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Chapter 11 Finite Element Analysis 173
CADAVERIC AND FE MODEL COMPARISON
C
Intact right rotation (cadaveric) Intact right rotation (FE model)
Spinal segment
Angular displacement (degrees)
CADAVERIC AND FE MODEL COMPARISON
B
Intact right bending (cadaveric) Intact right bending (FE model)
Angular displacement (degrees)
CADAVERIC AND FE MODEL COMPARISON
Angular displacement (degrees)
A
experimental testing and the FE model were compared across L3–S1, L3–L4, L4–L5, and L5–S1 segments. It was found that the FE model predicted angular displacements across the segments falling within one standard deviation of the experi­mental data (Fig. 11.6).
Finite Element Model of the Cervical Spine
A full cervical spine (C1–C7) computational model was developed that involved the following steps.
22 20 18 16 14 12 10
–2 –4 –6
–8 –10 –12
8 6 4 2 0
L3-S1
Flexion
Extension
L3-L4
Spinal segment
Intact flexion (cadaveric) Intact flexion (FE model) Intact extension (cadaveric) Intact extension (FE model)
L4-L5 L5-S1
Conversion of CT and MRI Scans to 3D Solid Model
To construct the geometry of the cervical spine, CT scan images of a woman (25 years old) without any abnormalities with 1-mm slice thickness were obtained from the radiography department of University of Toledo Medical School. Mimics
13.1 soware package (Materialise) was used to construct the
required 3D structures. For the CT images obtained, bone contrasting and thresholding procedures were done to each bone part, and related masks were developed. en, by utiliz­ing the region growing tool, the initial geometry was developed (Fig. 11.7). Smoothing, wrapping, and ltering functions were
executed to obtain good-quality geometry. A similar proce­dure was followed to obtain 3D structures of ve intervertebral discs (C23, C34, C45, C56, and C67) from MRI scans.
Meshing
Each individual 3D structure was imported into the Iowa FE Mesh soware for creating the mesh structure. A series of
building blocks was constructed around the 3D structure, assigned a desired mesh density, and projected onto the surface representation, creating a 3D FE model. Finally, the mesh quality module in the soware was used to evaluate, and thus develop, the high-quality mesh for the model. Fig. 11.8 shows the meshing procedure for C3 vertebra.
SECTION
I
14 12 10
8 6 4 2
0 –2 –4 –6 –8
–10 –12 –14
10
8
6
4
2
0
–2
–4
–6
–8
–10
FIG. 11.6 (A) Comparison of the experimental and nite element (FE)
model results for exion and extension in response to a 9-Nm pure
moment. (B) Experimental and FE model results are compared in left and right bending in response to a 9-Nm pure moment. (C) Experimental and FE model results are compared in left and right rotation in response to a 9 Nm pure moment.
Right bending
Left bending
L3-S1 L3-L4
Spinal segment
Right rotation
Left rotation
L3-S1 L3-L4
Intact left bending (cadaveric) Intact left bending (FE model)
L4-L5 L5-S1
Intact left rotation (cadaveric) Intact left rotation (FE model)
L4-L5 L5-S1
Finite Element Analysis (Using Abaqus Version 6.11)
Abaqus soware was used for the FEA. Meshed parts were imported into this soware for FEA. Ligament insertion points and material properties of all of the so and hard tissues were extracted from literature.
18a
Finally, assembling all of these parts and assigning their respective material properties developed the three-dimensional nonlinear full cervical spine FE model.
e intact model contained 217,366 nodes and 181,336 elements. e global coordinate system of the model (X, Y, and Z) was oriented in such a way that the positive Y is from anterior to posterior of the spine, positive X is from right to le of the spine, and positive Z is from bottom to top of the spine.
Vertebral Body and Posterior Bone
Similar to the lumbar model, the cervical vertebral body con­sists of a thin cortical shell (0.5 mm of thickness) surrounding a soer cancellous core. e posterior region was assigned attributes, which lay between those of the cortical and cancel­lous regions. ree-dimensional, isoparametric solid elements (C3D8) were used to dene the osseous geometry.
Facet Joints
A contact formulation was used to dene the contact pattern between articulating surfaces in facet joints with an initial gap of 0.5 mm based on CT imaging and dissection procedures. e contact was dened with an exponentially increasing modulus as the gap distance between the inferior and superior facets decreased, simulating the presence of cartilage in the facet region. e facets were oriented at approximately 45
174 BASIC SCIENCE
C
D
A
FIG. 11.7 Visualization module of Mimics version 13.1 (Materialise). (A–C) Frontal, axial, and sagittal scan views,
respectively, in which bone contrasting, thresholding, and masking were performed for the computed tomographic slices. (D) Three-dimensional structures developed by performing the smoothing and ltering
options.
B
FIG. 11.8 Meshing procedure for the C3 vertebra. The left image depicts the three-dimensional C3 vertebra,
the center image shows the constructed building blocks, and the right image depicts the meshed vertebra, respectively.
degrees from the horizontal plane, with some variation in the sagittal plane alignment, according to CT geometry. e facets were also of varying curvatures from right to le sides, indi-
cating the possibility of varying contact during right or le loading modalities from the right to le facets.
Intervertebral Disc and Luschka’s Joints
e anulus brosus was modeled as a composite conguration in which a series of bers simulating the lamellae of the disc were embedded in a ground substance surrounding a more gelatinous nucleus region. Each layer of ground substance contained two alternating layers of bers arranged at ±65 degrees from the transverse plane, with an overall ber content of 20% of the annular volume assumed. REBAR element type with no-compression option was used to dene the bers. Brick elements were used to model ground substance and the nucleus pulposis was dened as incompressible uid.
Luschka’s joints were modeled as well in the cervical discs.
ese were simulated around the area of the uncinate pro­cesses and the anulus horizontal layers around the uncinate processes.
Ligaments
e ligaments of the lower cervical spine that were modeled include the anterior longitudinal ligament (ALL), posterior longitudinal ligament (PLL), interspinous ligament (ISL), liga­mentum avum (LF), and the capsular ligaments (CAPs). e
alar ligament (AL), transverse ligament (TL), anterior and posterior atlantoaxial ligaments (AT-AX, PAT-AX) were modeled for the upper cervical spine. e ligaments were modeled using three-dimensional truss elements with hypo­elastic material behavior.
Fig. 11.9 shows a 3D view of an FE model of the C1–C7
spine and all its components. Material properties and
Chapter 11 Finite Element Analysis 175
Transverse
Spinous process
C1
C2
Intervertebral
Vertebral body
FIG. 11.9 Finite element model of the ligamentous C1–C7 cervical spine.
disc
Facet joint
C7
C5
C6
C3
C4
process
Uncinate process
cross-sectional areas used in dening the various entities in the C1–C7 model are summarized in Table 11.3. ese were chosen based on values published in the literature and were assumed to be homogeneous and isotropic.
7
Application of the Finite Element Model of the Spine
One of the main advantages of FE modeling of the spine is its extensive application in simulating the eects of various
trauma and spinal disorders on the biomechanics of the spine. Numerous studies have simulated dierent spinal injuries and compared various biomechanical parameters, such as angular motion and stress distribution across degenerated and adja­cent segments, between intact and injured spine models. e outcomes of such analysis have well served engineers in coming up with innovative ideas and solutions in the design of suitable implants to address the pain and restore to normal the biomechanics of the damaged segment. Implants are useful in treatment of spinal injuries when conservative therapies fail to reduce the pain and restore the patient to a normal daily routine. Invasive surgeries aim to remove the pain-causing structures, stabilize the segment, and correct bone failure due to trauma or disease.
Once the FE model of the intact spine is created, it can be easily modied to simulate dierent injuries by various tech­niques, such as removing certain elements (e.g., facetectomy, laminectomy), changing the material properties (e.g., laxity in ligaments), or modifying the geometry (disc herniation and degeneration).
For example, spinal stenosis is a progressive degenerative condition that occurs when the articulating facet joints become arthritic and no longer provide necessary stability to the spine. e arthritic facets become inamed and osteophytic
TABLE 11.3 Element Types and Material Properties for Finite Element Model of Intact C1–C7 Cervical Spine
Young’s Element Group Name
Cortical bone C3D8 10,000 0.3
Cancellous bone C3D8 450 0.25
Posterior bone C3D8 3500 0.25
Anulus ground
substance
Anulus bers REBAR 0.45
Nucleus
pulposus
ALL T3D2
PLL T3D2
LF T3D2
ISL T3D2
CAP T3D2 15 (20-40%)
TL T3D2 20 0.3 18.0
AL T3D2
AT-AX T3D2
PAT- A X T3D2
AL, alar ligament; ALL, anterior longitudinal ligament; AT-AX, anterior atlantoaxial ligament; CAP, capsular ligament; ISL, interspinous ligament; LF, ligamentum avum;
PAT-AX, posterior atlantoaxial ligament; PLL, posterior longitudinal ligament; TL, transverse ligament.
Element Typ e
C3D8 4.2 0.25
C3D8H 1 0.4999
Modulus
(MPa)
15 (<12%)
30 (>12%)
10 (<12%)
20 (>12%)
7 (<12%)
30 (>12%)
5(<25%)
10 (>25%)
30 (>40%)
3.0(<17%)
8.5(>17%)
0.2(<17%)
1.25 (>17%)
6.0(<17%)
10.0 (>17%)
Poisson’s Ratio
0.3 33.0
0.3 33.0
0.3 50.1
0.3 13.0
0.3 46.6
0.3 22.0
0.3 5.0
0.3 5.0
Cross-sectional Area (mm2)
(produce bony spurs), resulting in irritation and impingement of nearby nerves, leading to clinical symptoms. e current
nonconservative treatment for spinal stenosis is surgical decompression and spinal fusion with instrumentation to achieve spinal stability and symptom relief. Decompression is a surgical procedure, which is performed to alleviate pain caused by pinched nerves (neural impingement). e surgical procedure for decompression includes removal of part of the lamina (laminectomy), spinous process, facets (facetectomy), ligaments, and/or sometimes part of the intervertebral disc (microdiscectomy).
Although clinical studies have shown that decompression surgery enhances neurologic recovery, pain relief, and mobil­ity, signicant destabilization of the spinal motion segment is seen aer decompression, especially if the facet joint is
removed.
Addition of a posterior fusion system, including pedicle screws interconnected with a rigid rod, is a common proce­dure to restore the stability of the aected segment.
ough fusion is able to restabilize the implanted segment, it can result in accelerated degeneration of the adjacent motion
SECTION
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176 BASIC SCIENCE
segment and morbidity from muscle stripping. Fig. 11.8 shows an L3–S1 model of the spine with a fusion system at the L4–L5 level.
Clinical Application of the Finite Element Models of the Spine
FE analysis has become a cost-eective and ecient means to predict the biomechanics of the spine under physiologic and pathologic conditions. While useful, the model is not without limitations due to the constraints of a biologic system and its associated properties being modeled by a digital representa­tion. e material properties of the ligaments (supraspinous, interspinous, ligamentum avum, and so on) were obtained
from the literature, while the intervertebral disc was modeled as a homogeneous composite ground substance. It can be inferred that the data used to generate the models can be thought of as an “average” of the normal population, just as reference ranges are for determining the upper and lower threshold of certain markers in routine bloodwork.
FE models are based on a number of assumptions, such as the fact that the generated models should apply equally to all members of a population. In clinical practice, this does not oen hold true. Just as individual patients may have varia-
tions in their spine anatomy, the rate of degeneration and the impact of degenerative processes may vary from patient to patient, making generalizations about the “best” treatment for a particular type of spinal pathology far from simple. Oen in clinical practice, patients with a similar degree of degenerative pathology may have widely dierent clinical manifestations or,
in some cases, may be completely asymptomatic. e challenge in making decisions with patients in regard to their pathology rests on the ability of the clinician to integrate biomechani­cal data derived from FE models, the radiographic data, and the patient’s clinical symptoms. us, it becomes important to not use computational models alone to determine the appropriate treatment for an individual patient. Addition­ally, the patients that are seen in practice oen are far down the degenerative cascade, at which point surgery may only temporarily alleviate their symptoms before their recurrence due to scarring, nociceptor hypersensitivity, and/or further degeneration.
Another limitation of an FE model is that the stability of the ligamentous spine is less than a spine in vivo due to absence of the muscles and ligaments. e load-bearing qualities and structural support aorded by the muscles and ligaments have been shown to vary greatly, and are inuenced
by the age and quality of bone, the rate of loading, as well as other physiologic and hereditary characteristics that cannot be modeled by current computational techniques. In addition, there have been observations that cadaveric models may show
dierent biomechanical properties based on preparation, and that the in vivo tissue failure properties may be lower than that predicted by FE models.19 e importance of the muscu­lature and ligaments and their contribution to spinal stability is emphasized by the recent surge of interest in minimally invasive techniques for arthrodesis that minimize muscle dissection.
Currently, FE models are limited in their ability to evaluate the spine as a whole, and are instead divided into regions (cervi­cal, thoracic, lumbar) to facilitate analysis of their mechanical properties. By isolating these segments and subjecting them to biomechanical analysis, they do not address global spinal parameters, such as sagittal and coronal balance, which have become increasingly important in treating spinal pathology. In addition, the spine’s relationship to the pelvis and pelvic parameters—such as pelvic tilt, pelvic incidence, and sacral slope—are currently not addressed by FE models but are used increasingly by surgeons in making treatment decisions that impact clinical outcomes and patient satisfaction.
Because FE models are typically based on a specic subject
or an ideal average subject, there is concern regarding the applicability of FEA to clinical practice. Many studies have been conducted with the goal of accounting for intersubject variability as a result of aging and anatomic deformities. For example, patient-specic FE models have been constructed to investigate the risk of femoral neck fracture,20 account for intersubject variability of biomechanical factors in animal studies,21 and to support the interpretation of clinical results in follow-up studies. Reggiani et al. reported a preliminary validation of patient-specic FE models with regard to pre­dicting the subject-specic primary stability of cementless implants during preoperative planning.
22
Although a need remains for a validated model that accounts for injury, deformity, or disease, more recent studies have demonstrated the usefulness of coupling FEA with patient-specic information from clinical CT scans to mecha­nistically simulate bone failure. is approach has been vali­dated by numerous groups for the spine and hip, and clinically has been shown to be signicantly associated with incident and prevalent fracture in multiple cohorts. A study conducted by Kopperdahl et al. has further demonstrated clinical inte­gration of FEA through its use of FEA-based vertebral strength assessments and vertebral trabecular bone mineral density (BMD) to predict incident vertebral fractures in women.
23
e International Society for Clinical Densitometry (ISCD) has recently developed new ocial positions for the clinical use of quantitative CT (QCT)-based FEA of the spine and hip, specically with regard to the management of osteoporosis in adults. According to the ISCD, QCT-based FEA can be used to assess fracture risk, initiate pharmacologic treatment of low vertebral and femoral strength, as well as monitor age- and treatment-related changes to bone strength.
24
Perhaps the most important application of FE models in the spine is their utility in creating medical devices that are intended to arrest the degenerative cascade. In current clinical practice, a signicant proportion of spine procedures are centered around removing oending pathology (laminectomy, facetectomy,
corpectomy, and so on) and fusing the levels of interest using implants such as rods and pedicle screws. Over time, the inam-
matory cascade that promotes healing fuses the operated levels while placing stress on the adjacent motion segment. While, in many cases, the patient’s preoperative symptoms may temporar­ily improve, symptom recurrence and/or exacerbation in the future is not uncommon due to accelerating the degenerative cascade in the adjacent level. e existence of conditions such as
Chapter 11 Finite Element Analysis 177
ROM in extension
“failed back surgery syndrome” (FBSS) and patient dissatisfac­tion aer repeat fusion surgery suggest that the data used to
create implants and to perform spine surgery are limited in their ability to truly predict the surgical solution that is ideal for a particular patient. Importantly, the data used to generate FE models is from cadaveric spine specimens that have not undergone fusion surgery, making predictions about the rate of degeneration or adjacent-level disease approximations at best.
ese developments highlight the advantages of FEA and advance the goal of bringing FEA closer to clinical application. As FE models evolve, the ability to evaluate the spine as a whole, incorporation of global spinal alignment parameters, and including elements such as spinal musculature and ligaments may aid in increasingly accurate predictions of the spine in vivo. It should also be noted that current FE models are based on static imaging and do not incorporate dynamic radiographs (exion, extension, and lateral bending), which
also prove to be important in surgical decision making.
More recently, nonfusion-based spinal implants are being used as an alternative to stabilizing the spine aer decompres-
sion. Unlike fusion, nonfusion stabilizing systems allow for angular motion, shear stability, and adjusting to the instant axis of rotation of the motion segment during movement. Fig.
11.9 shows the L3–S1 spine implanted with a posterior
dynamic stabilizer system (PDS; Disc Motion Technologies). e implant was placed at L4–L5 following the surgical pro­cedure of total facetectomy at L4–L5. e PDS consisted of a pair of metallic (chrome-cobalt) sliding parts (male and female) connected to the spine by titanium pedicle screws at each side.
To simulate the physiologic loading condition on the spine, once the implanted model was created, both implanted and intact models were loaded with 400 N of compressive follower preload plus 10 Nm of moment to simulate exion, extension, le/right bending, and le/right rotation. Various biomechani­cal parameters such as motions, intradiscal pressure, and facet
loads were compared between the intact and implanted model (Fig. 11.10).
e intervertebral articial disc is another example of spinal implants recently proposed as a treatment for the degenerated disc. Unlike fusion systems, the total disc replace­ment (TDR) promises to address facet pain, mimic the motion of the intact spine, and avoid degeneration at the adjacent segment. ere are various designs available for discs. Some require an anterior surgical approach for replacement as opposed to others that are placed from the posterior side of the spine. Fig. 11.11 shows a posterior disc system (Disc Motion Technologies), including a pair of cobalt-chrome sliding parts. is disc is placed into the spine following the surgical removal of the facets at the operative level. Since the facets are removed, the spine is restabilized by the addition of a PDS system as previously discussed. e combination of PDS and disc is a 360-degree motion system that is able to restore the motion of the operated segment back to normal. To assess the biomechanics of the implanted spine, FEA was
FIG. 11.10 Fusion system at the L4–L5 level of the lumbar spine.
SECTION
I
PDS system
ROM in flexion
Extensions fixed into
pedicle screws
Ball & socket
joints
FIG. 11.11 The L3–S1 spine implanted with a posterior dynamic stabilizer system at L4–L5. ROM, range of
motion; PDS, posterior dynamic stabilizer.
178 BASIC SCIENCE
used, and motion, intradiscal pressure, and facet loads across segments were calculated and compared between intact and implanted models (Figs. 11.10–11.12).

Conclusion

In addition to its most obvious and time-tested uses, such as the evaluation of early-stage prototypes, FEA is a useful tool in the evaluation of the biomechanical eect of various surgi-
cal interventions, including a range of implants—from those that are designed for fusion to motion preservation devices. FEA aids in predicting the behavior of such implants in the long term by means of evaluating some crucial mechanical factors, such as wear and fatigue.
Studies in biomechanics of the spine have shown that FEA
and in vitro cadaveric testing are complementary techniques,
Posterior
artificial disc
FIG. 11.12 The L3–S1 spine implanted with a posterior dynamic stabilizer
and articial disc at L4–L5.
FIG. 11.13 Motion, intradiscal pressure, and facet loads across segments for intact and implanted models.
Ext., extension; Flex., exion; L.B., left bending; L.R., left rotation.
Chapter 11 Finite Element Analysis 179
and thus are well suited to characterize the complex biome­chanical behavior of the spine and its anatomic structures, including internal stresses/strains of the intervertebral disc, facet joints, and any ligaments of interest. However, like cadaver investigations, FE models have several limitations. For example, they do not account for variations in the geometry of the specimens, such as facet orientation and material prop­erties that vary from specimen to specimen. But, for a given model geometry, the predicted data are in reasonable agree­ment with the results from the in vitro investigations. us, the use of an experimentally validated FE model can provide very useful information for many clinical questions being raised by the use of spinal implants.
One of the most far-reaching and interesting questions for which FEA may be able to provide some insight is in the nature of adjacent-level degeneration. Because the FE method provides the means for simulation of changes in motion and loads over time along with the eects of surgical intervention and changes
in geometry and material properties due to degeneration, highly advanced, dynamic models of the spine may be able to replicate the progression of degeneration following surgical intervention and compare it to the natural course of the disease. While this will require considerable advancement in FE modeling techniques, it is perhaps the most promising means of answering the age-old question of whether adjacent-segment degeneration is actually attributable to surgical intervention or solely the manifestation of the underlying disease.

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II
SECTION
DIAGNOSIS
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