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Chapter 10 Outcomes Research for Spinal Disorders 163
An interesting feature of case-control studies includes their ability to be “nested” within a dened cohort. is is referred to as a nested case-control or nested case-cohort design. Here, the cohort has typically been assembled for another purpose and, as such, has previously stored images, specimens, and other data, or has been assembled de novo to answer the research question. e investigator would typically measure the outcome variable in this cohort to distinguish cases from controls, and then measure the predictor variables in the banked specimens and images. is allows for comparison of risk factors in the cases and controls. e main advantage of this subtype of case-control study design is that it is especially useful for minimizing costly measurements on serum and other specimens (since these will only have to be conducted on all the cases and a sample of the controls, instead of the entire cohort). Additionally, this design also preserves the advantages of cohort studies that result from collecting predic­tor variables prior to the occurrence of the outcome.
Although case-control studies have rarely been used in the spine literature, a hypothetical example would be the compari­son of the rate of exposure to nonsteroidal antiinammatory
drugs (NSAIDs) between patients with a lumbar pseudarthro­sis (the cases) and patients with a successful fusion (controls). is approach might prove useful in evaluating the hypothesis that NSAID use might aect the likelihood of successful
fusion. Sampling bias (e.g., dierential rates of smoking, dia­betes, and other risk factors for nonunion between the cases and controls) and recall bias (patients with pseudarthroses might be more likely to report exposure to NSAIDs) would have to be taken into account.

Case Series

Case series are reports of outcomes for patients undergoing a treatment without any control group. e spine literature is
replete with this type of study. No inferential conclusions can be made from case series because there is no control group with which to compare outcomes. Case series should be based on a consecutive series of patients to avoid selection bias in which the investigator includes only patients with desirable outcomes. ese studies are useful for hypothesis generating or reporting outcomes on rare conditions. ey should not be used to develop treatment guidelines because they lack a control group and do not allow for the assessment of eective-
ness of a treatment.

Levels of Evidence

Investigators have created a hierarchy of study designs based on the quality of causal inference that one can make with each study design (Fig. 10.7). Well-controlled RCTs and meta-analyses of such studies are at the pinnacle of the hierarchy. ese studies have been labeled level I evidence.59
Observational cohort studies or RCTs with methodologic shortcomings are level II evidence. Case-control studies are considered level III evidence. Descriptive studies such as case
Meta-
analysis
RCT
Cohort study
Case-control study
Case series/case
Expert opinion
FIG. 10.7 Hierarchy of research designs in evidence-based medicine.
series and case reports are level IV evidence. Expert opinion is considered level V evidence. As shown by the SPORT IDH RCT, all questions are not best answered with a randomized design. In addition, when modern observational studies are compared with RCTs, it has been shown that they do not usually overstate the treatment eect of an intervention.
Whereas the hierarchy of evidence is useful for comparing study designs in general, the merits of each individual study should be assessed, and high-quality, observational studies should not be discounted.
57,60
Cost-Eectiveness Analysis
Given the ever-increasing costs of health care, policymakers have recommended that medical interventions be evaluated for their cost-eectiveness.61 Cost-eectiveness analysis aims to determine the cost to society for the incremental health benet derived from an intervention that is more costly than
an alternative, less eective treatment. Although an RCT can show the ecacy of a treatment, further economic analysis can be performed alongside the RCT to evaluate how much society must pay for the treatment eect. To compare the cost­eectiveness of a wide variety of treatments across many medical specialties, a universal scale of health must be used to measure preference for health outcomes. In cost-eectiveness analysis, the quality-adjusted life-year (QALY), which com- bines length and quality of life in a single number, is the rec­ommended measure of health benet.
To estimate QALYs, a utility, which is a numeric preference rating of health ranging from 0 (equivalent to death) to 1 (perfect health) is used to value the health states associated with a treatment. Classically, utilities have been derived using techniques such as the time trade-o, which essentially deter­mines how much time in a state of suboptimal health people would be willing to trade for a lesser amount of time in perfect health.61 More recently, techniques have been developed to determine utilities based on standard questionnaires such as the SF-36.62 QALYs are determined by multiplying utility for each health state by the length of time in each health state and summing up over time. For example, 2 years spent in a poor health state with a utility of 0.5 followed by 10 years in a good
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health state with a utility of 0.8 would be equivalent to 9 QALYs (2 × 0.5 + 10 × 0.8). To compare the benets of various interventions, cost-eectiveness analysis determines the gain in QALYs associated with an intervention. e advantage of QALYs is that they allow for the comparison of very dierent health states across medical disciplines.
e other half of the cost-eectiveness equation is cost. Although an intervention typically produces a health benet, that benet comes at a cost to society. Determining the cost of an intervention is challenging; thus, many cost-eectiveness analyses use gross costing based on average reimbursements for various procedures. Aer determining the costs and ben- ets associated with an intervention, these must be compared with another treatment. is is done by determining the incre- mental cost-eectiveness ratio (ICER). e ICER is dened as the dierence in cost between two treatments divided by the dierence in utility. Tosteson and colleagues63 reported that discectomy resulted in a gain of 0.21 QALYs compared with nonoperative treatment at an additional cost of $14,137, which yielded an ICER of $67,319/QALY ($14,137/0.21 QALY). Traditionally, an ICER of $50,000/QALY has been used as a cost-eectiveness threshold because this was the ICER for hemodialysis, an intervention for which society has decided to pay.64 More recently, some authors have suggested that $100,000/QALY is a more realistic cost-eectiveness threshold because many frequently used interventions fall in the $50,000 to $100,000/QALY range.
63,65,66
eoretically, cost-eectiveness analysis should allow societies to maximize the value of their health care expendi­tures; the United Kingdom has set ICER thresholds to deter­mine which services should be provided by their National Health Service.67 ere is little evidence, however, that health care systems, including systems that currently ration care, have been consistently using cost-eectiveness analysis to guide rational treatment guidelines.68 As health care spending comes under greater scrutiny and decisions regarding which treatments to provide are made, evaluating the cost­eectiveness of an intervention will be essential.
Future of Outcomes Research: Patient-Specic Recommendations
Since the prior edition of this textbook, the quality of spine outcomes research has improved markedly alongside a more sophisticated understanding of the issues surrounding out­comes research within the spine community. A study of spine-related clinical trials published in 2007 reported that 60% were performed and reported in an acceptable fashion, a result that is better than seen in a general orthopaedic journal.69 Although this percentage is likely an improvement from years prior, there is further work to be done on the quality of the spine literature. e 4-year and 8-year outcome data from the SPORT IDH study, the largest scale outcomes research study ever performed in the eld of spinal disorders, have been published more recently. scale trials are able to determine the treatment eect of an intervention for the “average” patient, it can be dicult to
70,71
Although this and most large-
apply the results to clinical practice, in which no patient is “average.”
In the case of IDH, there are clearly patients who fail surgi­cal treatment and others who are very successful with nonop­erative treatment. Blind application of the results of SPORT to all patients who met the inclusion criteria (symptoms lasting at least 6 weeks, the presence of neurologic ndings, and
imaging consistent with their symptoms) would result in surgery for all such patients. Although this approach would result in greater clinical improvement than nonoperative treatment, on average, surgery would be performed on some patients who would have improved to an acceptable, and even to a greater, degree with nonoperative treatment. Other patients would fail to improve with surgery and perhaps experience an additional decrease in their quality of life.
To avoid unnecessary surgery on these two groups of patients, models that take individual characteristics and values into account when predicting outcomes are needed. When suciently powerful models are developed, individual base­line characteristics, physical ndings, and results from imaging studies can be entered into such models to determine the likelihood of success with surgery or nonoperative treatment. Individual patient values should also be considered in dening success and assigning utilities to the various possible out­comes. Such an approach represents the true integration of evidence-based medicine with shared decision making at the level of the individual patient and should be the next step in spine outcomes research.

KEY POINTS

1. With constantly increasing health care costs, policymakers are
demanding outcomes research to show the eectiveness of
treatments, especially in elds that require expensive
technology, such as spine surgery.
2.
There is substantial geographic variation in the rates of spine
surgery across the United States, indicating that further research
is needed to determine which patients are served best with
surgery.
3.
Chance, bias, and confounding all threaten the validity of
conclusions based on clinical research and need to be
addressed in study design and data analysis.
4.
RCTs can yield the highest level of evidence, although many
surgical questions are not amenable to this type of study
design. In these cases, well-designed observational studies may
be more appropriate.
5.
Cost-eectiveness analysis will become more important as
decisions need to be made about the use of scarce health care
resources.

KEY REFERENCES

1. Fisher ES, Wennberg DE, Stukel TA, et al. The implications of
regional variations in Medicare spending. Part 2: health
outcomes and satisfaction with care. Ann Intern Med.
2003;138:288-298.
This study showed wide variation in Medicare spending across
hospital referral regions with no measurable improvement in
outcomes in areas with the highest levels of spending.
2.
Weinstein JN, Lurie JD, Olson PR, et al. United States’ trends and
regional variations in lumbar spine surgery: 1992-2003. Spine.
2006;31:2707-2714.
Chapter 10 Outcomes Research for Spinal Disorders 165
This small area analysis showed the increase in the rate of lumbar fusion in the Medicare population throughout the 1990s and the wide geographic variation in fusion rates in this population.
3.
Bombardier C. Outcome assessments in the evaluation of
treatment of spinal disorders. Introduction. Spine. 2000;25:3097-3099.
This article reviews the dierences between dierent outcome measures used in the spine literature and introduces an issue dedicated to this topic.
4.
Kocher MS, Zurakowski D. Clinical epidemiology and
biostatistics: a primer for orthopaedic surgeons. J Bone Joint Surg
Am. 2004;86:607-620. This is a good review of basic epidemiology and biostatistics as they apply to orthopedics.
5.
Benson K, Hartz AJ. A comparison of observational studies and
randomized, controlled trials. N Engl J Med. 2000;342:1878-1886.
This article convincingly shows that well-designed observational trials yield similar results to randomized controlled trials.

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30. Atlas SJ, Deyo RA, Patrick DL, et al. e Quebec Task Force Classication for Spinal Disorders and the severity, treatment, and outcomes of sciatica and lumbar spinal stenosis. Spine. 1996;21:2885-2892.
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35. Wainer H, Dorans NJ, Flaugher R, Green BF, Mislevy RJ. Computerized Adaptive Testing: A Primer. Abingdon-on­ames, UK: Routledge; 2000.
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37. Rothrock NE, Hays RD, Spritzer K, et al. Relative to the general US population, chronic diseases are associated with poorer health-related quality of life as measured by the Patient-Reported Outcomes Measurement Information System (PROMIS). J Clin Epidemiol. 2010;63(11): 1195-1204.
38. Hung M, Hon SD, Franklin JD, et al. Psychometric properties of the PROMIS physical function item bank in patients with spinal disorders. Spine. 2014;39(2):158-163.
39. Rose M, Bjorner JB, Becker J, Fries J, Ware J. Evaluation of a preliminary physical function item bank supported the expected advantages of the Patient-Reported Outcomes Measurement Information System (PROMIS). J Clin Epidemiol. 2008;61(1):17-33.
40. Garcia SF, Cella D, Clauser SB, et al. Standardizing patient-reported outcomes assessment in cancer clinical trials: a patient-reported outcomes measurement information system initiative. J Clin Oncol. 2007;25(32):5106-5112.
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response theory to improve assessment of patient-reported outcomes. Clin Exp Rheumatol. 2005;23(5):S53.
43. Roland M, Fairbank J. e Roland-Morris Disability Questionnaire and the Oswestry Disability Questionnaire. Spine. 2000;25:3115-3124.
44. Weinstein JN, Tosteson TD, Lurie JD, et al. Surgical vs nonoperative treatment for lumbar disk herniation. e Spine Patient Outcomes Research Trial (SPORT): a randomized trial. JAMA. 2006;296:2441-2450.
45. Roland M, Morris R. A study of the natural history of low-back pain. Part II: development of guidelines for trials of treatment in primary care. Spine. 1983;8:145-150.
46. Kopec JA. Measuring functional outcomes in persons with back pain: a review of back-specic questionnaires. Spine.
2000;25:3110-3114.
47. Fritzell P, Hagg O, Wessberg P, et al. 2001 Volvo Award Winner in Clinical Studies. Lumbar fusion versus nonsurgical treatment for chronic low back pain: a multicenter randomized controlled trial from the Swedish Lumbar Spine Study Group. Spine. 2001;26:2521-2534.
48. Brox JI, Sorensen R, Friis A, et al. Randomized clinical trial of lumbar instrumented fusion and cognitive intervention and exercises in patients with chronic low back pain and disc degeneration. Spine. 2003;28:1913-1921.
49. Hulley SB, Newman TB, Cummings SR. Choosing the study subjects: specication, sampling, and recruitment. In: Designing Clinical Research. 2nd ed. Philadelphia: Lippincott Williams & Wilkins; 2001:25-35.
50. Spratt K. Statistical relevance. In: Garn S, Abitbolet J, eds. Orthopaedic Knowledge Update: Spine. Rosemont, IL: American Academy of Orthopaedic Surgeons; 2002:497-505.
51. Kocher MS, Zurakowski D. Clinical epidemiology and biostatistics: a primer for orthopaedic surgeons. J Bone Joint Surg Am. 2004;86:607-620.
52. Birkmeyer NJ, Weinstein JN, Tosteson AN, et al. Design of the Spine Patient Outcomes Research Trial (SPORT). Spine. 2002;27:1361-1372.
53. Newman TB, Browner WS, Hulley SB. Enhancing causal inference in observational studies. In: Designing Clinical
Research. 2nd ed. Philadelphia: Lippincott Williams & Wilkins; 2001:125-137.
54. Dawson B, Trapp RG. Basic and Clinical Biostatistics. 4th ed. New York: McGraw-Hill; 2004.
55. Flum DR. Interpreting surgical trials with subjective
outcomes: avoiding UnSPORTsmanlike conduct. JAMA. 2006;296:2483-2485.
56. Weinstein JN, Lurie JD, Tosteson TD, et al. Surgical vs
nonoperative treatment for lumbar disk herniation: the Spine Patient Outcomes Research Trial (SPORT) observational cohort. JAMA. 2006;296:2451-2459.
57. Benson K, Hartz AJ. A comparison of observational
studies and randomized, controlled trials. N Engl J Med. 2000;342:1878-1886.
58. Newman TB, Browner WS, Cummings SR, et al. Designing an
observational study: cross-sectional and case-control studies. In: Designing Clinical Research. 2nd ed. Philadelphia: Lippincott Williams & Wilkins; 2001:107-123.
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evidence: from case reports to randomized controlled trials. Clin Orthop Relat Res. 2003;413:19-24.
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observational studies, and the hierarchy of research designs. N Engl J Med. 2000;342:1887-1892.
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CHAPTER

Introduction

Computational and numeric methods have been used to assess the biomechanical behaviors of biologic systems. e
advent and continuous development of powerful computing systems in addition to improvement of the emerging compu­tational packages in computer-aided engineering (CAE) with enhanced modeling features have enabled scientists to develop more rigorous models of biologic systems to predict the behavior of these systems under dierent biologic conditions.
In orthopaedic biomechanics, the latest advances in medical imaging technologies have helped researchers obtain a better resolution of geometric and anthropometric specications of
individual organs in the human body, including micro-scale computational models of the knee, hip, spine, and bone itself.
In addition to ethical considerations, the practical diculties, restrictions, and cost involved in experimental in vitro and in vivo studies highlight the utility of computational models as complementary tools for studies in orthopaedic biomechanics.
e future challenge will be how to apply these approaches to those areas of science that are not yet considered and how to further improve present generation models to better simu­late the couplings and nonlinearities that occur in physical incidents.
One of the most applicable approaches used in biome­chanical studies is nite element analysis (FEA), in which the object or system is represented by a geometrically similar model consisting of multiple linked representations of discrete regions. e basic idea for the nite element (FE) method originated from advances made in aircra structural analysis
in the 1940s. Since then, the FE method has become a power­ful tool for the numeric solution to a wide range of engineering problems. In this method of analysis, a complex region den-
ing a continuum is broken into simple geometric shapes called nite elements. Material properties and governing relation­ships are assigned to the elements. With the advances in computational power and computer-aided drawing (CAD)

Finite Element Analysis

Emily Walsh
M. Saeid Asadollahi
Raj Nangunoori
Jie Zheng
Daniel Cook
Boyle C. Cheng
Vijay K. Goel
systems, complex problems can now be solved with relative ease. Specialized FE method soware—such as Abaqus
(Simulia), ANSYS, COMSOL Multiphysics, and others— provides linear, nonlinear, static, and dynamic solutions to many industrial problems.
In general, FEA includes three main steps: preprocessing,
analysis, and postprocessing. Preprocessing is the rst step in
FEA, in which an FE model of the structure is created. Most FEA packages require a topological description of the struc­ture’s geometric features as input, which can be in one-, two-, or three-dimensional (3D) form, representing line, surface, or structural elements, respectively. However, 3D models are used in most cases. Design les, CAD models, and preexisting digital scans can be imported into an FEA environment to be utilized for an FEA. Once the FE geometric model is devel­oped, a meshing procedure is used to dene and divide the model into small discrete elements. An FE model is dened by creation of a mesh network, which includes the geometric arrangement of elements and nodes. When the FE model is created, the material properties are assigned to the individual parts, and proper interactions and constraints are dened between interacting part and surfaces. Finally, the boundary conditions and loads are assigned to the model.
e next step is analysis, which solves the model to converge for solutions within the predened boundary, load conditions, and constraints. To better simulate the physical conditions of the problem, dierent types of analysis, such as static or
dynamic (time-dependent) simulation, can be considered. In static simulation, the inputs and outputs are independent of time and the system is solved to balance the load and bound­ary conditions. In dynamic simulation, time can aect the input and output parameters and the behavior of the model varies over the time. Examples of dynamic simulations are dynamic loading, impact, and long-term creep (or wear).
Once the simulation is nished, postprocessing of the data
can be performed using visualization tools. e analysis outputs can be in the form of nodal outputs, including
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FIG. 11.1 Steps of creating the nite element (FE) model of spine. The computed tomographic images are
used to develop a grid at each transverse plane. The coordinates of the nodes are imported to the FE package, and the elements are created. The material properties are dened for individual elements; the loads, boundary conditions, and constraints are dened as the last step in modeling. The model is run and various FE outputs, such as stresses and nodal displacements, are calculated for sections of interest.
displacement at each node and element outputs, such as stresses and strains (Fig. 11.1).
Finite Element Modeling of the Spine
Low Back Pain
e human spine is a complex structure that supports the upper trunk weight and external loads applied to the human body. e spine column also protects the delicate spinal cord and provides adequate exibility and stiness to perform
various daily activities. e stability of the ligamentous spine is signicantly reduced in vivo due to absence of muscles.
Low back pain (LBP) is one of the common musculoskeletal
disorders that aects the functionality of the spine. While
there are many causes of back pain, the most prevalent causes are muscle strain, degenerative disc disease, spinal stenosis, disc herniation, facet hypertrophy, isthmic spondylolisthesis, degenerative spondylolisthesis, or (rarely) a spinal tumor.
In the United States, LBP is one of the major reasons for disability for people younger than 45 years. More than 80% of Americans suer from LBP at some point in life. According to an estimate, LBP costs between $100 and $200 billion annu­ally, two-thirds of which is a result of decreased wages and productivity.1 us, there is a need to study the origin of pain associated with the lumbar spine and search for simple, cost­eective, and safe treatment options. While there are a number of avenues that researchers are pursing in this direction, the role of mechanical factors in back disorders is signicant.
us, it is prudent to undertake biomechanical studies of the spine in various conditions: intact-normal, degenerated, surgery, and then “stabilization” of some sort. ese issues have been investigated using cadaver models, animal models, and numeric tools. is chapter focuses on the application of numeric approaches in understanding the biomechanics of the human spine, especially the analyses of spinal implants.
e human spine is composed of highly specic tissues and structures, which together provide an extensive range of motion (ROM) and considerable load-carrying capacity.
1
FIG. 11.2 A motion segment in the lumbar spine.
Alteration of the form of these structures with increasing age, injury, or any other reason can have a profound inuence
on the quality of life. Low back pain is generally associated with degenerative changes occurring in the spine. Mechani­cal property changes resulting from degeneration are likely contributors to lumbar spine instability that may lead to other pathologies. is instability may be accelerated by injuries or deformities.2 Vertebral body degeneration and ligament degeneration are degenerative diseases that can occur with age.3 e intervertebral disc and two facet joints form a three­joint complex and share the majority of the load on the spine.4 Due to this, degenerative changes of the spine can be initiated as disc degeneration or facet joint osteoarthritis.
5
In a spine segment (Fig. 11.2), the intervertebral disc and facet joints are the main load-bearing structures in the spine, and thus are most susceptible to mechanical wear and tear. Back pain arising from degenerative disease could be
Chapter 11 Finite Element Analysis 169
discogenic or may be directly due to diseased facet joints. e advanced stage of disc degeneration or facet degeneration may call for replacement surgery to achieve spinal stability and symptom relief. Disc arthroplasty and facet joint replacement technologies aim to restore the normal kinematics of the spine by acting as load-bearing devices.5 Surgery for these devices is highly invasive. Replacing either the disc or the facet joint would be considered a partial joint replacement. As load­bearing structures, there is also a possibility of wear of the device, leading to osteolysis. ere is a lack of literature on the kinematic eect of these replacement technologies on the
remaining structures of motion segments.
Many cadaveric and experimental studies have been for­mulated to compare the biomechanical behavior of the intact spine versus the injured or implanted spine. Motion across the segments as well as disc pressure measurements and facet loads have been quantied. However, there are many factors
that come into play, such as specimen variability and errors involved in experimental testing. In addition, prototyping of many implants at once is not physically easy. Currently, math­ematical models are being widely used to quantify forces and moments acting on the lumbar spine during various activities in life. ey can be used to quantify stresses at any area and thus point to the area where a fracture might occur. Almost all results seen in experimental testing can be quantied by mathematical modeling. Hence, the use of a mathematical method such as the FE method is justied for the study of the lumbar spine.
Because of the diculty in analyzing the spine as a whole, it has been divided into a number of regions (e.g., cervical, thoracic, lumbar), and each area has been analyzed separately
in dierent studies. For example, numerous studies of the lumbar spine have applied the FE models of the entire liga­mentous lumbosacral spine (LI–S1) or individual lumbar functional spinal units (FSUs; each functional unit consists of two adjacent vertebrae with connecting ligaments and inter­vertebral disc) to investigate the biomechanical behavior of the spine.
Some of the previous FE models of the lumbar spine have studied only the response of the motion segments, neglecting posterior elements,6 while the others did the entire motion segment with posterior elements7 or multimotion segments or the whole ligamentous lumbosacral spine.8 It is crucial to bear in mind that the simplications made in the development of
the model—such as in geometry, material denitions, load and boundary conditions, and so on—will directly aect the
accuracy of predictions.
Once the FE model is developed, it must be validated with relevant in vivo and in vitro test data. e model to be vali­dated should replicate the crucial features and characteristics of the real specimen in order to be able to be compared to experimental data that may help in ne-tuning the FE model.
For components such as ligaments, the experimental test data are required to dene the true mechanical behavior as well as failure modes and hysteresis characteristics of the correspond­ing element in the model. All these will enhance the precision of the FE simulations and outputs and will make them com­parable with real behavior of the spine.
9
ere are some specic considerations that should be taken into account in FE modeling of the spine in order to make the FE prediction reliable under a specic loading or motion condition. Following are some of these characteristics10:
e geometry of specic features should match the real
case, in which the shape of the construct aects the biomechanical outputs; examples are geometry of discs at dierent levels with the proper boundary prole in
the sagittal plane and the proper simulation of the anterior/posterior disc height and the angle between vertebral endplates at each segment.
e correct simulation of the lordosis angle due to its
main role in the stability of the spine under loads and load sharing across the segments.
e geometry of the posterior bone and partitioning of
the bony elements into cancellous and cortical with proper thickness of cortical bone across the vertebrae.
Proper denition of the element types for specic fea-
tures, such as ligaments, which can be dened either by two-dimensional (2D) truss or beam elements connect­ing to nodes of the model with correct moment arm with respect to the center of the segment. Ligaments can be modeled either as a bundle with appropriate cross­section or as a combination of individual truss elements with cross-section of unity.
e geometry of the facet articulations with their gap
distance and likely asymmetry.
Contact pattern between the articulating surfaces of
facets as a nite large-displacement contact problem with proper sliding (with or without friction) and normal (so or hard) behavior.
e disc should be modeled as a nonhomogeneous
composite structure, including an amorphous matrix (protoglycan and water) reinforced by collagenous
bers. Proper element types should be used for each area of the disc, that is, the nucleus can be modeled with noncompressible uid elements, while the anulus can be modeled with solid elastic elements with bers at proper angles by considering the radial variation of the collagenous bers’ mechanical properties and volume fracture.
In case a nonstatic simulation—such as dynamic loading,
impact, long-term creep and wear—is being considered, the time-dependent behavior of elements and materials needs to be specied.
e denition of loads and boundary conditions for
example, if the study of kinematics of L3–S1 spine is of interest, S1 is xed in all degrees of freedom and the compressive loads and bending moments are applied at L3 level.
Modeling of the Lumbar Spine
e rst intact FE model of the ligamentous lumbar spine that was developed consisted of two motion segments (L3–L5).11 e geometric data for the L3–L4 motion segment were acquired from 1.5-mm thick computed tomography (CT) scans (transverse slices) of a cadaveric ligamentous spine
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170 BASIC SCIENCE
specimen. Radiographs and dual-energy x-ray absorptiometry (DEXA) were used to ensure that no osseous abnormalities existed with the specimen and that the bone quality was good. Each region was then divided into several quadrilaterally shaped elements. e four nodes characterizing a particular element were digitized to obtain their X and Z coordinates with respect to the global axes system. e Y coordinate equaled the depth of the corresponding transverse slice on the CT lm. e transverse cross-sectional shape of an intact normal specimen is symmetric about the midsagittal plane. us, only one-half of the model was digitized; the other half was simulated as a reection of the rst half automatically by the FE soware. e coordinate data of elements from dier-
ent cross-sections were then assembled to generate three­dimensional meshes. e midtransverse plane of the L3–L4 disc was horizontal. A lordotic curve of approximately 9 degrees was simulated at the L4–L5 level of the FE model, based on the anthropometric data. e model validation study was undertaken by Kong.
12
en, the L5–S1 disc and the S1 vertebral body were added to the existing L3–L5 model to construct an L3–S1 segment. A total lordotic curve of approximately 27 degrees was simu­lated across the L3–S1 level with the mid-L3–L4 disc kept horizontal. e concluding L3–S1 model has a total of 27,540 elements and 32,946 nodes (Fig. 11.3). e number of ele­ments and the material properties of the intact L3–S1 model are presented in Table 11.1.
vertebral bodies were modeled as a cancellous (porous) bone core surrounded by a 0.5-mm thick cortical (dense) bone shell. e appropriate isotropic material properties were
dened for the respective regions (see Table 11.1).
Intervertebral Disc
e intervertebral disc was modeled as the anulus brosus and nucleus pulposus. e anulus brosus was modeled as a composite solid ground substance, reinforced with embedded bers. e ground substance was made up of 3D solid hexago­nal elements. e REBAR option (Abaqus) was used to dene the bers, which were oriented at alternating angles ±30 degrees to the horizontal. e “no compression” option was used for the REBAR elements such that they could transmit
Vertebral Body and Posterior Bone
e vertebral body and posterior bony regions were dened using three-dimensional solid continuum hexagonal elements with eight nodes, each possessing six degrees of freedom. e
TABLE 11.1 Element Types and Material Properties for the Intact L3–S1 Finite Element Spine Model
Element Set Elements (n) Element Type Young’s Modulus (MPa) Poisson’s Ratio Cross-Sectional Area (mm2)
Bony Regions
Vertebral cortical bone 3312 C3D8 12,000 0.30 Vertebral cancellous 10,608 C3D8 100 0.20 Posterior cortical bone 3632 C3D8 12,000 0.30 Posterior cancellous 1834 C3D8 100 0.20
Intervertebral Disc
Anulus (ground) 5376 C3D8 1.2 0.45
Anulus bers 2685 REBAR 357.5–550 0.30 0.00601–0.00884 Nucleus pulposus 1920 C3D8 1.0 0.4999
Joints
Apophyseal joints 216 GAPUNI Softened, 12,000
Ligaments
Anterior longitudinal 216 T3D2 Posterior longitudinal 144 T3D2 Intertransverse 30 T3D2
Ligamentum avum 21 T3D2 Interspinous 21 T3D2 Supraspinous 9 T3D2 Capsular 84 T3D2
7.8 (<12%), 20.0 (>12%)
10.0 (<11%), 20.0 (>11%)
10.0 (<18%), 58.7 (>18%)
15.0 (<6.2%),19.5 (>6.2%)
9.8 (<14%), 12.0 (>14%)
8.8 (<20%), 15.0 (>20%)
8.48 (<25%), 32.9 (>25%)
FIG. 11.3 Finite element model of the ligamentous L3–S1 segment.
0.30 74
0.30 14.4
0.30 1.8
0.30 40
0.30 40
0.30 30
0.30 34
GAPUNI, two-node unidirectional gap element.
From Dooris A. Experimental and Theoretical Investigations Into the Eects of Articial Disc Implantation. Doctoral dissertation. Iowa City: University of Iowa; 2001.
Chapter 11 Finite Element Analysis 171
only tension; also, the ber thickness and stiness increased in the radial direction. An overall collagenous ber content of
16% of the annular volume was distributed in the anulus.
e nucleus pulposus was modeled with C3D8 hexagonal
elements. Isotropic material property with a stiness of 1 MPa
and near incompressibility simulated with a Poisson’s v =
0.4999 was assigned to the nucleus to simulate its hydrostatic characteristics.
Apophyseal (Facet) Joint
Simulation of the facet joints is crucial for the spine model since it drastically aects the outcome of the analysis. In this model, the facet joints were simulated using 20 three­dimensional gap elements (GAPUNI). e facets were oriented at an inclination of 72 degrees from the horizontal plane. An initial gap of 0.5 mm was specied between these elements.
Force is transmitted by using the Abaqus “soened contact,” which exponentially adjusts the force transfer as the gap is closed. At full closure, the joint assumes the same stiness as
the posterior bone (Fig. 11.4).
Ligaments
All seven major ligaments—interspinous, supraspinous, inter­transverse, capsular, posterior longitudinal, anterior longitu­dinal, and ligamentum avum—were simulated in the model.
e ligaments were modeled using three-dimensional two­node truss elements (T3D2). Hypoelastic material properties were assigned to each of these ligaments, allowing a “neutral zone” to be incorporated in which the ligament provided little stability under minimally applied external loads. e hypo­elastic material denition was given by specifying varying
Young’s modulus and Poisson’s ratio along with the strain invariants at the specied strain rate. e material properties of ligaments were taken from the literature, including our own experimental data.13 e dening elements were aligned along the respective ligament ber orientation. Although the ligamentum avum and the longitudinal ligaments experience
a prestress at rest, all ligaments were assumed to be unstressed initially. Modeling the ligaments causes nonlinearity in kine­matics of the spine model (see Fig. 11.3).
Medial
Lateral
e entire process of developing the FE models of the spine
has been simplied due to the advances in technology.
e reconstruction of so tissue and hard tissue geometry
from magnetic resonance imaging (MRI) and CT scans is completed through the use of Mimics v15.0 (Materialise). MRI is capable of imaging both hard and so tissue (vertebrae and intervertebral discs) through manual segmenting. CT scans are capable of autosegmenting hard bone tissue but are dicult to use for reconstruction of so tissue. e segmented geom­etry is exported in the form of a standard triangle language (STL) surface le. ese les (especially manually segmented
geometries) are not smooth and require further processing.
Surface processing of the reconstructed geometry is
conducted in Geomagic Studio 2014. is soware is a
reverse-engineering soware that provides surface geometry modications. Aer importing the geometry, there are various functions that allow the surface to be precisely smoothed and edited. e smoothing is utilized to be able to achieve uniform meshes that are critical for achieving accurate and stable FE solutions. e editing that is conducted is used to adjust the overlapping surfaces to satisfy the requirements of the FE analysis soware.
e prepared surface geometry is then imported into HyperMesh 14.0 (Altair) to create the three-dimensional meshes. ese meshes are created such that they have optimal Jacobian and aspect ratios. Multiple mesh densities are created of each body to then perform mesh convergence. Mesh con­vergence is used to show that the solution of the FE problem is independent of mesh density. is method allows us to utilize accurate mesh with the lowest possible computational expense.
e converged mesh is then imported into Abaqus 6.14 (Simulia), and constructed. e construction of the model consists of assigning material properties to all geometries. Abaqus has the capability of assigning a variety of material types and constitutive models to accurately simulate the linear elastic, plastic, and hyperelastic properties of bones, implants, and so tissue. Interactions are then generated to tie surfaces together, such as the vertebral endplate to the intervertebral disc. Interactions are also used to generate contact denitions,
such as the articulation between a cage and endplate, to accu­rately simulate the contact force, contact area, stress, displace­ment, and so on. e appropriate one-dimensional elements are then added to the model to represent the small so-tissue
restraints that are not able to be reconstructed through MRI or CT data. Loading and boundary conditions are then applied to simulate various clinically relevant conditions. e outputs of the model are ROM, stress, strain, force, and contact mechan­ics in all of the reconstructed and instrumented geometries. Complex subroutines are available to simulate growth and deformities of the spine. Last, both static and dynamic loading scenarios are available to fully capture all studies of interest.
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FIG. 11.4 Facet joint in the nite element model of the L3–S1 spine.
Validation of the Lumbar Model
Formulating an FE model for a biologic system oen involves making justiable assumptions. Validation of an FE model is
essential in order to indicate whether the model predictions
172 BASIC SCIENCE
are similar to the experimental predictions. Previous biome­chanical studies using the intact two-segment FE model were validated with experimental in vitro studies.
12,14–17
Axial compressive preload acts as the major component of the in vivo preload. e exact degree and magnitude of the net preload relies on the degree of lumbar lordosis and the posture of the individual during physiologic loading. Axial compressive preload aects the load displacement character-
istics of the joint.4 e model was subjected to an axial preload of 400 N as a follower load since it is physiologic. In addition to the axial preload, motion was predicted for all six degrees of freedom with a moment of 10 Nm. Schultz et al.12 have reported the load-displacement properties in all principal directions with a compressive preload of 400 N. e compres­sive preload of 400 N was maintained while moments (4.7 Nm and 10 Nm) about the three principal axes were applied individually. Table 11.2 provides a comparison of the model predictions in response to bending and torsional moments compared to those reported by Schultz et al.12 e predicted facet loads were compared with Yang and King, and Drouin,
17b
and Kim.15 Radial disc bulge predictions at
17a
Shirazi-Adl
L4–L5, measured at the disc mid-height, were compared to previous experimental and analytic results. In response to the
TABLE 11.2 Comparison of Intact L3–L5 and L3–S1 Finite Element Predictions and Results From Schultz et al.
L3/5 FE Model Predictions
Rotation (Degrees) From 4.7 Nm Moment + 400 N Compression
Flexion L3–L4: 3.29
L4–L5: 3.36
Extension L3–L4: 1.84
L4–L5: 1.62
Right lateral bending L3–L4: 2.33
L4–L5: 2.31
Left lateral bending L3–L4: 2.33
L4–L5: 2.31
Right axial rotation L3–L4: 1.28
L4–L5: 1.25
Rotation (Degrees) From 10.6 Nm Moment + 400 N Compression
Flexion L3–L4: 5.32
L4–L5: 5.08
Extension L3–L4: 3.45
L4–L5: 3.35
Right lateral bending L3–L4: 5.13
L4–L5: 5.18
Left lateral bending L3–L4: 5.13
L4–L5: 5.18
Right axial rotation L3–L4: 2.98
L4–L5: 2.75
Finite element model predictions fall within one standard deviation of in vitro results.
12
L3/S1 FE Model Predictions
L3–L4: 3.20 L4–L5: 3.32 L5–S1: 4.45 L3–L4: 1.67 L4–L5: 1.40 L5–S1: 0.59 L3–L4: 2.32 L4–L5: 2.13 L5–S1: 1.63 L3–L4: 2.32 L4–L5: 2.13 L5–S1: 1.63 L3–L4: 1.34 L4–L5: 1.20 L5–S1: 1.00
L3–L4: 5.19 L4–L5: 5.00 L5–S1: 6.45 L3–L4: 3.83 L4–L5: 3.80 L5–S1: 3.72 L3–L4: 5.15 L4–L5: 4.91 L5–S1: 3.73 L3–L4: 5.15 L4–L5: 4.91 L5–S1: 3.73 L3–L4: 3.17 L4–L5: 2.97 L5–S1: 2.56
In Vitro Results
5.13 ± 1.86
2.12 ± 0.98
4.47 ± 1.63
4.32 ± 1.47
0.69 ± 0.33
5.51 ± 1.00
2.99 ± 1.02
5.64 ± 1.22
4.90 ± 0.79
1.50 ± 0.67
compressive preload, the mean lateral disc bulge was 0.12 mm for a 400 N load. Although these values are somewhat low, the values were in the range reported by Dooris et al.7 Ligament strains were predicted in response to an axial compressive load of 400 N, coupled with bending moments of 5 and 10 Nm about the three principal axes. e trends seen were close to
the in vitro work reported by Panjabi et al.
17
e FE solutions are dependent on the mesh renement. Using a large number of elements is known to reduce error, and the mesh should be rened until a stage is reached at which the results from the current renement iteration are similar to the results obtained by the previous renement iterations. Such a mesh would be an optimized mesh, which enables the model to predict correct results. Further rene­ment beyond this point can theoretically induce more errors. us, the mesh of the L3–L5 FE model was further rened and the L5–S1 segment was added. e results between the L3–L5 model and L5–S1 model exhibited a strong correlation (see
Table 11.2).
To further validate the L3–S1 model, a cadaveric study was undertaken recently. e study involved comparing experi­mentally predicted load-displacement behavior using the Optotrak with FE model predictions.18 Five fresh ligamentous lumbar L1–S1 spine specimens were used for the experimental tests. Specimens were potted in a rigid base secured to the sacrum and a loading frame likewise was secured to the L1 vertebral body. To determine the load-displacement behavior of the specimen, a set of three light-emitting diodes (LEDs) was attached to each vertebral body (Fig. 11.5). e Optotrak motion measuring system (Northern Digital Inc.) was used to track the spatial location of the LED markers secured rigidly to the vertebral bodies, including the base, during the load­displacement evaluation. e specimen was loaded to a maximum of 9 Nm in all six degrees of freedom. e intact FE model was also subjected to similar loading of 9 Nm as the cadaveric testing. e angular displacement data for the
FIG. 11.5 The ligamentous L1–S1 segment with light-emitting diodes, used
to predict angular displacements.