. Adams MA, Hutton WC. e eect of posture on diusion into lumbar intervertebral discs. J Anat. 1986;147: 121-134.
68. Adams MA, Hutton WC, Stott JR. e resistance to exion of the lumbar intervertebral joint. Spine. 1980;5: 245-253.
69. Adams MA, Green TP, Dolan P. e strength in anterior bending of lumbar intervertebral discs. Spine. 1994;19:2197-2203.
70. Adams MA, Dolan P. Time-dependent changes in the lumbar spine’s resistance to bending. Clin Biomech (Bristol, Avon). 1996;11:194-200.
71. Peng B, et al. Possible pathogenesis of painful intervertebral disc degeneration. Spine. 2006;31:560-566.
72. Benzel EC, Kayanja M, Fleischman A, Roy S. Spine biomechanics: fundamentals and future. Clin Neurosurg. 2006;53:98-105.
73. Cheng B, Goel V. Foreword, Biomechanics Special Issue. Int J Spine Surg. 2015;9:31.
74. Marras WS, et al. e classication of anatomic- and
symptom-based low back disorders using motion measure models. Spine. 1995;20:2531-2546.
75. Marras WS, Wongsam PE. Flexibility and velocity of the normal and impaired lumbar spine. Arch Phys Med Rehabil. 1986;67:213-217.
76. Stokes IA, Wilder DG, Frymoyer JW, et al. 1980 Volvo award in clinical sciences. Assessment of patients with low-back pain by biplanar radiographic measurement of intervertebral motion. Spine. 1981;6:233-240.
77. Marras WS, et al. e quantication of low back disorder using motion measures: methodology and validation. Spine. 1999;24:2091-2100.
78. Anderst WJ, Donaldson WF 3rd, Lee JY, Kang JD. Cervical motion segment percent contributions to exion-extension during continuous functional movement in control subjects and arthrodesis patients. Spine. 2013;38(9): E533-E539.
79. Anderst WJ, Lee JY, Donaldson WF 3rd, Kang JD. Six-degrees-of-freedom cervical spine range of motion during dynamic exion-extension aer single-level anterior arthrodesis: comparison with asymptomatic control subjects. J Bone Joint Surg Am. 2013;95(6):497-506.
80. Li G, Wang S, Passias P, et al. Segmental in vivo vertebral motion during functional human lumbar spine activities. Eur Spine J. 2009;18(7):1013-1021.
81. Passias PG, Wang S, Kozanek M, et al. Segmental lumbar rotation in patients with discogenic low back pain during functional weight-bearing activities. J Bone Joint Surg Am. 2011;93(1):29-37.
82. Adams MA, Dolan P. Recent advances in lumbar spinal mechanics and their clinical signicance. Clin Biomech (Bristol, Avon). 1995;10(1):3-19.
83. Anderst W. Narrative review of the in vivo mechanics of the cervical spine aer anterior arthrodesis as revealed by dynamic biplane radiography. J Orthop Res. 2016;34(1): 22-30.
84. Panjabi M, Chang D, Dvorák J. An analysis of errors in kinematic parameters associated with in vivo functional radiographs. Spine. 1992;17(2):200-205.
85. Inoue N, Espinoza Orías AA. Biomechanics of intervertebral disk degeneration. Orthop Clin North Am. 2011;42(4): 487-499.
86. Volkheimer D, Malakoutian M, Oxland TR, Wilke HJ. Limitations of current in vitro test protocols for investigation of instrumented adjacent segment biomechanics: critical analysis of the literature. Eur Spine J. 2015;24(9): 1882-1892.
87. Malakoutian M, Volkheimer D, Street J, et al. Do in vivo kinematic studies provide insight into adjacent segment degeneration? A qualitative systematic literature review. Eur Spine J. 2015;24(9):1865-1881.
88. Nachemson A, Morris JM. In vivo measurements of intradiscal pressure discometry, a method for the determination of pressure in the lower lumbar discs. J Bone Joint Surg Am. 1964;46:1077-1092.
89. Nachemson A. e load on lumbar disks in dierent positions of the body. Clin Orthop Relat Res. 1966;45:107-122.
Chapter 6 Biomechanics of the Spinal Motion Segment 117
90. Wilke HJ, Neef P, Caimi M, Hoogland T, Claes LE. New in vivo measurements of pressures in the intervertebral disc in daily life. Spine. 1999;24(8):755-762.
91. Sato K, Kikuchi S, Yonezawa T. In vivo intradiscal pressure measurement in healthy individuals and in patients with ongoing back problems. Spine. 1999;24(23):2468-2474.
92. Rohlmann A, Pohl D, Bender A, et al. Activities of everyday life with high spinal loads. PLoS One. 2014;9(5).
93. Rohlmann A, Dreischarf M, Zander T, Graichen F, Bergmann G. Loads on a vertebral body replacement during locomotion measured in vivo. Gait Posture. 2014;39(2):750-755.
94. Tawhai M, Bischo J, Einstein D, et al. Multiscale modeling in computational biomechanics. IEEE Eng Med Biol Mag. 2009;28(3):41-49.
95. Erdemir A, Bennetts C, Davis S, Reddy A, Sibole S. Multiscale cartilage biomechanics: technical challenges in realizing a high-throughput modelling and simulation workow. Interface Focus. 2015;5(2).
96. Freutel M, Schmidt H, Dürselen L, Ignatius A, Galbusera F. Finite element modeling of so tissues: material models, tissue interaction and challenges. Clin Biomech (Bristol, Avon). 2014;29(4):363-372.
97. Fagan MJ, Julian S, Mohsen AM. Finite element analysis in spine research. Proc Inst Mech Eng H. 2002;216(5):281-298.
98. Schmidt H, Heuer F, Drumm J, et al. Application of a calibration method provides more realistic results for a nite element model of a lumbar spinal segment. Clin Biomech (Bristol, Avon). 2007;22(4):377-384.
99. Schmidt H, Heuer F, Wilke HJ. Which axial and bending stinesses of posterior implants are required to design a exible lumbar stabilization system? J Biomech. 2009;42(1):48-54.
100. Rohlmann A, Mann A, Zander T, Bergmann G. Eect of an articial disc on lumbar spine biomechanics: a probabilistic nite element study. Eur Spine J. 2009;18(1):89-97.
101. Adams MA, Freeman BJ, Morrison HP, Nelson IW, Dolan P. Mechanical initiation of intervertebral disc degeneration. Spine. 2000;25(13):1625-1636.
102. Adams MA. Basic science of spinal degeneration. Surgery (Oxford). 2012;30(7):347-350.
103. Aubin CE, Petit Y, Stokes IA, et al. Biomechanical modeling of posterior instrumentation of the scoliotic spine. Comput Methods Biomech Biomed Engin. 2003;6(1):27-32.
104. Faizan A, Goel VK, Garn SR, et al. Do design variations in
the articial disc inuence cervical spine biomechanics? A nite element investigation. Eur Spine J. 2012;21 (suppl 5):S653-S662.
105. Knapik GG, Mendel E, Marras WS. Use of a personalized hybrid biomechanical model to assess change in lumbar spine function with a TDR compared to an intact spine. Eur Spine J. 2012;21(suppl 5):S641-S652.
106. Bell GH, Dunbar O, Beck JS, et al. Variations in strength of vertebrae with age and their relation to osteoporosis. Calcif Tissue Res. 1967;1:75-86.
107. Messerer O. Uber Elasticitat and Festigkeit der Meuschlichen Knochen. Stutgart: J.G. Cottaschen Buch-handling; 1880.
108. Perry O. Encyclopedia of Medical Radiology. New York: Springer Verlag; 1974.
109. Perry O. Fracture of the vertebral end-plate in the lumbar spine. Acta Orthop Scand. 1957;25(suppl).
110. Begeman PC, Visarius H, et al. Viscoelastic shear responses of the cadaver and hybrid III lumbar response. Presented at the 38th Stapp Car Crash Conference, Ft. Lauderdale, FL; 1994.
111. Frei H, Oxland TR, Nolte LP. oracolumbar spine mechanics contrasted under compression and shear loading. J Orthop Res. 2002;20:1333-1338.
112. Bisschop A, Mullender MD, Kingma I, et al. e impact of bone mineral density and disc degeneration on shear strength and stiness of the lumbar spine following laminectomy. Eur Spine J. 2012;21:530-536.
SECTION
I
This page intentionally left blank
Nerve Root Pain in Disc Herniation and
SECTION
7
CHAPTER
e clinical symptoms associated with lumbar disc herniation and spinal stenosis are attributed to pathophysiologic changes in spinal nerve roots. Recent research has dened the basic
pathophysiologic events at the tissue, cellular, or subcellular levels in relationship to the pathogenesis of sciatica and nerve root pain. is chapter reviews the current knowledge about
these mechanisms and discusses these mechanisms in relation to the clinical features of lumbar disc herniation and spinal stenosis.
Nerve root pain is typically radiating in nature and usually
related to a specic nerve root or adjacent roots. It is associ-
ated with pathologic changes and nerve dysfunction and may be present in motor and sensory modalities, producing motor weakness and sensory disturbances. ese changes are tightly
linked through mechanisms that are discussed in this chapter.
Two specic mechanisms at the “tissue level” may be
dened: (1) mechanical deformation of the nerve roots and (2) biologic or biochemical activity of the disc tissue causing neuroinammation of nerve roots.
Mechanical Eects on Nerve Roots
Enclosed by the vertebral bones, the spinal nerve roots are relatively well protected from external trauma, although somewhat more susceptible to injury than peripheral nerves. In 1934, Mixter and Barr1 described that intervertebral discs can rupture and cause mechanical compression of the nerve roots, leading to sciatica. However, there has been moderate research interest in the past regarding nerve root compression. Gelfan and Tarlov2 in 1956 and Sharpless3 in 1975 performed some initial experiments on the eects of compression on nerve impulse conduction and showed that nerve roots were more susceptible to compression than peripheral nerves. Interest in nerve root pathophysiology has increased more recently, and numerous studies are reviewed here.
In 1991, a model was presented that allowed for experi­mental, graded compression of cauda equina nerve roots at known pressure levels.4 In this model, the cauda equina of pigs
Spinal Stenosis
Robert R. Myers
Björn Rydevik
Kjell Olmarker
Shinichi Kikuchi
was compressed by an inatable balloon xed to the spine (Fig. 7.1). e cauda equina could also be observed through the translucent balloon. is model made it possible to study the ow in the intrinsic nerve root blood vessels at various pressure levels.5 e average occlusion pressure for the arteri­oles was found to be slightly below and directly related to the systolic blood pressure. e blood ow in the capillary net­works was intimately dependent on the blood ow of the adjacent venules. is nding corroborates the assumption that venular stasis may induce capillary stasis and changes in the microcirculation of the nerve tissue, which has been sug­gested as one mechanism in carpal tunnel syndrome.6 e mean occlusion pressures for the venules showed large varia­tions; however, a pressure of 5 to 10 mm Hg was found to be sucient for inducing venular occlusion.
Because the nutrition of the nerve root is aected by ischemia, a compression-induced impairment of the vascu­lature may be one mechanism for nerve root dysfunction. e nerve roots also have a considerable nutritional supply via diusion from the cerebrospinal uid.7 To assess the compression-induced eects on the total contribution to the nerve roots, an experiment was performed in which
3
H-labeled methylglucose was allowed to be transported to the nerve tissue in the compressed segment via the blood vessels and via the cerebrospinal uid diusion aer systemic injec-
tion.8 e results showed that no compensatory mechanism from cerebrospinal uid diusion could be expected at low
pressure levels. On the contrary, 10 mm Hg compression was sucient to induce a 20% to 30% reduction of the transport
of methylglucose to the nerve roots.
It is known from experimental studies on peripheral nerves that compression may also induce an increase in vascular permeability, leading to intraneural edema formation.9 Such edema may increase the endoneurial uid pressure, which impairs the endoneurial capillary blood ow and nutrition of the nerve roots.10 Because the edema usually persists for some time aer the removal of a compressive agent, edema may negatively aect the nerve root for a longer period than the
compression itself. e presence of intraneural edema is also
I
119
120 BASIC SCIENCE
C
D
B
A
FIG. 7.1 Schematic of an experimental nerve root compression model.
Cauda equina (A) is compressed by an inatable balloon (B) that is xed to the spine by two L-shaped pins (C) and Plexiglas plate (D). (From Olmarker K, Holm S, Rosenqvist A-L, et al. Experimental nerve root compression: a model of acute, graded compression of the porcine cauda equina and an analysis of neural and vascular anatomy. Spine [Phila Pa 1976]. 1991;16:61-69.)
related to subsequent formation of intraneural brosis,11 a neuroinammatory response that is seen in some patients
with nerve compression disorders.
Nerve root compression directly aects nerve conduc-
12,13
tion. more susceptible to compression than the motor bers.
Our data show that the sensory bers are slightly
13,14
One factor that has not been fully recognized in compres­sion trauma of nerve tissue is the onset rate of the compression. e onset rate (i.e., the time from compression start until full compression) may vary clinically from fractions of seconds in traumatic conditions to months or years in association with degenerative processes.
A rapid-onset rate of less than 1 second has been found to induce more pronounced pathophysiologic dysfunction. For the rapid-onset compression, which is likely to be more closely related to spine trauma or disc herniation than to spinal steno­sis, it has been seen that a pressure of 600 mm Hg maintained only for 1 second is sucient to induce a gradual impairment
of nerve conduction during the 2 hours studied aer the compression was ended.15 In the case of spinal stenosis, the rate may be a great deal slower, and pain or nerve dysfunction may not be seen until aer considerable ischemic injury.
Chronic Experimental Nerve Root Compression
To mimic various clinical situations, compression must be applied for long periods. In clinical syndromes with nerve root compression, the onset time may be quite slow and the dura­tion may be quite long. A gradual development of degenerative changes that induce spinal stenosis leads to an onset time that can be many years. It is dicult to mimic such a situation in an experimental model. Chronic models should induce a controlled compression with a slow-onset time that is easily reproducible.
Delamarter and colleagues16 introduced a model on the dog cauda equina in which they applied a constricting plastic band that was le in place for various times. e band was tightened around the thecal sac to induce a 25%, 50%, or 75% reduction of the cross-sectional area. e data indicated that structural and functional changes were proportional to the degree of constriction.
To induce a slower onset and more controlled compression, Corneord and colleagues17 used a constrictor to compress the nerve roots in the pig. e constrictor consisted of an outer metal shell that on the inside was covered with a mate­rial called ameroid that expands when in contact with uids. Because of the metal shell, the ameroid expands inward with a maximum of expansion aer 2 weeks, resulting in a compres­sion of a nerve root placed in the central opening of the constrictor. Compression of the rst sacral nerve root in the pig resulted in a signicant reduction of nerve conduction velocity and axonal injuries.17 It has also been found that there is an increase in substance P in the nerve root and the dorsal root ganglion aer such compression.18 Substance P is a neurotransmitter that is related to pain transmission.
One important aspect in clinical nerve root compression conditions is that the compression level is probably unstable and varies as the result of changes in posture and move-
19,20
ments.
In 1995, Konno and colleagues21 introduced a model in which the pressure could be changed aer some time of initial chronic compression. An inatable balloon was introduced under the lamina of the seventh lumbar vertebra in the dog. By inating the balloon at a known pressure slowly over 1 hour with a viscous substance that would harden in the balloon, compression of the cauda equina could be induced with a known initial pressure level. e compression was veri­ed by myelography. Because the balloon under the lamina was composed of a twin set of balloons, the second balloon component could be connected to a compressed air device and could be used to add compression to the already chronically compressed cauda equina.
Acute nerve root compression experiments have established critical pressure levels for interference with various physiologic parameters in the spinal nerve roots. Studies on chronic compression may provide knowledge that would be more applicable to the clinical situation.
Spinal Stenosis: Experimental-Clinical Correlation
Patients with double or multiple levels of spinal stenosis may have more pronounced symptoms than patients with stenosis only at one level.22 e mechanism for the dierence between
single and double compression may not simply be based on the fact that the nerve impulses have to pass more than one compression zone at double-level compression. ere may also be a mechanism based on the local vascular anatomy of the nerve roots. In contrast to peripheral nerves, there are no regional nutritive arteries from surrounding structures to the intraneural vascular system in spinal nerve roots. pression at two levels might induce a nutritionally impaired region between the two compression sites. In this way the segment aected by the compression would be widened. Data
23–25
Com-
Chapter 7 Nerve Root Pain in Disc Herniation and Spinal Stenosis 121
from a study on the nutritional transport to the nerve tissue in double-level compression showed that there is a reduction of this transport to the uncompressed nerve segment located between the two compression balloons that was similar to the reduction within the two compression sites.26 us, there is experimental evidence that the nutrition to the nerve segment located between two compression sites in nerve roots is severely impaired, although this nerve segment itself is uncompressed.
If nerve compression is of an extremely low onset rate, as in spinal stenosis, there may be an adaptation of the nerve tissue to the applied pressure. In cadaveric experiments, Schönström and colleagues27 found that when a hose clamp was tightened around a human cadaveric cauda equina speci­men there was a critical cross-sectional area of the dural sac when the rst signs of pressure increase among nerve roots were recorded by a catheter placed in the compression zone. is cross-sectional area was approximately 75 mm2, which was also found to correlate with a corresponding measure­ment on computed tomography (CT) in patients with spinal stenosis.28 When the hose clamp was tightened further, the pressure increased. Owing to creep phenomena in the nerve tissue, the pressure decreased with time, however. When the pressure did not normalize within 10 minutes, the “sustained size” was registered and was found to be in the range of 45 to 50 mm2.27 is study indicates that even in acute compression there is an adaptation of the nerve tissue to the applied pres­sure. From a longer perspective, this probably means that the nerve may also be reorganized in its microstructural elements, which would result in a nerve with a smaller diameter. Under such circumstances, with gradually decreasing nerve diameter, the pressure acting on the nerve would be reduced to some degree.
ere is a correlation between the experimental animal observations regarding critical pressures for functional and nutritional changes in nerve roots under compression and the measurements of pressure levels among nerve roots in human cadaveric lumbar spines aer experimental constriction of the
dural sac.
Epidural pressure measurements have been performed, evaluating the relationship between epidural pressure and posture.20 It was found that the local epidural pressure at the stenotic level was low in lying and sitting postures and high in standing postures. Pressure was increased with extension but decreased with exion of the spine. e highest epidural
pressure, 117 mm Hg, was found in standing with extension. Measurements have also been reported regarding changes in epidural pressure during walking in patients with lumbar spinal stenosis.29 e pressure changed during walking with a wave pattern of increasing and decreasing changes. Such observations correlate with the previously mentioned experi­mental observations regarding intermittent cauda equina compression.
19
pain. Howe and colleagues30 found that mechanical stimulation of nerve roots or peripheral nerves resulted in nerve impulses of short duration and that these impulses were prolonged if the nerve tissue had been exposed to mechanical irritation by a chromic gut ligature for 2 to 4 weeks. Corresponding results were obtained in an in vitro system using rabbit nerve roots.31 In this setup, it was also evident that the dorsal root ganglion was more susceptible to mechanical stimulation than the nerve roots. e dorsal root ganglion has elicited special interest in this regard, and an increase in the level of neurotransmitters related to pain transmission has been found in the dorsal root ganglion in response to whole-body vibration of rabbits.32 A similar increase has been seen in the dorsal root ganglion and nerve root aer local constriction of the same nerve root.18
In vivo models of pain behavior have shown that mechanical nerve deformation superimposed on inammation is painful,
whereas either factor alone might not cause severe pain. e magnitude of nerve root compression pressure (measured intraoperatively) correlates with neurologic decit but not with degree of straight-leg raising test.
31–34
Neuropathologic Changes and Pain
ere is considerable research evidence regarding the relation­ship of pain to neuropathologic changes.35 Much of what is known has been studied in relationship to mechanical and inammatory injury of the sciatic nerve in the rat. Entrapment of a peripheral nerve produces pathologic change in propor­tion to the degree of compression and its duration,36 as is known to be the case for nerve root compression. In an elec­tron microscopic study,36 minor degrees of nerve compression were associated with ischemic injury to Schwann cells, result­ing in their necrosis and in demyelination. Severe nerve compression was associated with injury to the axon, resulting in wallerian degeneration.
Subsequent experiments established the relationship of pain to these forms of neuropathologic change.37 ese studies established that mild levels of ischemia producing demyelin­ation were generally not painful, whereas severe ischemia­producing wallerian degeneration resulted in hyperalgesia. e pathology of the chronic constriction injury model of neuropathic pain is based on this relationship and the added insult of inammation caused by the chromic gut ligatures used to compress the nerve.38 It is now recognized that the cytokine-driven processes of wallerian degeneration are the dominant neuropathologic factors linking nerve injury and
37,39,40
pain eration relate directly to the magnitude and duration of hyperalgesia.
and that the degree and extent of wallerian degen-
41
Biologic and Biochemical Eects on Nerve Roots
SECTION
I
Mechanical Nerve Root Deformation and Pain
Some experimental observations indicate that mechanical nerve root deformation per se may induce impulses that cause
e clinical picture of sciatica with a characteristic distribu­tion of pain and nerve dysfunction in the absence of herniated disc material at radiologic examination and at surgery has indicated that mechanical nerve root compression may not be
122 BASIC SCIENCE
the only factor that is responsible for sciatic pain. In 1984 it was suggested that the disc tissue per se may have some injuri­ous properties.42 It was later conrmed experimentally that local epidural application of autologous nucleus pulposus in the absence of mechanical deformation induces signicant changes in structure and function of the adjacent nerve roots.
43
Biologic Eects of Nucleus Pulposus
In 1993, Olmarker and colleagues43 published a study that showed that autologous nucleus pulposus can induce a reduc­tion in nerve conduction velocity and light microscopic structural changes in a pig cauda equina model of nerve root injury. ese axonal changes had a focal distribution, however, and the quantity of injured axons was too low to be responsible for the signicant neurophysiologic dysfunction observed. A follow-up study of areas of the nerve roots exposed to nucleus pulposus that appeared to be normal by light microscopy revealed that there were signicant injuries of Schwann cells with vacuolization and disintegration of Schmidt-Lanterman incisures (Fig. 7.2).44 Schmidt-Lanterman incisures are essen­tial for the normal exchange of ions between the axon and the surrounding tissues. An injury to this structure would be likely to interfere with the normal impulse conduction proper­ties of the axons, although these models’ changes may not fully explain the neurophysiologic dysfunction observed.
M
M
A
S
e pathophysiologic potential of the nucleus pulposus was emphasized further in an experiment using a dog model in which it was seen that a surgical incision of the anulus brosus,
with minimal leakage of nucleus pulposus, was enough to induce signicant changes in structure and function of the adjacent nerve root.45 It has also been seen that epidural application of the autologous nucleus pulposus within 2 hours induces an intraneural edema
46,47
that leads to a reduction of
the intraneural blood ow.47 Histologic changes of the nerve
roots are present aer 3 hours,48 and a subsequent reduction of the nerve conduction velocity starts 3 to 24 hours aer application.
43,48
e nucleus pulposus may also interfere with the nutrition to the intraspinal nerve tissue. Aer application to the dorsal root ganglion, it was found that the intraneural blood ow was dramatically decreased and that there was a
simultaneous increase of the tissue uid pressure.
47
Methylprednisolone reduces the pathophysiologic events of the nucleus pulposus–induced nerve root injury if given within 24 hours. To establish if the presence of autologous nucleus pulposus could initiate a leukotactic response from the surrounding tissues, a study was initiated that assessed the potential inammatogenic properties of the nucleus pulposus.49 Autologous nucleus pulposus and autologous retroperitoneal fat were placed in separate perforated titanium chambers and placed subcutaneously, together with a sham chamber, in the pig. e number of leukocytes was assessed 7 days later for the chambers. e nucleus pulposus–containing chambers had a number of leukocytes that exceeded the two others by 150%. In another experiment, autologous nucleus pulposus and muscle were placed in Gore-Tex tubes subcuta­neously in rabbits.50 Aer 2 weeks, there was an accumulation
of macrophages and T-helper and T-suppresser cells in the tube with nucleus pulposus that persisted the full observation time of 4 weeks.
Kawakami and colleagues51 showed that neuropathic pain in an experimental setting seems to be mediated by inltrating
leukocytes, a nding consistent with the previous observa­tions of neuroimmunologic inammatory changes and pain.52
In rats made leukopenic by using nitrogen mustard, the pain response was absent aer application of nucleus pulposus,
whereas normal rats with nucleus pulposus application dis­played a pathologic response to stimulation. e same group also showed that inhibition of cyclooxygenase-2 might reduce nucleus pulposus–induced pain behavior.53 Taken together, these data further support the impression that autologous nucleus pulposus may elicit inammatory reactions when
outside the intervertebral disc space and that such reactions may not be restricted to resorption of the herniated tissue but also may be intimately involved in the pathophysiology of sciatica.
FIG. 7.2 Seven days after application of nucleus pulposus. Myelinated
nerve ber with prominent vesicular swelling of Schmidt-Lanterman incisure. Note mononuclear cell (red M) in close contact with nerve ber. Arrowheads indicate myelin sheath layers outside Schmidt-Lanterman incisure. A, well-preserved axon; white M, myelin sheath; S, outer Schwann cell cytoplasm. (Bar = 2.5 µm.) (From Olmarker K, Nordborg C, Larsson K, et al. Ultrastructural changes in spinal nerve roots induced by autologous nucleus pulposus. Spine [Phila Pa 1976]. 1996;21:411-414.)
Nucleus Pulposus and Sciatic Pain
Pain is much more dicult to assess than nerve conduction in controlled experimental studies. e available literature indicates that pain may be induced by both mechanical factors and nucleus pulposus–mediated factors. e role of the nucleus pulposus in this context is interesting in view of