Available online at www.sciencedirect.com Clinical Biomechanics 23 (2008) 859–869 www.elsevier.com/locate/clinbiomech Stress distribution in the intervertebral disc correlates with strength distribution in subdiscal trabecular bone in the porcine lumbar spine Garrett Ryan a,b,*, Abhay Pandit a,b, Dimitrios Apatsidis a a Department of Mechanical and Biomedical Engineering, National University of Ireland, Galway, Ireland b National Centre for Biomedical Engineering Science, National University of Ireland, Galway, Ireland Received 18 June 2007; accepted 20 March 2008 Abstract Background. It is understood that an interdependence of properties exists between the intervertebral disc and the subdiscal trabecular bone. Determining the biomechanics of this relationship is important in the development of novel spinal implants and instruments. The aim of this study was to analyze this relationship for the porcine lumbar spine and to compare it with that of the human spine. Methods. The stress distribution within the intervertebral disc of 10 porcine lumbar (L4/L5) motion segments was recorded using a 1.5 mm needle pressure transducer. For dynamic loading a specialized testing rig was developed to apply flexion/extension and medial/ lateral bending while intervertebral disc stress was simultaneously recorded. The regional variation in mechanical properties of trabecular bone was also examined for an additional 10 porcine (L5) vertebral bodies. For compressive testing of the subdiscal bone, columns were prepared using a low speed cutting saw and subjected to axial compression. Findings. Under pure compressive loading, stress levels within the intervertebral disc were relatively uniform. However, during asymmetric loading large peak stresses were evident in the periphery of the intervertebral disc in areas underlying the annulus fibrosus. The mechanical properties of trabecular bone demonstrated regional variations within the vertebral body. The ratio of compressive yield strength of bone underlying the outer annulus fibrosus to that of bone underlying the nucleus pulposus averaged 1.36. Interpretation. Although the effects of stress distribution and bone mass adaptation cannot be directly related, it is probable that peak stresses arising in the annulus fibrosus during asymmetric loading provide greater stimuli for the underlying bone to undergo adaptive remodeling to withstand the greater forces experienced. Findings of intervertebral stress distribution and strength distribution of subdiscal trabecular bone for the porcine spine may aid in the development of strategies for preclinical animal testing of spinal implants. Ó 2008 Elsevier Ltd. All rights reserved. Keywords: Biomechanics; Intervertebral disc; Trabecular bone; Adaptive remodeling; Porcine 1. Introduction Animal spines are widely used in the biomechanical analysis of prospective spinal instruments, due to the low availability and high cost of human tissues. For practical reasons, bovine and porcine spines, especially the latter, * Corresponding author. Present address: CIMRU Building, Nuns Island, National University of Ireland, Galway, Ireland. E-mail address: [email protected] (G. Ryan). 0268-0033/$ - see front matter Ó 2008 Elsevier Ltd. All rights reserved. doi:10.1016/j.clinbiomech.2008.03.066 are most popularly selected as the model for both in vitro and in vivo studies (Kaigle et al., 1997; Keller et al., 1990; Pfeiffer et al., 1994; Teo et al., 2006). Interpretation of data from such studies usually considers the limitations related to the mismatch of properties between the human and animal tissues. Although the physical and mechanical response of the human lumbar spine have been widely studied (White and Panjabi, 1990), less efforts have been made in comparing its properties with those of porcine spines, despite ongoing clinical studies using these animals. Understanding the mechanism of load transfer through the various 860 G. Ryan et al. / Clinical Biomechanics 23 (2008) 859–869 tissues of the porcine spine is important in the testing and validation of new spinal implants and in the interpretation of mechanical data from studies using these animals. The porcine intervertebral disc (IVD) is constructed, as in humans, of a central gel-like nucleus pulposus (NP) surrounded by a peripheral firm annulus fibrosus (AF). Since it is essentially composed of two parts, it is important to determine how each of these structures contributes to the IVDs load bearing capacity and resulting redistribution of load to subdiscal trabecular bone. In studying the human spine, researchers have shown that several factors such as posture (Adams et al., 2000a,b; Edwards et al., 2001; Steffen et al., 1998), muscle tone (Wilke et al., 1996a,b), spinal load (McNally and Adams, 1992; Ranu, 1990), and time (Adams et al., 1996a,b) are significant in influencing the distribution of stress within the IVD. With regards the distribution of strength within the vertebral body, research has aimed towards better prediction of osteoporosis and related fractures. In these efforts, a number of researchers have shown an uneven distribution in mechanical and morphological properties of trabecular bone inside the vertebral body of human and quadrupedal species (Gong et al., 2006; Keller et al., 1989; Lin et al., 1997). Keller et al. (1989) found that the mechanical properties (strength, stiffness) and density of subdiscal trabecular bone specimens prepared from 12 regions within the vertebral body were highest in regions underlying the NP and lowest in regions underlying the AF. Similarly, a study by Lin et al. (1997) analyzing the regional strength distribution of trabecular bone in the porcine lumbar vertebral body found that the average ultimate strength of the bone underlying the NP was consistently higher than the bone underlying the AF. Recently, Gong et al. (2006) investigated the three-dimensional microstructural properties of L4 vertebral bodies using micro-computed tomography (lCT). Specimens were divided into two groups according to the average structure model index (SMI) of the 15 specimens inside the vertebral body. Trabecular specimens with lower mass were liable to form a high-SMI group and it was found that the anterior column (underlying the AF) in this group was more susceptible to vertebral body wedge fracture. However, in the low-SMI group, off-axis bone damage was found to be most harmful to the central column of vertebral trabeculae, which underly the NP. In light of Wolff’s law that stress-morphology relationships exist for most biological structures (Wolff, 1884), load transfer through the IVD and subdiscal vertebral bone properties should be interrelated. This is apparent in a recent study by Adams et al. (2006), who showed that IVD degeneration was associated with reduced loading of the anterior vertebral body in upright postures. Removal of stimulus to the bone underlying the anterior IVD permitted negatively balanced remodeling and corresponded with reduced bone mineral density (BMD) and inferior trabecular architecture in this region. This predisposed the anterior vertebral bone to compressive fracture when the spine was flexed. For the human and quadrupedal spine, it is evident that an interdependence of properties exists between the IVD and subdiscal trabecular bone. Accordingly, the objectives of this research were twofold: firstly, to examine the stress distribution in the IVD of porcine lumbar functional spine units or ‘motion segments’ under physiological activities using multi-localized pressure measurements, and secondly, to analyze the regional distribution of compressive properties of the subdiscal trabecular bone of porcine lumbar vertebral bodies. Results are compared with those of human spines and the effect of anatomical and age-related variation is addressed. 2. Methods Twenty fresh porcine lumbar spines were harvested from 8-month-old landrace pigs weighing 90–100 kg immediately after sacrificing. The spines, with attached muscles and ligaments, were vacuum sealed and kept in frozen storage at 20 °C until testing. Before testing, each specimen was thawed to room temperature overnight and then wrapped in normal saline soaked cloth for 4–5 h. Separate spines were used for each of the two studies as outlined below. 2.1. Measurement of stress distribution in the IVD A pressure probe similar to that described by McNally and Adams (1992) was developed for use in this study. The probe consisted of a miniature pressure transducer embedded in a 1.5 mm diameter stainless steel needle (Gaeltec Ltd., Isle of Skye, Scotland). The transducer diaphragm was rectangular in shape and measured 2.5 mm 1 mm. The needle had a sharp pointed tip to facilitate easy insertion into the IVD and had been graduated by the authors with laser markings so that the depth of insertion could be gauged. The probe was calibrated using a sealed pneumatic chamber (Instrument Technology Ltd., Dunboyne, Co., Meath, Ireland) and was found to have a linear ramp up to 4 MPa without damage. A testing rig was developed to introduce controlled flexion/extension and medial/lateral bending to the porcine motion segment, while data from the needle pressure transducer could be simultaneously recorded (Fig. 2). The testing rig was designed for mounting with the Instron 8874Ò servohydraulic testing machine (Instron Corp., Norwood, MA, USA), which can apply axial and torsional loads to the motion segment. Ten L4–L5 motion segments were harvested from the porcine lumbar spines. Care was taken to preserve the ligaments while other soft tissues were completely removed. The major coronal and sagittal diameters of the L3/L4 and L5/L6 IVD’s were recorded. An average of these values was used to approximate the size of the L4/L5 IVD. This data was later used to determine the placement of the pressure transducer probe in predefined locations within the IVD according to the arrangement in Fig. 1. G. Ryan et al. / Clinical Biomechanics 23 (2008) 859–869 0.85 L 0.9 D 0.6 L 0.2 D L 0.4 L 0.6 L D Fig. 1. Schematic showing pressure measurement points in the IVD. The intersection of the major coronal and sagittal diameters was taken as the centre of rotations of each motion segment based on these average values. The motion segments were secured with bone screws and potted using low melting point alloy (Tm: 40 °C). A dowel pin was positioned in the centre of the cementing pot to hold the motion segment in position while it was being secured. The testing rig consisted of a number of tiers, separated by large deep-groove ball bearings as illustrated in Fig. 2. The potted motion segment was attached to the upper tier, which was essentially a geared platform. The centre of rotation lay 15 mm from the base of the cementing pot. The NP was placed at the centre of rotation of the geared platform with careful reaming of the L5 vertebral body so that the base of the vertebral body was 15 mm from the centre of the IVD. Also, an aligning hole for the central dowel pin was drilled into the vertebral body directly below the centre of the NP. This was taken from previous measurements of the L3/L4 and L5/L6 IVD’s. The geared platform revolved to introduce varying degrees of flexion/extension and medial/lateral bending to the motion segment. The bearings allowed the entire platform to be rotated to alternate between flexion/extension and medial/lateral bending without disruption of the motion segment. Using a 1mm diameter needle, incisions were made into the IVD prior to introducing the needle pressure probe in order to limit the risk of damaging the transducer diaphragm. The needle pressure probe was gradually advanced into the IVD with the transducer diaphragm facing upward so that only axial stress was recorded. A clamp held the needle in position while measurements were carried out. For positioning in the posterior AF the needle was first pushed through the IVD, then retracted slowly until a sharp increase in stress was noted. The needle’s position was then confirmed on the basis of the earlier standard measurements. Initially, stress data was recorded at each measurement location, with incremental axial compressive loads of 200 N up to 800 N, applied to the motion segment. The axial loads adopted in this study were chosen based on previous studies using porcine spines (Park et al., 2005; van Deursen et al., 2001). Subsequently, a sequence of movements was executed with the testing rig. This involved flexion/extension from 1° to 4° followed by medial and lateral bending from 1° to 4°. The range of motion was adopted L4/L5 Spinal Motion Segment & Intervertebral Disc Needle Pressure Transducer Upper Tier (Attaches To Servohydraulic Testing Machine) Stepper Motor Internal Gear And Pinion 861 Universal Joint Assembly Middle Tier (Introduces Flex./Ex. & Lat. Bending) Deep Groove Ball Bearings Stepper Motor Bottom Tier (Rotates Middle Tier Between Flex/Ex. & Lat. Bending) X-Y Table Fig. 2. Schematic showing spinal testing apparatus and relevant components. 862 G. Ryan et al. / Clinical Biomechanics 23 (2008) 859–869 from previous research involving ovine and bovine spines (Wilke et al., 1996a,b, 1997), as no data was available for the range of motion of porcine spines. The rig’s stepper motors were employed to introduce the movements at a rate of 1°/s. We developed a software programme using LabViewÒ (National Instruments Corp., Austin, TX, USA) to synchronize control of the rig’s two stepper motors and the data recording process. Data was collected using a USB 6008Ò data acquisition device (National Instruments Corp.). Throughout this movement sequence the axial load was maintained at 300 N. Care was taken to keep the motion segment hydrated at all times by continuously spraying with saline solution. Following testing, the L4/L5 motion segment was isolated and cut along the transverse plane so that it’s cross sectional area (CSA) could be measured. This was performed by placing a transparent plastic grid over the IVD and sketching the outline onto the plastic. By counting the squares of the grid that fell within the outline, the CSA could be determined. The outer perimeter of the NP was defined by the presence of laminae of fibrous AF tissue. By outlining this boundary on the transparent plastic grid the CSA of the NP was also determined. 2.2. Measurements of strength distribution in subdiscal trabecular bone Ten L5 vertebral bodies were harvested from the porcine spines. The vertebrae had all soft tissues and bony processes removed using a bone saw. A low speed cutting saw (Buehler Ltd., Lake Bluff, IL, USA) with specially designed clamping fixtures was used to section each vertebral body into 5 mm 5 mm 12 mm cubes from predetermined anatomical regions as portrayed in Fig. 3. In total, 16 rectangular columns of trabecular bone were prepared from each vertebral body. The dimensions of each specimen were measured using a precision micrometer. The long axis of each specimen was kept parallel to the lonMid-Coronal Plane D E F A B C G H Mid-Sagittal Plane Fig. 3. Schematic showing locations of trabecular bone columns sectioned from the L5 porcine vertebral body. gitudinal axis of the spinal canal. Six of these pieces (A–F) were cut from trabecular bone along the mid-coronal plane, 4 mm from the posterior wall of the vertebral body. The remaining two (G and H) were cut along the mid-sagittal plane. The middle two specimens of the six in the midcoronal plane (C and D) were chosen as being strictly beneath the NP. This particular configuration and sample size was chosen to maximize the number of samples that could be cut from the vertebral body while care was taken to avoid any cortical bone in the outermost samples. This was governed by the size and shape of the smallest vertebral body. Uniaxial compression was carried out using a Zwick universal testing machine (Zwick GmbH, Ulm, Germany) at a deformation rate of 5 mm/min along the long axis of the specimen. A video extensometer (Messphysik Materials Testing Ltd., Furstenfeld, Austria) was used to gauge specimen displacement. Load–displacement curves were recorded for later data analysis. Each specimen was loaded until a decrease in the load was observed, at which point the load was removed. The yield stress and strain were calculated using a 0.2% offset. The material parameters, including elastic modulus (E), yield stress (ryield) and ultimate compressive stress (rucs), were obtained from calculations using the load–displacement curves. 2.3. Statistical analysis For both studies, statistical analyses were carried out using statistical software (MinitabTM, v.13.32). Statistical variances between regions were determined by one-way analysis of variance (ANOVA). Tukey’s honesty significant difference test was used for post hoc evaluation of differences between groups. A P-value of <0.05 was considered to be statistically significant. 3. Results 4.1. Stress distribution in the IVD The mean CSA of the 10 porcine IVDs was 8.68 cm2 (SD 0.24) and the average IVD height was 5.7 mm (SD 0.2). The porcine endplate revealed a slightly concave curvature shifted posteriorly. The stationary placement of the pressure probe provided identical measurement sites so that stress readings obtained under different loading regimens could be compared. The axial stress recorded in both the AF and NP displayed a closely linear relationship to the applied load. The average intrinsic stress on transducer insertion for all measurement sites was 288.7 kPa (SD 70.5). Thereafter, the mean ratio of stress measured to the theoretical IVD stress was 2.13 (SD 0.43) where theoretical IVD stress is simply the axial force applied divided by the CSA of the IVD. Stresses measured in the NP were on average, slightly lower than those measured in the AF. The mean ratio of NP stress to the theoretical stress was 1.95 (SD 0.19) over the complete loading range. Fig. 4 illustrates the relationship between stress and applied axial load G. Ryan et al. / Clinical Biomechanics 23 (2008) 859–869 863 Fig. 4. Stress across the mid-coronal and mid-saggital planes due to increasing axial load (values reported as mean (+SD) n = 10). at the various positions across the IVD under static compression. In the mid-coronal plane and under no axial load, the stress measured across the IVD was lowest in the outer AF (Positions 1 and 5). Values of stress in the NP and inner AF (Positions 2 and 4) were slightly greater and almost identical. With rising axial load the stress became distributed evenly over the area of the IVD and there is no statistically important difference between the stress at any location across the mid-coronal or mid-sagittal planes above 400 N compression (analysis of variance [ANOVA], P > 0.05). At 800 N the average IVD stress measured 1611.2 kPa (SD 198.4). Increasing axial load coincided with a slight bulging in the annular part of the IVD. Plots of typical stress profiles during dynamic loading are shown in Fig. 5. Also shown is the sequence of movements produced by the testing rig. It is evident that as the testing rig introduces flexion/extension and medial/lateral bending, stresses in the AF rise rapidly when the movement is directed towards the sensor location. Peak stress values always occurred at highest angles of flexion/exten- sion and medial/lateral bending. Stress values below those experienced during pure compressive loading were often noted in the AF when flexion/extension or medial/lateral bending was directed away from the sensor location. For these instances, it may be that the annular tissue lost slight contact with the sensor. A drop in stress was very uncommon in the NP. There was no statistical difference between peak stresses measured for left and right AF positions during ipsilateral and contralateral bending. These findings underline the reproducibility of the technique. Therefore, peak stresses obtained for Positions 1 and 2 were pooled with those of Positions 5 and 4, respectively for data analysis. For the posterior AF, stress peaks were greatest during extension. Similarly, for the anterior AF, stress peaks were greatest during flexion. However, no statistical difference was evident between stress peaks in the posterior and anterior AF. In all specimens, greatest peak stresses were observed in the AF as opposed to the NP (P < 0.05). The peak stresses at each measurement location for the movement sequence are presented in Figs. 6 and 7. Fig. 5. An example of three stress history profiles at various locations within the IVD during dynamic loading of the porcine motion segment. Also shown is the change in angle produced by the testing apparatus, beginning with flexion/extension and followed by lateral bending. 864 G. Ryan et al. / Clinical Biomechanics 23 (2008) 859–869 Fig. 6. Regional peak stress values across the mid-coronal plane recorded during dynamic loading (values reported as mean (+SD) n = 10). Fig. 7. Regional peak stress values across the mid-sagittal plane recorded during dynamic loading (values reported as mean (+SD) n = 10). 4.2. Strength distribution in subdiscal trabecular bone The constant deformation conditions of the uniaxial compressive tests resulted in a mean strain rate of 0.008 s 1 (SD 0.001). The typical load-deformation response involved an initial nonlinear region followed by a linear, elastic region until yield. Mean compressive yield strain was 2.7% (SD 0.7). Loading continued until failure, defined as the first detectable decrease in load. At failure, the mean compressive ultimate strain was 4.2% (SD 1.3) or 1.5% strain post-yield. The mean values of material parameters were: compressive elastic modulus (E): 394.4 MPa (SD 183.2); compressive yield stress (ryield): 11.9 MPa (SD 4.2), and ultimate compressive stress (rucs): 12.8 MPa (SD 4.0). Results obtained for all positions are displayed in Table 1. No macroscopic changes in the specimen appearance were evident, and the microscopic appearance of the specimens was not examined. No significant differences were observed for material parameters (E, rult, ryield) between the cranial and caudal regions in the vertebral body so these values were pooled for statistical significance. Variations in the strength of trabecular bone in relation to anatomical position were, however, observed within each region for all eight vertebral segments that were examined. Statistical analysis revealed that the variations in the material parameters were significant within the eight positions studied (P < 0.05). In order to assess the differences in specimen strength in these regions, the data was separated into the six segments lying along the mid-coronal plane and four segments lying along the mid-sagittal plane. An average of the two central specimens was taken, as these underlie the NP and showed almost identical results. For further statistical analysis the segments were grouped according to their symmetry and their anatomical position into the following sub-groups; specimens A and F, specimens B and E, specimens C and D, and specimens G and H. All material properties tended to be greater on the periphery compared to the central regions. Differences between sub-groups were determined using ANOVA and the corresponding P-value for each material property is reported in Table 2. The most striking differences with respect to anatomical position were found G. Ryan et al. / Clinical Biomechanics 23 (2008) 859–869 865 Table 1 Compressive properties for trabecular bone columns taken from distinct locations within the porcine vertebral body (values reported as mean (SD) n = 10) Property Cranial position A B C D E F G H Young’s modulus (E) (MPa) Yield strength (ryield) (MPa) Ultimate compressive strength (rucs) (MPa) 437.8 (199.3) 13.8 (4.6) 14.9 (3.3) 267.4 (129.5) 10.4 (3.7) 10.5 (3.7) 368.1 (144.7) 10.0 (2.4) 10.7 (2.2) 333.2 (103.2) 10.7 (2.6) 11.3 (2.6) 268.8 (170.8) 9.1 (3.4) 9.8 (3.3) 457.1 (148.5) 12.9 (3.7) 14.7 (3.6) 467.1 (239.8) 14.1 (5.8) 16.8 (6.6) 408.8 (159.4) 13.9 (3.8) 15.7 (3.5) Caudal position Young’s modulus (MPa) Yield strength (ryield) (MPa) Ultimate compressive strength (rucs) (MPa) A B C D E F G H 488.9 (173.7) 15.5 (4.8) 15.2 (2.7) 299.8 (191.9) 9.1 (2.6) 9.6 (2.3) 337.1 (138.5) 10.4 (2.3) 10.6 (1.4) 295.3 (166.2) 9.6 (2.7) 10.8 (1.9) 342.6 (218.8) 9.1 (4.4) 9.7 (2.7) 399.2 (186.4) 13.2 (4.7) 14.3 (3.5) 544.6 (236.0) 13.1 (4.5) 13.9 (2.9) 400.7 (115.4) 14.6 (5.2) 16.1 (3.7) Table 2 Statistical variances between trabecular bone column sub-groups as determined by one-way analysis of variance (ANOVA) Young’s modulus (E) ANOVA: P < 0.001 Tukey’s HSD test B and E C and D G and H * Yield stress (ry) ANOVA: P < 0.0001 Tukey’s HSD test A and F B and E C and D * n/a n/a n/a * * B and E C and D G and H Ultimate compressive stress (ru) ANOVA: P < 0.0001 Tukey’s HSD test A and F B and E C and D * n/a n/a n/a * * * B and E C and D G and H A and F B and E C and D * n/a n/a n/a * * * P < 0.05. for compressive strength with the outer regions, underlying the AF, tending to be stronger than central regions underlying the AF (P < 0.05). 5. Discussion According to Wolff’s law the mechanical properties of the vertebral trabecular bone should reflect the distribution of stresses that exist in the IVD, which correlates with findings of this research. During everyday activities, the porcine spine inevitably undergoes certain flexion/extension and medial/lateral bending. As shown in this study, peak stresses that occur during these physical activities would provide greater stimuli for the underlying bone to undergo adaptive remodeling as to withstand the greater forces present. The trabecular network of the load bearing vertebral bodies, constructed with thick plates and columns in vertical direction and thin horizontal struts, is formed on the basis of these forces (Frost, 1983). A drawback of the study is that motion segments from different spines were used for measuring the IVD stress and the strength of subdiscal trabecular bone. This was necessary as the vertebral bodies of the motion segments used in the stress distribution study needed to be cut in order to properly locate the NP at the centre of rotation of the testing rig. Therefore, bone from these vertebral bodies could not be sectioned and mechanically tested. However, because interspecimen variation in age, weight, and size of porcine motion segments should be low, we suggest that of strength distribution of vertebral trabecular bone between samples would be consistent. From the mechanical point of view, a quadruped is a complex system. There are different types of joints, and the distribution of the muscles and their activity during movements are largely unknown. Due to dominant muscle and ligament forces, the quadrupedal spine is mainly loaded under axial compression similar to the human spine, although it is almost impossible to determine the actual loads in the living systems (Smit, 2002). In examining the human motion segments in vitro using similar techniques to the present study, axial loads ranging from 600 N to 2 kN have been employed (Pollintine et al., 2004; Steffen et al., 1998). However, because the width of the porcine L5 endplate is approximately 0.8 times smaller than the human equivalent (Dath et al., 2007; Panjabi et al., 1992), and the average animal weight is approximately 95 kg, we estimated that the loading range (0–800 N) tested in this study provided an appropriate estimate for the axial loading experienced in daily life. During the different forms of quadrupedal locomotion, axial torsion, flexion-extension, and lateral bending moments are important loads that work on the spine. It has been demonstrated that the range of motion of lumbar segments of ovine and bovine spines is similar to that of human spines (Wilke et al., 1997, 1996a,b). For the ovine spine, the range of motion for the L4–L5 motion segment was approximately 5° in extension, 4° in flexion and 4.5° in lateral bending (Wilke et al., 1997). For the bovine spine, the range of motion in flexion 866 G. Ryan et al. / Clinical Biomechanics 23 (2008) 859–869 in the lumbar levels ranged from an average of 2.8° for L1– L2 to 5.0° for L5–L6, with a similar range of motion for extension (Wilke et al., 1996a,b). In this study, we employed a maximum angle of 4o for flexion/extension and lateral bending movements and on inspection found no visible damage to the tissues, which suggests that the motion segments remained within their physiological range of motion. During these movements we employed an axial compressive load of 300 N. This load was found to be an appropriate level in previous biomechanical studies using porcine spines (Keller et al., 1990). Although it is smaller than the maximum force that was employed during pure axial compression, far greater localised stresses were generated in the IVD during asymmetric loading. The initial application of the guiding needle was necessary to facilitate an easier entry of the needle transducer and to prevent artifacts caused by contact stresses. The height of the porcine IVD was found to be approximately 5.7 mm, which is significantly smaller than that of the human IVD which was found to be approximately 10.8 mm for healthy young working males (Nissan and Gilad, 1986). We found that the introduction of the needle transducer into the IVD created an almost equal rise in pressure in both the NP and AF. A comparison of the estimated mean stress across the IVD to the stresses in the NP and AF provides insight for interpreting the stress distribution across the IVD. The net stress passed from the annulus to the endplate is the combined effect of the tension of the annulus fibers and the stress within the matrix material. Brinckmann and Grootenboer (1991) obtained measurements from isolated human IVDs (with posterior elements removed) and found that the pressure in the NP was on average 1.68 times the estimated mean stress over a range of compression from 300 to 2000 N. For the porcine spine we found a slightly higher ratio of approximately 2.13. This is in fact an underestimation of the ratio as we did not take into account the load resisted by the neural arch. In the human spine the NP comprises about 30% the IVD area (Brinckmann and Grootenboer, 1991). We found that the NP in the porcine spine consisted of approximately 23% of the CSA, and therefore would experience increased tension from the annular fibers compared to the human spine. We observed an almost even distribution of stress across the porcine IVD during pure compressive loading while the spinal motion segment maintained an upright posture. In comparison with the human spine, this finding is in contrast with early research by Nachemson and Morris (1964), who suggested that under pure compressive loading conditions, vertical stresses in the AF are half those in the NP. More recent studies however, are in good agreement with our findings and show that there is a one-to-one relationship between the stress in the NP and the AF. Horst and Brinckmann (1981) analyzed the distribution of axial stress under the IVD of human lumbar and thoracic motion segments with the aid of five miniature piezoelectric pressure transducers placed just below the vertebral endplate. Results indicated that the stress distribution depends essentially on the state of degeneration of the IVD and on the relative position of the adjacent endplates. Ranu (1990) also found a one-to-one relationship between the two areas of the IVD, by placing two different pressure transducers in the AF and NP of cadaveric lumbar motion segments which were then loaded to failure. Similar results were reported by McNally and Adams (1992), using a technique they pioneered and is known as ‘stress profilometry’, in which a needle pressure transducer is pulled incrementally across the mid-sagittal plane of the IVD. During asymmetrical loading, we found that peak stresses predominantly occurred in the AF. We found that pressure within the nucleus was relatively insensitive to flexion/ extension and lateral bending. On occasion, a rise in stress within the NP was noted. However, these stresses were not to the same level as those experienced in the AF. Some needle bending due to asymmetrical loading cannot be excluded. However, visual inspection of the pressure signal during manual needle bending showed only marginal effects of bending. Our findings are in good agreement with several studies analyzing IVD stress distribution due to asymmetrical loading in the human spine. Ongoing research by Adams and co-workers has revealed the presence of peak stresses in the posterior AF due to IVD degeneration (Adams et al., 1996a,b, 2000a,b), after creep loading (Adams et al., 1996a,b), and due to minor damage of the IVD (Adams et al., 2000a,b). Steffen et al. (1998) performed simultaneous multilocalised IVD pressure measurements in human cadaveric lumbar spines to gather information on stress distribution during asymmetrical loading. For all loading conditions, stress gradients were directed towards the NP. Peak stresses were recorded in the posterolateral inner AF, during flexion and when combined with axial rotation. Several of the aforementioned studies predominantly show peak stresses arising in the posterior AF. In this study, we found no statistical difference between pressures recorded in the posterior and anterior AF. This apparent contradiction with previous research may be explained by the inherent differences between the anatomical features of the porcine vertebral spine and the human spine. Compared to the human lumbar spine, there are a number of anatomical differences in the porcine lumbar spine, including wider pedicles, longer body height and especially the interlocking facet joints (Cotterill et al., 1986). It seems plausible that the strong interlocking relationship of the facet joints performs as a mechanical hinge and in doing so acts to stress shield the posterior AF during extension. The effect to which the vertebral endplate alters the load transfer process is important in analyzing the relationship between IVD stress distribution and subdiscal trabecular bone strength. The vertebral endplate is a thin layer of dense, subchondral bone adjacent to the IVD. Its density and thickness have been shown to increase toward the vertebral periphery (Grant et al., 2001; Roberts et al., 1997). In studying the vertebral endplate curvature of different species, Langrana et al. (2006) showed that the canine G. Ryan et al. / Clinical Biomechanics 23 (2008) 859–869 and chimpanzees, i.e. the quadrupeds, have a different curvature of their upper endplates compared with those in humans (bipeds). Finite element analysis predicted that the shape of the endplate alters the distribution of loads transferred along the spine. The stress distribution varied as the location of the maximum curvature shifted from the centre to a more posterior position. The stresses in the vertebral core were found to decrease, with the shell taking more of the load, which is due to a redistribution of load to the periphery. In the porcine spine we found that the endplate possessed a slightly concave curvature shifted posteriorly, which may explain the distribution of bone strength found in this study. The strength of the subdiscal trabecular bone was not homogenous inside the vertebral body. We found that the two central specimens (regions C and D), which correspond to sections overlying the NP, had lower strength and modulus values compared to specimens approximately underlying the AF. A number of studies have reported regional variation in trabecular bone strength within the vertebral body. Grant et al. (2001) and later Oxland et al. (2003) performed a series of indentation tests at predetermined locations across the lumbar vertebral body with the endplates both intact and removed. They found that for both cranial and caudal endplates, the posterior region was stronger than the anterior, and the periphery stronger than the centre, with the strongest points in the posterolateral test sites just in front of the pedicles. With endplate removal, although there was a 33% decrease in failure load for indentation testing, the basic failure pattern remained the same, with the periphery stronger than the centre. In contrast to these findings, Keller et al. (1989) found that bone underlying the NP is stronger than that underlying the AF when studying the compressive properties of human lumbar vertebral trabecular bone. For non-degenerated IVDs, they found that the ratio of strength of bone overlying the NP to bone overlying the AF was 1.25. Similarly, Lin et al. (1997), in a porcine model, found that the ratio of strength of bone overlying the NP to that overlying the AF was approximately 1.16. Both authors equate their findings to greater stress in the NP as opposed to the AF, which we found not to be the case for the porcine spine, especially when asymmetrical loading was applied. It has been reported that the structure of the vertebral body is closely related to the degenerated or aged status of the IVD (Adams and Roughley, 2006; Adams et al., 1996a,b, 2006; Keller et al., 1989, 1993; Simpson et al., 2001). In the human spine, healthy IVDs contain a large and highly hydrated NP whereas degenerative IVDs are associated with a loss of fluid and associated height (Horst and Brinckmann, 1981). The young healthy IVD acts to spread the force evenly over its area (Adams et al., 2006). With age, the reduction in size of the hydrostatic compressive region coincides with the appearance of peak stresses in the AF (Adams et al., 1986, 1996a,b). Furthermore, studies performed by Adams et al. have shown that a reduction in IVD height caused by either excessive com- 867 pressive loading or prolonged creep loading can produce peak stresses in the AF, usually posteriorly to the NP (Adams et al., 1996a,b, 2000a,b). In this study, all porcine spines tested were of good quality with no apparent IVD degeneration. However, heights recorded for porcine IVDs were considerably smaller than what is normal in human samples, and the AF comprised a much greater fraction of the total IVD area compared to the human spine. These two factors appear to be responsible for the peak stresses recorded in the AF during asymmetrical loading. It appears that the trabecular bone of the young porcine spine can adapt to withstand the greater forces generated in the AF during asymmetrical loading better than how the vertebral bone of the aged human spine might respond to its changing loading environment. Bone loss due to inactivity, especially in the elderly is a common finding (Lunt et al., 2001; Nguyen et al., 2007). However, it has also been demonstrated that bone growth and adaptation has a reduced responsiveness to mechanical stimulus in the elderly (Bassey et al., 1998). It is possible that a combination of these traits can predispose the thoracolumbar spine of the elderly to anterior vertebral fractures when the spine is flexed (Adams et al., 2006), which seems not to be the case for the young porcine spine. Findings of increased stresses in subdiscal trabecular bone underlying the AF suggest that adaptive bone remodeling has occurred to withstand the greater forces present in this region. It is widely understood that there are various anatomical and biomechanical differences between humans and even the closely related primates. Therefore, animal cadaveric analyses may not directly explain phenomena associated with human physiology. From a clinical perspective, results of regional distributions in trabecular strength of porcine vertebral bodies provide little useful information for the treatment of age-related degeneration of the human spine or the design of implants meant for human use. However, once an implant has been designed, animal models are widely used to investigate the biologic as well as mechanical behavior of the implants. Interpretation of data from such studies usually considers the limitations related to the mismatch of properties between the human and animal tissues. This study raises awareness and identifies such limitations. 6. Conclusions In the porcine lumbar spine we found that asymmetrical loading generated peak stresses in the periphery of the IVD, namely the AF. Assuming asymmetrical loading is part of everyday activities, this has implications on bone mass adaptations in accordance with the magnitude and direction of the forces that are applied to them over time. We demonstrated that bone underlying the AF is significantly stronger than bone underlying the NP. Although these two features cannot be directly related, this suggests that there is a correlation between the stress in the IVD and strength of underlying trabecular bone. 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