Molecular Interactions between Collagen and Aggrecan from...
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Molecular Interactions between Collagen and Aggrecan from the Cartilage Extracellular Matrix
by
Fredrick P. Rojas
Submitted to the Department of Materials Science and Engineering
in Partial Fulfillment of the Requirements for the Degree of
Bachelor of Science
at the
Massachusetts Institute of Technology
June 2011
© 2011 Fredrick P. Rojas All rights reserved
The author hereby grants to MIT permission to reproduce and to
distribute publicly paper and electronic copies of this thesis document in whole or in part in any medium now known or hereafter created
Signature of Author ............................................................................................................................ Department of Materials Science and Engineering
May 12, 2011
Certified by ........................................................................................................................................ Christine Ortiz
Professor of Materials Science and Engineering Thesis Supervisor
Certified by ........................................................................................................................................
Alan J. Grodzinsky Professor of Biological, Electrical and Mechanical Engineering
Thesis Supervisor
Accepted by ....................................................................................................................................... Lionel C. Kimerling
Thomas Lord Professor of Materials Science and Engineering Chairman, Undergraduate Thesis Committee
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Molecular Interactions between Collagen and Aggrecan from the Cartilage Extracellular Matrix
by
Fredrick P. Rojas
Submitted to the Department of Materials Science and Engineering on on May 6, 2011 in Partial fulfillment of the
requirements for the Degree of Bachelor of Science in Materials Science and Engineering
Abstract
In this study, colloidal force spectroscopy was utilized to quantify interactions between collagen and aggrecan in physiological and non-physiological aqueous solutions. An aggrecan-functionalized probe tip (R ~ 2.5µm) was indented ~500nm into the surface of a native collagen network, composed of trypsin-treated, proteoglycan-depleted cartilage. The resulting force-indentation curves were used to calculate the adhesion force and adhesion energy of the molecular interaction. Heterogeneous long-range adhesion was observed up to ~ 2.5 µm extension upon retraction after compressing the tip into the sample for a given surface dwell time, t. The adhesion force showed an asymptotic nonlinear increase with t, reaching a maximum value of 3.1 ± 0.2 nN at t = 60 s. Aggrecan-collagen interactions displayed a dependence on ionic strength, with a maximum adhesion force of 4.3 ± 0.3 nN at 1.0 M NaCl (t = 30 s). In addition, aggrecan-collagen interactions showed [Ca2+]-dependence with a maximum adhesion force of 7.4 ± 0.3 nN with a [Ca2+] = 20 mM (t = 30 s, 0.15 M). Molecular interactions between aggrecan and collagen are important in determining structural integrity of the cartilage extracellular matrix and its biological functions, such as energy dissipation, osmotic swelling and hydraulic permeability.
Thesis Supervisor: Christine Ortiz Title: Professor of Materials Science and Engineering Thesis Supervisor: Alan J. Grodzinsky Title: Professor of Biological, Electrical and Mechanical Engineering
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Table of Contents Abstract ...................................................................................................................................... 2 List of Figures and Tables ......................................................................................................... 4 1. Background and Motivation ................................................................................................. 7 1.1 Cartilage Collagen Network .......................................................................................... 7 1.2 Aggrecan .......................................................................................................................... 9 1.3 Reported Collagen-Aggrecan Binding Studies .......................................................... 13 2. Experimental Methods ........................................................................................................ 15 2.1 Sample Preparation ...................................................................................................... 15 2.2 Colloidal Force Spectroscopy ...................................................................................... 16 2.3 Data Processing and Analysis ...................................................................................... 18 3. Results ................................................................................................................................... 20 3.1 Effect of Surface Dwell Time on Aggrecan-Collagen Adhesion ............................... 21 3.2 Effect of Ionic Strength on Aggrecan-Collagen Adhesion ........................................ 24 3.3 Effect of Ca2+ on Aggrecan-Collagen Adhesion ......................................................... 27 4. Discussion ............................................................................................................................. 31 5. Conclusion ............................................................................................................................ 35 6. Acknowledgements .............................................................................................................. 36 7. References ............................................................................................................................. 37
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List of Figures and Tables
Figure 1-1 Schematic representation of the collagen type II, IX, and XI hetero-fibrillar network. Type XI collagen is found in the interior of the type II collagen fibril, while type IX collagen is located throughout the surface of the fibril and crosslinks other type II and IX collagen fibrils (6). ................................................................................................................................. 8
Table 1-1 Chemical properties and corresponding amino acid compositions of type II collagen from adult porcine articular cartilage at physiological conditions (adapted from (9, 10)). ..... 8
Figure 1-2 Schematic depicting the varying collagen fiber orientations found in cartilage (11). .. 9
Figure 1-3 Schematic depicting the regions of aggrecan and the structural subunits of glycosaminoglycan chains (adapted from (15)). .................................................................... 10
Figure 1-4 (a) Schematic of colloidal force spectroscopy experiment on retraction involving interactions between an aggrecan-functionalized planar substrate and an end-grafted aggrecan spherical probe tip. (b) An example of the resulting data from the experiment shown in (a) plotting the adhesive energy as a function of the time held at maximum compressive load (surface dwell time) and bath ionic strength. These data indicate that aggrecan is capable of undergoing self-adhesion given a sufficient compressive hold time. Statistically significant adhesion values were observed as a function of surface dwell times and ionic strength (4). ............................................................................................................ 12
Figure 1-5 Schematic showing possible binding mechanisms between neighboring GAG chains while in solution. Dashed arrows represent possible hydrogen bonding, while an example of calcium ion-bridging is shown in the square (adapted from (22)). ........................................ 13
Figure 1-6 Possible supramoleular assemblies found within the cartilage extracellular matrix. Illustration showing possible pathways of interaction between aggrecan and collagen, along with known dissociation constants (25). ................................................................................ 14
Figure 2-1 Tapping mode height images of (a) single fetal epiphyseal aggrecan macromolecule on an atomically flat mica surface (adapted from (30)) and (b) air-dried calf femoral condyle knee cartilage surface with aggrecan digested, where the porous structure collapsed while the nanoscale structural features of the collagen fibrils were retained. (c) Schematic of interactions between the collagen network on cartilage surface and the aggrecan end-functionalized spherical probe tip simulating the in vivo situation (3,4,20). ......................... 17
Figure 2-2 Calibration curves performed on a clean glass slide for an aggrecan functionalized tip in 1 mM and 1 M ionic strength (pH ~5.6). ........................................................................... 18
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Figure 2-3 Characteristic force-indentation curve of the indentation of a collagen sample with an aggrecan-functionalized probe tip (t =30 s, PBS (IS =0.15 M), pH ~6.4), with appropriately marked variable definitions (35). ........................................................................................... 19
Figure 3-1. Characteristic force-indentation curves for the indentation (500 nm indentation depth, surface dwell time of t = 30, 0.150 M NaCl, pH ~6.4) of trypsin-treated cartilage samples with colloidal probe tips functionalized with either aggrecan or OH-SAM. ......................... 21
Figure 3-2. Characteristic force-indentation curves for the indentation of trypsin-treated cartilage samples (500 nm indentation depth, 0.150 M (PBS), [Ca2+]= 0.0 mM, pH ~6.4) with colloidal probe tips functionalized with aggrecan for surface dwell times of 10 and 30 seconds. .................................................................................................................................. 22
Figure 3-3 The force of adhesion versus surface dwell time for the indentation (500 nm indentation depth, 0.150 M (PBS), [Ca2+]= 0.0 mM, pH ~6.4) of trypsin-treated cartilage samples with colloidal probe tips functionalized with either OH-SAM or aggrecan. Error bars correspond to the standard error of measure (n = 75). ................................................... 23
Figure 3-4 The energy of adhesion versus surface dwell time for the indentation (500 nm indentation depth, 0.150 M (PBS), [Ca2+]= 0.0 mM, pH ~6.4) of trypsin-treated cartilage samples with colloidal probe tips functionalized with either OH-SAM or aggrecan. Error bars correspond to the standard error of measure (n = 75). ................................................... 24
Figure 3-5 Characteristic force-indentation curves for the indentation (500 nm indentation depth, t = 30 s, ([Ca2+]= 0.0 mM, pH ~5.6) of trypsin-treated cartilage samples with colloidal probe tips functionalized with aggrecan in solution ionic strengths of 0.15 M NaCl and 1.0 M NaCl. ...................................................................................................................................... 25
Figure 3-6 The force of adhesion versus ionic strength for the indentation (500 nm indentation depth, t = 30 s, [Ca2+]= 0.0 mM, pH ~5.6) of trypsin-treated cartilage samples with colloidal probe tips functionalized with OH-SAM or aggrecan. Error bars correspond to the standard error of measure (n = 50). ...................................................................................................... 26
Figure 3-7 The energy of adhesion versus ionic strength for the indentation (500 nm indentation depth, t = 30 s, [Ca2+]= 0.0 mM, pH ~5.6) of trypsin-treated cartilage samples with colloidal probe tip functionalized with OH-SAM or aggrecan. Error bars correspond to the standard error of measure (n = 50). ...................................................................................................... 27
Figure 3-8 Characteristic force-indentation curves for the indentation (500 nm indentation depth, t = 30 s, IS = 0.15 M, pH ~5.6) of trypsin-treated cartilage samples with colloidal probe tips functionalized with aggrecan for [Ca2+]= 0.0 mM and 20 mM. ............................................ 28
Figure 3-9 The force of adhesion versus [Ca2+] for the indentation (500 nm indentation depth, t = 30 s, IS = 0.15 M, pH ~5.6) of trypsin-treated cartilage samples with colloidal probe tips
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functionalized with OH-SAM or aggrecan. Error bars correspond to the standard error of measure (n = 40). ................................................................................................................... 29
Figure 3-10 The energy of adhesion versus [Ca2+] for the indentation (500 nm indentation depth, t = 30 s, IS = 0.15 M, pH ~5.6) of trypsin-treated cartilage samples with colloidal probe tips functionalized with OH-SAM or aggrecan. Error bars correspond to the standard error of measure (n = 40). ................................................................................................................... 30
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1. Background and Motivation
Cartilage tissue sustains loads and absorbs shocks between joints during biomechanical
motion. It is a highly hydrated macromolecular fiber-reinforced composite, in which the
extracellular matrix (ECM) is composed of a fibrillar collagen network surrounded by a matrix
of highly negatively charged brush-like aggrecan proteoglycans (1). Currently, relatively little is
known about the molecular details of the interactions between two major cartilage extracellular
matrix (ECM) macromolecular components, the collagen network and the highly negatively
charged aggrecan moiety. This interaction is hypothesized to play a structural and biomechanical
functional role in determining the integrity and tissue function of cartilage (1,2). Toward this end,
in order to elucidate the mechanistic origins of cartilage properties from its molecular
components and structure, we propose to quantify the molecular interactions between aggrecan
and the collagen network under physiologically relevant conditions using atomic force
microscope (AFM)-based colloidal force spectroscopy (3).
1.1 Cartilage Collagen Network
Approximately 60 wt. % of the solid mass found in articular cartilage is composed of
collagen, with type II collagen being the major constituent (4,5). Within a single collagen fibril,
type II collagen is copolymerized in the interior on a template of type XI collagen, while the
fibril surface contains type IX collagen that is capable of cross-linking with type II and IX
collagen neighboring structures (Figure 1-1) (5,6).
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Figure 1-1 Schematic representation of the collagen type II, IX, and XI hetero-fibrillar network. Type XI collagen is found in the interior of the type II collagen fibril, while type IX collagen is located throughout the surface of the fibril and crosslinks other type II and IX collagen fibrils (6).
The molecular structure of collagen is defined as a triple helix that has the amino acid
sequence of (Gly-X-Y) (7). The amino acid residues at positions X and Y are exposed to the
surrounding solvent and are fully capable of intramolecular and intermolecular interactions (7).
Furthermore, as indicated in Table 1-1, Type II collagen possesses both positively and
negatively charged amino acids. Hence, molecular adhesion with the negatively charged
glycosaminoglycans of aggrecan is a possibility, through van der Waals interactions, hydrogen
bonding, ionic bonding, etc. (8,9).
Chemical Property Amino Acid Composition (Residues/1000 residues)
Positive 92 Negative 138
Polar 46 Nonpolar 542
Hydrophobic 182 Table 1-1 Chemical properties and corresponding amino acid compositions of type II collagen from adult porcine articular cartilage at physiological conditions (adapted from (9, 10)).
In addition, cartilage consists of three distinct regions, each containing a preferred
collagen fibril orientation and morphology (Figure 1-2). The bottom layer consists of a calcified
region and provides the connection from articular cartilage and bone. In the deep zone, the
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collagen fibers are arranged perpendicular to the subchondral bone. Through the middle zone the
collagen fibers slowly transition to the orientation found in the superficial zone, which is a
layered conformation that is tangential to the articular surface (lamina splendens) (11,12). In this
study, the collagen network was harvested from the top superficial layer of calf knee cartilage,
which remained intact during the microtoming and subsequent chemical treatments to remove
proteoglycans. In the superficial layer, the long fiber axis of collagen fibrils are randomly
oriented in the plane perpendicular to the surface (13).
Figure 1-2 Schematic depicting the varying collagen fiber orientations found in cartilage (11).
1.2 Aggrecan
Aggrecan is the most abundant proteoglycan in cartilage (1) and a major constituent of
the cartilage extracellular matrix, making up approximately 30% of its dry weight (14). As
shown in Figure 1-3, aggrecan consists of a core protein with three globular domains (G1, G2,
and G3) and a “brush-like” region with densely packed chondroitin sulfate glycosaminoglycans
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CS-GAGs) and keratan sulfate glycosaminoglycans (KS-GAGs) covalently bonded to the core
(1,15). These GAG chains are composed of an alternating sequence of N-acetylgalactosamine
and glucuronic acid, and are negatively charged under physiological conditions. Each aggrecan
molecule is composed of ~100 CS-GAG chains that are densely packed along its core protein,
and are ~40 nm in contour length (16). There are a total of ~104 negative charges per aggrecan
macromolecule [15, 17]. The highly negatively charged aggrecan molecules create a surrounding
of high osmotic pressure that adds to the unique biomechanical properties of cartilage in
compression and shear (1,2).
Figure 1-3 Schematic depicting the regions of aggrecan and the structural subunits of glycosaminoglycan chains (adapted from (15)).
The charged GAG chains also provide a source of electrical double layer repulsive
interactions within and between aggrecan molecules. The implications of the electrical double
layer in an environment with electrolytes are described by the Poisson-Boltzmann equation
∇!Ψ = !! sinhΨ (1)
Ψ = ! ! !! !
= ! ! !! !
(2)
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where Ψ is the reduced surface potential, ! is the charge number, ! is Faraday’s constant, ! is
the universal gas constant, ! is the absolute temperature, and ! is the inverse Debye screening
length (3, 18, 19). The Debye Length (!!!) is the distance at which the potential decays to 1 !
of its initial value. For electrostatic interactions, as in the case of the GAG chains in aggrecan,
the full range of effect is approximated as ~5!!!. The Debye-Huckel Approximation provides a
linear approximation for charged surfaces to the Poisson-Boltzmann equation and defines the
Debye length as
!!! = ! ! !! !!!!!!
(3)
where !! is the ionic strength of the solution and ! is the permittivity of the solution. The extent
of potential interactions depends only on properties of the bath solution. Of interest is the fact
that increasing the ionic strength decreases the extent of long-range repulsion between two
charged surfaces (3, 18, 19).
In previous nanomechanical studies, we have shown that aggrecan provides compressive
and shear stiffness via electrostatic and steric repulsion between its glycosaminoglycan (GAG)
side chains (3,20,21) and can undergo molecular self-adhesion after compression, which is
hypothesized to be important for the self-assembled architecture and structural integrity of the
cartilage matrix (22). Recently, these nanomechanical force spectroscopy experiments analyzed
interactions between an aggrecan-functionalized planar substrate and an end-grafted aggrecan
spherical probe tip during retraction (Figure 1-4).
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Figure 1-4 (a) Schematic of colloidal force spectroscopy experiment on retraction involving interactions between an aggrecan-functionalized planar substrate and an end-grafted aggrecan spherical probe tip. (b) An example of the resulting data from the experiment shown in (a) plotting the adhesive energy as a function of the time held at maximum compressive load (surface dwell time) and bath ionic strength. These data indicate that aggrecan is capable of undergoing self-adhesion given a sufficient compressive hold time. Statistically significant adhesion values were observed as a function of surface dwell times and ionic strength (4).
In accordance with equation (3), aggrecan self-adhesion was found to have a dependence
on ionic strength of the liquid medium: experiments performed in the presence of calcium ions
measured a nearly four-fold increase in adhesion. These effects were believed to be the result of
ion-bridging of multivalent ions between the monovalent negative charges found in the GAG
chains as depicted in Figure 1-5 (22). As is evident in Figure 1-3 and Figure 1-5, GAG chains
consist of non-polar sugar rings with the following function groups: three hydroxyl (polar), one
sulfate (polar), one carboxyl (polar), and one methyl (nonpolar) (1, 22). This would indicate that
aggrecan is also capable of van der Waals and hydrophobic interactions through its nonpolar
regions and capable of hydrogen bonding through its polar functional groups.
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Figure 1-5 Schematic showing possible binding mechanisms between neighboring GAG chains while in solution. Dashed arrows represent possible hydrogen bonding, while an example of calcium ion-bridging is shown in the square (adapted from (22)).
1.3 Reported Collagen-Aggrecan Binding Studies
Individual chondroitin sulfate E glycosaminoglycan chains were previously reported to
bind to type II collagen, under physiological pH and varying salt concentrations conditions, with
an equilibrium dissociation constant of 39 nM (23). In addition, isolated segments of keratin
sulfate-rich of aggrecan domains have been found to have a dissociation constant of 1.1 µM with
type I and isolated type II collagen (24), via peptide-collagen interactions.
Recent work also indicates that aggrecan-collagen interactions may be assisted through
two adaptor proteins, matrilin-3 and cartilage oligomeric matrix protein (COMP) (Figure 1-6)
(25). The collagen type II affinity of COMP in the presence of divalent ions was found to have a
dissociation constant of ~10-9 M (26). COMP has also been observed to have a significant
CS-GAG
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interaction with matrilin in the form of a dissociation constant on the order of 10-9 M (27).
Furthermore, in addition to interactions with collagen, matrilin is also capable of binding
aggrecan, which may promote the collagen-aggrecan interactions in vivo via collagen-COMP-
matrilin-aggrecan interactions (28, 29). A future endeavor of this project is to determine whether
this adaptor-assisted interaction between aggrecan and collagen is more physically relevant than
the current aggrecan-collagen model.
Figure 1-6 Possible supramoleular assemblies found within the cartilage extracellular matrix. Illustration showing possible pathways of interaction between aggrecan and collagen, along with known dissociation constants (25).
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2. Experimental Methods
The molecular interactions between aggrecan and the collagen network from the cartilage
ECM were directly measured using colloidal force spectroscopy in aqueous solutions. Aggrecan
was chemically end-grafted to a micrometer-sized spherical probe and the collagen network was
prepared via enzymatic degradation of the superficial region of intact cartilage tissue, using prior
established protocols (3, 22). The functional form of the interaction profile (force versus distance)
on approach and retraction was analyzed and the adhesion force and energy was measured in
physiological and non-physiological aqueous electrolyte solution conditions as a function of
surface dwell time (t), ionic strength (IS), and calcium ion concentration ([Ca2+]). As a means of
comparison, spherical probes that were functionalized with hydroxyl self-assembled monolayers
(OH-SAM) were also tested under the same conditions.
2.1 Sample Preparation
Disks with intact cartilage surface were harvested from the femoropatellar groove of 1 –
2 week old bovine calves by microtoming off the top 1 mm thick layer of 6 mm cartilage plugs,
followed by 0.1 mg/ml trypsin (0.15 M NaCl, 0.05 M sodium phosphate, pH 7.2) digestion for 12
hours at 37°C. The residual plug consisted of an intact collagenous matrix that was devoid of
nearly all non-collagenous components (30), without introducing any significant structural
changes to the fibrillar network either microscopically (31) or macroscopically (32).
Aggrecan was extracted from fetal bovine cartilage that was obtained from the epiphyseal
growth plate region. Aggrecan fractions (A1A1D1D1) were purified through dialysis using 500
volumes of 1M NaCl and deionized water (16). The synthetic cross-linker dithiobis
(sulfosuccinimidyl propionate) (DTSSP) was added to an aggrecan aqueous solution and reacted
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with aggrecan to form disulfide bonds at the N-terminus end of the aggrecan core proteins.
Dithiothreitol (DTT) was then used to reduce the disulfide bonds to thiol bonds. Thereafter, the
thiol functionalized aggrecan was filtered and diluted to a 1 mg/mL concentration in deionized
water. Gold-coated colloidal spherical probe tips (R = 2.5 µm, nominal spring constant k = 0.5
N/m, Novascan) were end-functionalized with aggrecan by immersion into 100 µL 1 mg/mL
thiol-functionalized aggrecan solution for 48 hours (3). The thiol-gold bonding between the
aggrecan and the colloid resulted in an aggrecan packing density ~50 mg/mL, within the
physiological concentration in the cartilage ECM (3). Control experiments utilized a probe tip
functionalized with a hydroxyl-terminated self-assembled monolayer (OH-SAM, 11-
mercaptoundecanol, HS(CH2)11OH). Identical gold-coated colloidal spherical probe tips were
functionalized by immersion into 5mg/mL ethanol solution of OH-SAM.
2.2 Colloidal Force Spectroscopy
Given that the type II collagen fibrils are randomly aligned in the 2D surface plane within
superficial zone of cartilage (Figure 2-1b) interactions between the aggrecan-depleted cartilage
disk with the intact surface present and the aggrecan functionalized spherical tip can accurately
mimic the interactions between these two components in vivo, without the interference of
artifacts introduced by the disassembled collagen fibrils from the middle-zone cartilage due to
microtoming, (Figure 2-1c) (11). Adhesion between the 2D collagen network and the end-
attached aggrecan layer was measured using the 3D molecular force probe (MFP-3D, Asylum
Research) in electrolyte aqueous solutions at varying ionic strengths (0.01 to 1 M NaCl, with or
without 2 mM [Ca2+]), as seen in Fig. 2-1. Differing the surface holding time conditions from 0
to 60 seconds between the aggrecan tip and collagen substrate at a constant indentation depth
(~500 nm) were also tested via the indenter mode. The cantilever deflection sensitivity (nm/V)
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was calibrated on a hard mica surface, where the cantilever deflection equals the Z-piezo
displacement in the contact region. The thermal oscillation method was applied to determine the
actual cantilever spring constant (33). The zero contact point was determined via methods
discussed previously (34).
Figure 2-1 Tapping mode height images of (a) single fetal epiphyseal aggrecan macromolecule on an atomically flat mica surface (adapted from (30)) and (b) air-dried calf femoral condyle knee cartilage surface with aggrecan digested, where the porous structure collapsed while the nanoscale structural features of the collagen fibrils were retained. (c) Schematic of interactions between the collagen network on cartilage surface and the aggrecan end-functionalized spherical probe tip simulating the in vivo situation (3,4,20).
As mentioned earlier, ionic strength of the liquid medium has an effect on the long-range
repulsion of aggrecan. During calibrations of aggrecan functionalized cantilever tips, force
spectroscopy was preformed on glass slides, which acted as charged surfaces. Figure 2-2 depicts
two calibration curves performed on a clean glass slide for an aggrecan-functionalized tip in 10.0
mM and 1.0 M NaCl monovalent ion solution. In accordance with Equations (1-3), higher ionic
strength hindered long range repulsion by decreasing the Debye length, allowing the probe tip to
approach closer to the glass slide before significant cantilever bending. Similar calibration curves
were used to ensure that aggrecan was indeed on the surface of the colloidal probe tip before
indentation experiments were performed (18). This test was also performed in between
experimental sets as a measure of sample integrity. Aggrecan functionalized probe tips that lost
the long-range repulsion under low ionic strength conditions were replaced.
100 nm 300 nmNative Collagen Network
(a) (b) aggrecan(c)
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Figure 2-2 Calibration curves performed on a clean glass slide for an aggrecan functionalized tip in 10 mM and 1 M ionic strength (pH ~5.6).
2.3 Data Processing and Analysis
All data collected from the experiments above were exported to ASCII format and
processed in MatLab (Version 7.1, MathWorks). We quantified the maximum adhesion force,
adhesion distance and adhesion energy from each pair of loading-unloading curves. Relevant
statistical tests (e.g. student’s t-test, analysis of variance, etc.) were performed to examine the
tested effects, including the surface dwell time, ionic strength, and presence of Ca2+. Once the
adhesion between aggrecan and collagen was quantified, molecular interaction theories that
relate the macromolecular components and structures to the interaction magnitudes could be
implemented to explain the observations and elucidate the molecular origins of collagen-
aggrecan interactions.
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The combination of long range adhesion between aggrecan and collagen during retraction
and the viscoelastic properties of cartilage made it difficult to fit the experimental data collected
for this project to established contact mechanic models to extract adhesion values. For this study,
we utilized the criterion as stated by Lee, which is shown in Figure 2-3 (35). The adhesion
energy was estimated as the area between the loading and unloading curve that corresponds to a
negative force and the force of adhesion was defined as the greatest absolute force during
retraction.
Figure 2-3 Characteristic force-indentation curve of the indentation of a collagen sample with an aggrecan-functionalized probe tip (t =30 s, PBS (IS =0.15 M), pH ~6.4), with appropriately marked variable definitions (35).
-‐3000 -‐2500 -‐2000 -‐1500 -‐1000 -‐500 0 500 1000-‐10
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Fad
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3. Results
We utilized atomic force microscopy to quantify interactions between collagen and
aggrecan in various aqueous environments. Characteristic force-indentation interaction curves
for the different aqueous solutions are shown below. The adhesion force and energy between
aggrecan and collagen were measured as a function of surface dwell time, ionic strength, and
calcium ion concentration ([Ca2+]). As a means of comparison, we also measured the interactions
between collagen and a hydroxyl terminated self-assembling monolayer (OH-SAM). For all
experimental data sets, each data corresponds to the use of 2-3 bovine joints with a total number
of indentations between 40-75. Two-way analysis of variance (ANOVA) of the data sets showed
no significant differences in adhesion between samples (ANOVA, p > 0.1).
Figure 3-1 depicts characteristic force-indentation curves for the indentation of a
proteoglycan-depleted cartilage sample with both aggrecan functionalized and OH-SAM
functionalized spherical probe tips (500 nm indentation depth, surface dwell time of t = 30, 0.150
M NaCl). The results of these experiments were highly reproducible. The force-indentation
curves displayed some energy hysteresis during retraction due to the viscoelastic properties of
collagen and adhesion (negative forces) caused by the interaction between the native collagen
network and the functionalized spherical probe tips. OH-SAM probe tips often displayed an
overall greater adhesion force and had an adhesive interaction distance of ~1 μm, whereas
aggrecan functionalized probe tips displayed prolonged smaller adhesion forces with adhesive
interaction distances of up to ~2.5 μm.
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Figure 3-1. Characteristic force-indentation curves for the indentation (500 nm indentation depth, surface dwell time of t = 30, 0.150 M NaCl, pH ~6.4) of trypsin-treated cartilage samples with colloidal probe tips functionalized with either aggrecan or OH-SAM.
3.1 Effect of Surface Dwell Time on Aggrecan-Collagen Adhesion
Characteristic force-indentation curves for aggrecan-collagen interactions (500 nm
indentation depth, 0.150 M (PBS), [Ca2+]= 0.0 mM) under various surface dwell times are shown
in Figure 3-2. Increasing the surface dwell time increased the hysteresis of the reaction curve
and resulted in significantly greater maximum force of adhesion at larger retraction distances.
Though the extent of adhesive interactive distances did not change, the respective adhesion
forces did increase significantly (one-way ANOVA, p < 0.5).
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AggrecanOH-‐S AM
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Figure 3-2. Characteristic force-indentation curves for the indentation of trypsin-treated cartilage samples (500 nm indentation depth, 0.150 M (PBS), [Ca2+]= 0.0 mM, pH ~6.4) with colloidal probe tips functionalized with aggrecan for surface dwell times of 10 and 30 seconds.
The overall dwell time dependence of the adhesion force and energy is shown in Figure
3-3 and Figure 3-4. For the control experiment (OH-SAM probe tip), adhesion forces varied
from 1.2 ± 0.1 nN to 5.6 ± 0.3 nN, for t = 0 s and t = 60 s, respectively. The aggrecan probe tip
experienced adhesion forces of 0.8 ± 0.1 nN at t = 0 s and 3.1 ± 0.2 nN at t = 60s s. In both cases,
there was minimal adhesion that trended upward towards an asymptotic horizontal limit with
respect to time. At shorter dwell times, the adhesion force of the two different probe tips were
comparable, but OH-SAM probe tips showed significantly greater adhesion force compared to
the aggrecan tip for t > 0 s (two-way ANOVA, p < 0.5).
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Indentation Depth (nm)
Force (nN)
30 sec.10 sec.
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Figure 3-3 The force of adhesion versus surface dwell time for the indentation (500 nm indentation depth, 0.150 M (PBS), [Ca2+]= 0.0 mM, pH ~6.4) of trypsin-treated cartilage samples with colloidal probe tips functionalized with either OH-SAM or aggrecan. Error bars correspond to the standard error of measure (n = 75).
Figure 3-4 shows that the OH-SAM probe tips experienced adhesion energy values of 0.6
± 0.1 fJ at t = 0 s to 3.5 ± 0.3 fJ at t = 60 s. The aggrecan-collagen interactions varied from 1.33
± 0.2 fJ for t = 0 s to 3.9 ± 0.3 fJ at t = 60 s (Figure 3-4). In both systems, adhesion energy
increased with surface dwell time in a non-linear fashion. Unlike Figure 3-3, the horizontal
asymptotic limit was less pronounced. The adhesion energy for the aggrecan and OH-SAM
functionalized probe tips were comparable for all dwell times (two-way ANOVA, p > 0.5),
except for the condition of no surface dwell time (t = 0 s).
0 10 20 30 40 50 600
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Adh
esion Fo
rce (nN)
AggrecanOH-‐S AM
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Figure 3-4 The energy of adhesion versus surface dwell time for the indentation (500 nm indentation depth, 0.150 M (PBS), [Ca2+]= 0.0 mM, pH ~6.4) of trypsin-treated cartilage samples with colloidal probe tips functionalized with either OH-SAM or aggrecan. Error bars correspond to the standard error of measure (n = 75).
3.2 Effect of Ionic Strength on Aggrecan-Collagen Adhesion
The effect of ionic strength (IS) on the adhesion between aggrecan and collagen at a
constant indentation depth of ~500 nm and a surface dwell time of t = 30 s was investigated in
NaCl aqueous solutions with varying ionic strength (0.01 M, 0.15 M, 1.0 M). The effect of ionic
strength on the aggrecan-collagen interaction is evident in Figure 3-5, which depicts a set of
characteristic force-indentation curves for the aggrecan functionalized tip at a constant surface
dwell time of 30 seconds. Higher ionic strength corresponded to slight increases in adhesion
energy and force, but the adhesive interaction distance was not significantly affected.
0 10 20 30 40 50 600
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Adh
esion Ene
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)
AggrecanOH-‐S AM
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Figure 3-5 Characteristic force-indentation curves for the indentation (500 nm indentation depth, t = 30 s, ([Ca2+]= 0.0 mM, pH ~5.6) of trypsin-treated cartilage samples with colloidal probe tips functionalized with aggrecan in solution ionic strengths of 0.15 M NaCl and 1.0 M NaCl.
The indentation of native collagen samples was performed in electrolyte solutions
varying in ionic strength from 0.01 M to 1M NaCl; the overall dependence of adhesion is shown
in Figure 3-6 and Figure 3-7. The adhesion force of the OH-SAM and collagen interactions
varied from 6.4 ± 0.3 nN at 0.01 M NaCl to 5.37 ± 0.3 nN at 1.0 M NaCl. The adhesion force of
the aggrecan-collagen interactions varied from 2.5 ± 0.2 nN at 0.01 M NaCl to 4.3 ± 0.3 nN at
1.0 M NaCl. Interestingly, the difference between 0.01 M and 0.15 M did not lead to a
significant increase in adhesion between aggrecan and collagen. Only at 1M NaCl was there a
significant increase in adhesion (t-test, p < 0.5). In all monovalent conditions, the adhesion force
for the OH-SAM and collagen interactions was significantly greater than the aggrecan-collagen
interactions (one-way ANOVA, p < 0.5).
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0.15 M1.0 M
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Figure 3-6 The force of adhesion versus ionic strength for the indentation (500 nm indentation depth, t = 30 s, [Ca2+]= 0.0 mM, pH ~5.6) of trypsin-treated cartilage samples with colloidal probe tips functionalized with OH-SAM or aggrecan. Error bars correspond to the standard error of measure (n = 50).
Figure 3-7 shows that the adhesion energy of the OH-SAM and collagen interactions
varied from 6.2 ± 0.4 fJ at 0.01 M NaCl to 6.0 ± 0.6 fJ at 1.0 M NaCl. As for aggrecan-collagen
interactions, the adhesion energy changed from 4.4 ± 0.3 fJ at 0.01 M NaCl to 5.6 ± 0.4 nN at 1.0
M NaCl. The adhesion energy OH-SAM probe tip did not change significantly for the different
ionic strengths (one-way ANOVA, p > 0.05). This may indicate that the slight decrease in
adhesion force of OH-SAM for the greater ionic strength was merely a statistical anomaly.
Similar to the adhesion force, the adhesion energy of the aggrecan-functionalized probe tips only
changed significantly in the 1 M NaCl solution. Adhesion energy values for the aggrecan tip
were still comparable to those experienced by OH-SAM tip for the 0.1 M and 1.0 M NaCl
solutions (t-test, p > 0.05).
0.01 0.15 1.0 0
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Adh
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Figure 3-7 The energy of adhesion versus ionic strength for the indentation (500 nm indentation depth, t = 30 s, [Ca2+]= 0.0 mM, pH ~5.6) of trypsin-treated cartilage samples with colloidal probe tip functionalized with OH-SAM or aggrecan. Error bars correspond to the standard error of measure (n = 50).
3.3 Effect of Ca2+ on Aggrecan-Collagen Adhesion
The native collagen networks derived from trypsin treated cartilage samples were also
indented (500 nm indentation depth, surface dwell time of t = 30 s) in aqueous environments
with an overall ionic strength of IS =150 mM, but with varying concentrations of calcium ions in
the form CaCl2 ([Ca2+]= 0.0 mM, 2 mM, 20 mM). Characteristic force-indentation curves for the
aggrecan-functionalized tip under these experimental conditions are shown in Figure 3-8.
Increasing the divalent calcium ion concentration significantly increased the adhesion energy and
adhesion force. The extent of the adhesive interaction distance was not affected by the [Ca2+],
(one-way ANOVA, p > 0.05). Additionally, the effect of [Ca2+] diminished greatly after ~1 µm
retraction from the surface.
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Figure 3-8 Characteristic force-indentation curves for the indentation (500 nm indentation depth, t = 30 s, IS = 0.15 M, pH ~5.6) of trypsin-treated cartilage samples with colloidal probe tips functionalized with aggrecan for [Ca2+]= 0.0 mM and 20 mM.
The overall calcium ion dependence of the adhesion energy and force is shown in Figure
3-9 and Figure 3-10. The adhesion force of the OH-SAM and collagen interactions differed from
4.8 ± 0.4 nN in the absence of Ca2+ to 4.87 ± 0.2 nN with a [Ca2+] = 20 mM. For the OH-SAM
tip, there was no overall dependence of adhesion force on calcium ion concentration (one-way
ANOVA, p > 0.05). The adhesion force of the aggrecan-collagen interactions differed from 2.95
± 0.2 nN in the absence of Ca2+ to 7.4 ± 0.3 nN with a [Ca2+] = 20 mM. The aggrecan-collagen
system experienced drastic changes in adhesion force with respect to [Ca2+] (one-way ANOVA,
p < 0.05). With a [Ca2+] = 20 mM, the aggrecan-collagen interactions were greater than the OH-
SAM and collagen control interactions.
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[C a2+] = 0.0 mM
[C a2+] = 20.0 mM
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Figure 3-9 The force of adhesion versus [Ca2+] for the indentation (500 nm indentation depth, t = 30 s, IS = 0.15 M, pH ~5.6) of trypsin-treated cartilage samples with colloidal probe tips functionalized with OH-SAM or aggrecan. Error bars correspond to the standard error of measure (n = 40).
Figure 3-10 shows that the adhesion energy of the OH-SAM and collagen interactions
varied from 2.5 ± 0.3 fJ in the absence of Ca2+ to 2.9 ± 0.2 fJ with a [Ca2+] = 20 mM. For the
OH-SAM tip, adhesion energy was independent of calcium ion concentration (one-way
ANOVA, p > 0.05). As for aggrecan-collagen interactions, the adhesion energy changed from
3.2 ± 0.7 fJ in the absence of Ca2+ to 4.8 ± 0.4 fJ with a [Ca2+] = 20 mM. There was a significant
increase in adhesion energy for the aggrecan-collagen interactions in aqueous solutions with a
[Ca2+] = 20 mM (t-test, p < 0.05). Furthermore, in contrast to other aqueous conditions, a [Ca2+]
= 20 mM resulted in a greater adhesion energy for the aggrecan tip compared to OH-SAM probe
tip (t-test, p < 0.05).
0.0 2.0 20.00
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Figure 3-10 The energy of adhesion versus [Ca2+] for the indentation (500 nm indentation depth, t = 30 s, IS = 0.15 M, pH ~5.6) of trypsin-treated cartilage samples with colloidal probe tips functionalized with OH-SAM or aggrecan. Error bars correspond to the standard error of measure (n = 40).
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4. Discussion
In this study, aqueous colloidal force spectroscopy was used to quantify interactions
between collagen and aggrecan in aqueous solutions. An aggrecan-functionalized probe tip (R
~2.5μm) was utilized to obtain force-indentation curves on the surface of a native collagen
network, which consisted of trypsin-treated, proteoglycan-depleted cartilage samples (composed
of mostly type II collagen fibrils). The force-indentation curves of the system were analyzed and
used to calculate the adhesion force and energy. Experiments were conducted in physiological
and non-physiological aqueous electrolyte solution conditions, as a function of surface dwell
time, ionic strength, and calcium ion concentration. As a means of comparison, identical tests
were performed with a probe tip functionalized with a hydroxyl self-assembling monolayer.
As previously mentioned, the GAG chains of aggrecan are capable of hydrophobic and
van der Waals interactions by means of their nonpolar regions of methyl functional groups and
sugar rings. Furthermore, the GAG chains are also capable of hydrogen bonding via their
hydroxyl, carboxyl, and sulfate polar functional groups. Similarly, as displayed in Table 1, the
varied amino acid composition of collagen type II enables hydrogen bonding, nonpolar,
hydrophobic, and van der Waals interactions by means of its polar and charged functional groups.
The dependence of surface dwell time for the aggrecan and OH-SAM functionalized
probe tips is evident in Figures 3-3 and 3-4. The adhesion force showed a significant nonlinear
increase with respect to surface dwell time asymptotically approaching a maximum value of 3.1
± 0.2 nN at t = 60 seconds. In addition, there was a nearly four-fold increase in adhesion energy
for the aggrecan-functionalized probe tip for t = 60 s. These results can be attributed to an
increase in molecular interactions: prolonged contact with the collagen network allowed the
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aggrecan macromolecules to rearrange and spread across the surface of the fibers, effectively
increasing the relative contact area and sites of molecular interactions.
The indentation of the collagen samples with the OH-SAM probe tips resulted in overall
greater adhesion force for all dwell times. This indicates that the interactions between collagen
and individual aggrecan macromolecules were not as strong as those between the hydrophilic
hydroxyl functional groups and collagen. Despite the weaker individual molecular aggrecan-
collagen interactions, the adhesion energy of the two probe tips were statistically similar for t > 0
s. The larger deformability of aggrecan, compared to the OH-SAM (HS(CH2)11OH), enabled
more molecular contacts with the collagen network under the same indentation conditions. This
effect was most evident in the heterogeneous long-range adhesion that was observed at up to
~2.5 μm extension upon retraction for the aggrecan-functionalized probe tips. Given that the
contour length of aggrecan is approximately 400 nm, the extension on the order of microns
suggests that the collagen network was also being pulled during reaction. The different aqueous
conditions did not change the adhesive interaction distance for the aggrecan-functionalized probe
tip.
As seen in Figure 3-5, there was no significant long-range repulsion detectable between
aggrecan and collagen during approach for any ionic strength condition. Given the highly
negative charge of aggrecan, this indicates that the surface of the collagen network did not
display a significant overall charge. However, in Figure 3-6 the adhesion force of the aggrecan
tip nearly doubled between ionic conditions of 10 mM NaCl (2.5 ± 0.2 nN) and 1 M NaCl (4.3 ±
0.3 nN). The increase in adhesion with respect to ionic strength indicates that regions of the
collagen network surface had negatively charged amino acids that were exposed and provided a
source of electrostatic repulsion for individual aggrecan molecules. Given the variation in local
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charges of the collagen network, shielding of electrostatic repulsion was only experienced at
some molecular interaction sites and thus the adhesion energy only increased ~20% for the 1 M
NaCl solution.
Figure 3-9 and Figure 3-10 show the dependence of adhesion for aggrecan-collagen
interactions on calcium ion concentrations ([Ca2+]). The adhesive interaction distance was
observed to be similar at different [Ca2+], but the adhesion force increased more than two-fold in
magnitude from 0 mM (2.95 ± 0.2 nN) to 20 mM (7.4 ± 0.3 nN). These results are in accordance
with previous experiments that showed the divalent ion-bridging capabilities of aggrecan during
self-adhesion (22,36). Similarly, divalent ion bridging would facilitate an interaction mechanism
between two negative point charges present in aggrecan and the collagen surface. The fact that
the adhesion energy only experienced a 50% increase in the presence of 20mM of CaCl2 denotes
that the divalent ion-bridging was only present in certain (negative) regions of the collagen
network. Moreover, the effect of [Ca2+] on adhesion diminished greatly beyond ~1 µm,
indicating that divalent ion-bridging was present only at shorter lengths. The exact effective
range cannot be estimated, since collagen also contributed to the adhesive interaction distance.
The different ionic conditions provided insight into the collagen-aggrecan interactions
present in vivo. Our study showed there was significant adhesion between aggrecan and the
collagen network at physiological ionic strength of ~150 mM, showing some shielding of
electrostatic repulsion between aggrecan and exposed negatively charged amino acids on the
fibrillar surface of collagen. As would be the case in physiological conditions, a small presence
of calcium ions (~2mM) also increased the adhesion between aggrecan and collagen. The effect
of ionic strength and [Ca2+] on the aggrecan-collagen interaction was similar to that observed in
previous work on aggrecan-aggrecan adhesion. For the physiological condition of 0.15 M ionic
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strength and [Ca2+] ~2mM, the adhesion of aggrecan-collagen interactions were ~50% greater
than aggrecan-aggrecan interactions.
However, given the increase in adhesion for aggrecan-collagen in 1.0 M ionic strength
solution, there are still some electrostatic repulsion forces present between the two cartilage
extracellular components under physiological ionic concentrations. Therefore, aggrecan is
capable of interacting with collagen in the extracellular matrix but is not immobilized once in
contact with the fibrillar surface of collagen. In turn, this would allow aggrecan to maintain
mobility within the extracellular matrix and continue to provide osmotic pressure and hydraulic
permeability. Furthermore, the adhesion energy between aggrecan and collagen provide another
means of energy dissipation while under loading. As was postulated for the aggrecan-aggrecan
interaction, energy dissipation can help maintain the structural integrity of the cartilage
extracellular matrix (22). Ultimately, we are hopeful that these findings will provide further
insight into the self-assembly of the cartilage extracellular matrix and help develop principles for
tissue regeneration and replacement.
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5. Conclusion
An aggrecan-functionalized probe tip (R ~2.5µm) was indented ~500nm into the surface
of a native collagen network, composed of trypsin-treated, proteoglycan-depleted cartilage. The
molecular interactions between aggrecan and collagen were quantified in various aqueous
conditions. The aggrecan-collagen adhesion showed a significant ionic strength and [Ca2+]-
dependence. Under the physiological conditions of 0.15 M ionic strength and a [Ca2+] ~2mM,
aggrecan-collagen interactions showed an adhesion force of 5.3 ± 0.9 nN (t = 30 s). Full
electrostatic shielding is evident at 1.0 M ionic strength, indicating there are still some repulsive
electrostatic forces present between aggrecan and collagen at physiological concentrations.
Aggrecan-collagen adhesion was increased through calcium ion-bridging between aggrecan and
negatively charged amino acids exposed at the collagen fibrillar surface. We believe that
aggrecan-collagen adhesion adds to the structural integrity of the cartilage extracellular matrix
and plays a role in the biomechanical properties of cartilage. We are hopeful that these findings
will provide further insight into the self-assembly of the cartilage extracellular matrix and help
develop principles for tissue regeneration and replacement.
The methodologies developed here can be extended to the other underlying layers of
cartilage, where aggrecan content and fibrillar structure vary significantly compared to the
superficial layer. Future work can also incorporate the effects of osteoarthritis, specifically the
degradation of the collagen fibrillar network and its effects on aggrecan-collagen adhesion. In
addition, similar indentation experiments can be performed in the presence of other extracellular
components, such as COMP and matrilin-3, to analyze any possible tertiary effects that are
caused by adaptor mediated interaction mechanisms.
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6. Acknowledgements
I would like to give a special thanks to Han-Hwa Hung for her assistance with sample
preparation and other laboratory work, Lin Han and Alan Shwartzman for their help with MFP-
3D training and related problems, and Alan Grodzinsky and Christine Ortiz for their helpful
advice and resources.
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