# The Effect of Silver Nanofibers on the Deformation Properties of Blood Vessels: Towards the Development of New Nanotechnologies to Prevent Rupture of Aneurysms

Authors: Miguel Gonzalez; Daniel Rivera; Alam Marcelino; Gabriela Agront; Rafael Rodriguez; Miguel Castro
Journal: Journal of Nanomaterials
 (2014)

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## Abstract

An aneurysm is the result of a widening or ballooning of a portion of a blood vessel. The rupture of an aneurysm occurs when the mechanical stress acting on the inner wall exceeds the failure strength of the blood vessel. We propose an innovative approach to prevent the rupture of an aneurysm based on the use of nanotechnology to improve the strength of the blood vessel. We present results on the effect of silver nanofibers on the resistance toward deformation of blood vessels. The silver nanofibers are grown on the surface of the blood vessels. The nanofibers are120
±
30 nm in diameter and 2.7
±
0.8 μm in length. The deformation per applied force of blood vessels was found to decrease from 0.15 m/N in control blood vessels to 0.003 m/N in blood vessels treated with the nanofibers. This represents an increase in the resistance towards deformation of a factor of 50. The increase in the resistance towards deformation is clinically significant since blood pressure increases by factors slightly larger than one in the human body. Treatment of blood vessels with silver nanofibers is a potential translational clinical tool for preventing rupture of aneurysms in a clinical setting.


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## Body

## 1. Background

An aneurysm is a condition identified as an abnormal widening or ballooning formation on segments of blood vessels that can result in adverse health effects in the population [1–5]. A few of direct implications of different types of the disease in humans are highlighted in Table 1. The development of an aneurysm in a blood vessel is summarized on Figure 1. The biomechanical properties of blood vessels are disrupted by the shear stress associated with the hemodynamics in the region of an aneurysm. Loss of the blood vessel characteristic elasticity allows a persistent widening of the area and the formation and growth of the aneurysm [4, 5]. The biomechanical stress exerted by the regional hemodynamic condition allows for a weakening of vessel walls and increases the risk of aneurysm rupture [4, 5]. Open or endovascular surgery is the recommended treatment for aneurysms that reach a critical size to prevent rupture [2–5]. Open surgery is performed to replace the affected vessel area with a man-made graft [3–6]. Endovascular surgery, on the other hand, is performed with the insertion of a catheter through the vascular system to reach the affected area. A variety of apparatus or materials, including stents, coils, and polymers, can be inserted through the catheter and placed on the aneurysm area to protect the affected region of the vessel wall from hemodynamic effects [1, 3–5, 7–10]. In the context of the discussion presented above, devices employed to prevent aneurysm rupture are expected to become smaller to reduce the risks associated with invasive endovascular procedures and improve biocompatibility [11–17].Table 1
Incidence and risk factors of aneurysms.
Aneurysm type
Incidence and risk factors
Intracranial aneurysm (IC) [7]
About 30,000 patients are treated for IC ruptures each year in the US 60% of these cases ended up with disabilities or dead
Thoracic aortic aneurysm (TAA) [32, 33]
Incidence of 10.4 per 100,000 persons per year 2.9 to 3.5 rupture cases per 100,000 people annually
Abdominal aortic aneurysm (AAA) [4, 32, 34, 35]
150,000 cases per year
Distribution of 12.5% in men and 5.2% in women in people between 75 and 84 years of age
Ruptures have a 90% risk of deathFigure 1
The formation and growth of aneurysm due to the shear stress caused by the intermittent blood flow. The drawing is intended to guide the eye through the text.Developments of new imaging tools with increased spatial resolution and the general interest in the biomedical applications of nanotechnology motivate the present study [18–27]. In particular, the use of nanotechnologies to increase the strength of blood vessels in the early stages of formation of aneurysms may prevent growth of the widening area. In this regard, molecularly guided assembly offers the opportunity to grow nanofibers directly on the tissue and it represents a unique opportunity for developing technologies acting on tissue-specific locations [28, 29]. Here, we report on the use of molecularly guided assembly of nanoparticles into a mesh consisting of nanofibers for improving the strength of blood vessels. We have explored the growth of silver nanofibers on the surface of blood vessels endothelial surfaces obtained fromsus scrofa domestica(domestic pig) with the purpose of contributing to the current body of knowledge related to the applications of nanotechnology in biomedical science and tissue bioengineering research. The nanofibers are composed of small particles and clusters. This innovative approach targets novel biomedical applications for preventing the rupture of aneurysms. It is based on the assembly of silver into one dimensional nanostructures guided by mercaptoacetic acid (HSCH2CO2H) [30, 31]. The sulfur end of the thiol molecule attaches to silver, while the carboxylic acid end forms hydrogen bonds to the carboxylic acid end of another thiol which in turn is bonded to silver. The nanofibers form when water is removed from the dispersion and is completely irreversible. We found that the silver nanofibers increase the resistance of blood vessels towards deformation as compared to untreated tissue.


## 2. Materials and Methods

### 2.1. Synthesis of Silver-Thiol Dispersion: Precursors to Silver Nanofibers

About two (2) micrograms (μg) of silver nitrate (AgNO3, Fisher) were mixed with an equivalent number of moles of mercaptoacetic acid (HSCH2CO2H, Aldrich) and 10.0 mL of deionized water. The mixture was shaken by hand for a few of seconds and the suspension was stored at dark under room temperature.


### 2.2. Blood Vessels

Blood vessels were obtained from the head of asus scrofa domestica that was donated by a local slaughter house: the animal was killed for marketing purposes and not for the measurements reported here. The head was kept frozen in a refrigerator and was allowed to defrost prior to the removal of samples containing blood vessels. Blood vessel-containing tissue samples were cut in sections measuring approximately 10 cm in length. A flow of air was passed through selected blood vessels to facilitate the dissection from the tissue (Figure 2(a)). Sections of the blood vessels were cut wide open to expose the internal endothelial surface. The blood vessel sections employed for the measurements presented in this work were 2 cm long, 2 cm wide and between 1 and 4 mm in depth (Figure 2(b)).(a) Representative images of pieces of tissue containing blood vessels and (b) a piece of blood vessel cut wide open.
(a)
(b)


### 2.3. Preparation of Blood Vessels Treated with Nanofibers and Control Tissue

Regions of the internal endothelial surface of the blood vessels were treated with a total volume of 60.0μL of the silver-thiol dispersion in 10 μL incremental steps. The internal blood vessels’ endothelial surfaces were allowed to dry in air to allow for the formation of the silver nanofibers. Control tissue was prepared by treating regions of the internal endothelial surface of the blood vessels with a total volume of 60.0 μL of H2O in 10 μL incremental steps.


### 2.4. Characterization of Nanofibers

#### 2.4.1. SEM Imaging

SEM images were obtained with an environmental JEOL JSM-6460 LV SEM. Blood vessels were fixed to a conductive carbon tape and placed in the SEM analysis chamber. SEM images were collected with an acceleration voltage of 5 kV in the high vacuum mode with spot sizes between 35 and 40. The diameter and length of the nanofibers were estimated from the SEM images using the software package provided by JEOL.


#### 2.4.2. UV-Visible Measurements

UV-visible absorption spectroscopy measurements on dry deposits of the nanofibers formed on the surface of the blood vessels were performed with an Ocean Optics 2000 spectrometer coupled to an Olympus microscope operated in the reflection mode and UV grade optics. The Mie model of spheres and wires was used for simulation of the optical absorption spectrum [36]. The simulations were performed in a Dell PC using Igor software.


### 2.5. Determination of Displacement as a Function of Pressure

The deformation of the tissue was determined by applying a force with a pin. The blood vessel samples were placed on a flat aluminum holder. The holder has an aperture that is 1 cm in diameter to allow the pin to come in contact with the blood vessel surfaces. The area of the pin that comes into contact with the sample is 1.5 mm2. A cantilever system was developed and employed to apply the force on the tissue (see Figure 3). The cantilever consisted of a pin (d = 1.4 mm) glued to the inner wall of a glass cylinder and a recipient at the other end to place a weight. The force was controlled by placing a known weight of sand on the recipient to drive the movement of the tip upward at the other end. The mass of the sand was determined with a Mettler Toledo microbalance model AT 20. The microbalance allowed the determination of the mass of the sand to within 10−6 grams. The displacement was determined using a calibrated ruler placed next to the tip. The displacement was recorded with a standard digital camera and was determined using commercially available software. A few micrograms of sand are needed to get the pin in touch with the tissue (region A). There is a region in which further addition of mass does not result in a measureable displacement (region B) until a small amount of sand added to the counterweight results in a displacement of the tip (Region C). That point is taken to correspond to the minimum force required to bend the internal blood vessels’ endothelial surface.Figure 3
Experimental set up used to measure tissue deformation as a function of applied pressure. The pin has a free displacement (region A) until it reaches contact with the tissue (region B). There is a range in which the pressure applied with the pin is not enough to cause a deformation in the tissue, highlighted as region B in the figure. Further increase in the force applied with the pin results in the deformation of the tissue which is measured by a change in the displacement of the pin as highlighted by region C in the same figure. The force applied is estimated by the mass of the sand used to drive the movement of the pin.


## 2.1. Synthesis of Silver-Thiol Dispersion: Precursors to Silver Nanofibers

About two (2) micrograms (μg) of silver nitrate (AgNO3, Fisher) were mixed with an equivalent number of moles of mercaptoacetic acid (HSCH2CO2H, Aldrich) and 10.0 mL of deionized water. The mixture was shaken by hand for a few of seconds and the suspension was stored at dark under room temperature.


## 2.2. Blood Vessels

Blood vessels were obtained from the head of asus scrofa domestica that was donated by a local slaughter house: the animal was killed for marketing purposes and not for the measurements reported here. The head was kept frozen in a refrigerator and was allowed to defrost prior to the removal of samples containing blood vessels. Blood vessel-containing tissue samples were cut in sections measuring approximately 10 cm in length. A flow of air was passed through selected blood vessels to facilitate the dissection from the tissue (Figure 2(a)). Sections of the blood vessels were cut wide open to expose the internal endothelial surface. The blood vessel sections employed for the measurements presented in this work were 2 cm long, 2 cm wide and between 1 and 4 mm in depth (Figure 2(b)).(a) Representative images of pieces of tissue containing blood vessels and (b) a piece of blood vessel cut wide open.
(a)
(b)


## 2.3. Preparation of Blood Vessels Treated with Nanofibers and Control Tissue

Regions of the internal endothelial surface of the blood vessels were treated with a total volume of 60.0μL of the silver-thiol dispersion in 10 μL incremental steps. The internal blood vessels’ endothelial surfaces were allowed to dry in air to allow for the formation of the silver nanofibers. Control tissue was prepared by treating regions of the internal endothelial surface of the blood vessels with a total volume of 60.0 μL of H2O in 10 μL incremental steps.


## 2.4. Characterization of Nanofibers

### 2.4.1. SEM Imaging

SEM images were obtained with an environmental JEOL JSM-6460 LV SEM. Blood vessels were fixed to a conductive carbon tape and placed in the SEM analysis chamber. SEM images were collected with an acceleration voltage of 5 kV in the high vacuum mode with spot sizes between 35 and 40. The diameter and length of the nanofibers were estimated from the SEM images using the software package provided by JEOL.


### 2.4.2. UV-Visible Measurements

UV-visible absorption spectroscopy measurements on dry deposits of the nanofibers formed on the surface of the blood vessels were performed with an Ocean Optics 2000 spectrometer coupled to an Olympus microscope operated in the reflection mode and UV grade optics. The Mie model of spheres and wires was used for simulation of the optical absorption spectrum [36]. The simulations were performed in a Dell PC using Igor software.


## 2.4.1. SEM Imaging

SEM images were obtained with an environmental JEOL JSM-6460 LV SEM. Blood vessels were fixed to a conductive carbon tape and placed in the SEM analysis chamber. SEM images were collected with an acceleration voltage of 5 kV in the high vacuum mode with spot sizes between 35 and 40. The diameter and length of the nanofibers were estimated from the SEM images using the software package provided by JEOL.


## 2.4.2. UV-Visible Measurements

UV-visible absorption spectroscopy measurements on dry deposits of the nanofibers formed on the surface of the blood vessels were performed with an Ocean Optics 2000 spectrometer coupled to an Olympus microscope operated in the reflection mode and UV grade optics. The Mie model of spheres and wires was used for simulation of the optical absorption spectrum [36]. The simulations were performed in a Dell PC using Igor software.


## 2.5. Determination of Displacement as a Function of Pressure

The deformation of the tissue was determined by applying a force with a pin. The blood vessel samples were placed on a flat aluminum holder. The holder has an aperture that is 1 cm in diameter to allow the pin to come in contact with the blood vessel surfaces. The area of the pin that comes into contact with the sample is 1.5 mm2. A cantilever system was developed and employed to apply the force on the tissue (see Figure 3). The cantilever consisted of a pin (d = 1.4 mm) glued to the inner wall of a glass cylinder and a recipient at the other end to place a weight. The force was controlled by placing a known weight of sand on the recipient to drive the movement of the tip upward at the other end. The mass of the sand was determined with a Mettler Toledo microbalance model AT 20. The microbalance allowed the determination of the mass of the sand to within 10−6 grams. The displacement was determined using a calibrated ruler placed next to the tip. The displacement was recorded with a standard digital camera and was determined using commercially available software. A few micrograms of sand are needed to get the pin in touch with the tissue (region A). There is a region in which further addition of mass does not result in a measureable displacement (region B) until a small amount of sand added to the counterweight results in a displacement of the tip (Region C). That point is taken to correspond to the minimum force required to bend the internal blood vessels’ endothelial surface.Figure 3
Experimental set up used to measure tissue deformation as a function of applied pressure. The pin has a free displacement (region A) until it reaches contact with the tissue (region B). There is a range in which the pressure applied with the pin is not enough to cause a deformation in the tissue, highlighted as region B in the figure. Further increase in the force applied with the pin results in the deformation of the tissue which is measured by a change in the displacement of the pin as highlighted by region C in the same figure. The force applied is estimated by the mass of the sand used to drive the movement of the pin.


## 3. Results

### 3.1. Optical Absorption Spectroscopy Measurements

The absorption spectra of thiol-silver dispersions have been published elsewhere [30]. It has absorption peaks due to silver dimers (Ag2) in the ultraviolet region at 260 nm and 280 nm as well as a broader band resulting from light absorption by silver nanoparticles at 360 nm. Representative UV-visible absorption spectrum of the nanofibers grown on the blood vessel surface is illustrated on Figure 4. The experimental spectrum of the nanofibers that are formed when the water is removed from the dispersion has a continuous absorption band from the UV to the visible. No evidence is found for a localized band in the absorption spectrum of the nanofibers, in marked contrast to the absorption spectrum of the dispersion used to prepare the nanofibers that exhibits well-defined bands due to the absorption of light by silver nanoclusters and nanoparticles [30].Figure 4
A representative absorption-reflection spectrum silver nanofiber deposited on the blood vessels is displayed on (a). The inserts (b) and (c) simulated absorption spectra of silver nanospheres with a diameter of 30 nm and silver nanowires with a length of 1μm and 50 nm in diameter, respectively.Light absorption by metallic silver results from a collective excitation of electrons known as plasmons. Silver nanoparticles have a transverse plasmon mode while a longitudinal plasmon mode can be observed in the spectrum of silver nanowires. Simulations of the absorption spectrum of wires and particles provided insight about the electronic excitations that contribute to the absorption spectrum of the nanofibers. The inserts (b) and (c) in Figure4 illustrate computer simulations using Mie theory of the light absorption of particles and wires, respectively [36]. The simulation assumes wires with a length and diameter of 1 μm and 50 nm, respectively. The diameter of the spheres used in the simulation is 30 nm. The light absorbed by the wires is predicted to decrease with wavelength between 200 and 300 nm and to exhibit a sharp increase at 310 nm until it peaks at 360 nm. The amount of light absorbed by the wires is predicted to decrease gradually with wavelength from 360 nm up to 1000 nm. The spectrum simulated for the spheres, on the other hand, has a well-defined absorption band centered on 380 nm. The absorption spectrum of the nanofibers is remarkably similar to the one simulated for the wires. Thus, the tail toward long absorption wavelengths observed in the spectrum of the nanofibers results from excitations of the longitudinal plasmon mode in silver. This interpretation highlights the metallic character of the nanofibers that result from coupling silver through molecular interactions among the thiol molecules. The absorption of light between 200 and 360 nm in the experimental spectrum likely results from the presence of thiol molecules in the sample.


### 3.2. Electron Microscopy Measurements

SEM measurements were performed to establish the morphology of the nanofibers grown on the surface of the blood vessel walls. A representative image of a region of the interior surface of blood vessels is labeled (a) on the upper left hand side of Figure5. Representative images of areas of blood vessel surfaces where we have grown the nanofibers are labeled (b), (c), and (d) on Figure 5. The deposit of the nanofibers resembles a mesh of the order of several microns in the SEM image labeled (b). The nanofibers that compose the mesh can be identified in images obtained at slightly higher magnifications, like in Figures 5(c) and 5(d). The diameter and length distribution of the nanofibers grown on the surface of the blood vessels are summarized on Figures 5(e) and 5(f), respectively. The nanofibers are (120 ± 30) nm in diameter and have lengths of the order of (2.7 ± 0.8) μm.Representative SEM images of (a) the control blood vessel. Images of the surface of a blood vessel where the silver nanofibers were grown are labeled (b), (c), and (d). The diameter and length distribution of the one dimensional nanostructures grown on the surface of the blood vessels are illustrated in (e) and (f), respectively.
(a)
(b)
(c)
(d)
(e)
(f)


### 3.3. Effect of Silver Nanofibers on the Deformation of the Blood Vessel Tissue

The squares and circles in Figure6 represent the displacement of the blood vessel surface as a function of the applied force in a control and nanofiber modified blood vessel, respectively. The deformation of the blood vessel is measured from the displacement of a pin head that exerts the indicated force on a 1.5 mm2 area. There is an initial tension due to the procedure employed to hold the tissues that is taken to be the same on both types of tissue samples; thus, our results must be taken by comparison among the control and modified tissue samples and should not be considered to represent absolute numbers. There is a region where no displacement is detected upon the application of an external force. This region is evident in the data summarized in the insert on the right hand side of Figure 6. The onset of displacement in the control and nanofiber treated blood vessel are observed around 3 × 10−3 and 3.4 × 10−1 N, respectively. We conclude that the resistance of the blood vessels toward deformation is increased by the presence of the nanofibers. This is further supported by analysis of the initial slope in the rise of the displacement with applied force. The slope of the initial rise in displacement with applied force is markedly different in both cases. The slopes of the rise in displacement with force are 0.15 and 0.003 m/N for the control and nanofibers modified tissue, respectively. The smaller slope in the deformation curve of the blood vessels modified by the nanofibers lead us to conclude that these nanostructures increase the resistance to deform the tissue.Figure 6
Dependence of the displacement, in meters (m), on the applied force, in newtons (N).


## 3.1. Optical Absorption Spectroscopy Measurements

The absorption spectra of thiol-silver dispersions have been published elsewhere [30]. It has absorption peaks due to silver dimers (Ag2) in the ultraviolet region at 260 nm and 280 nm as well as a broader band resulting from light absorption by silver nanoparticles at 360 nm. Representative UV-visible absorption spectrum of the nanofibers grown on the blood vessel surface is illustrated on Figure 4. The experimental spectrum of the nanofibers that are formed when the water is removed from the dispersion has a continuous absorption band from the UV to the visible. No evidence is found for a localized band in the absorption spectrum of the nanofibers, in marked contrast to the absorption spectrum of the dispersion used to prepare the nanofibers that exhibits well-defined bands due to the absorption of light by silver nanoclusters and nanoparticles [30].Figure 4
A representative absorption-reflection spectrum silver nanofiber deposited on the blood vessels is displayed on (a). The inserts (b) and (c) simulated absorption spectra of silver nanospheres with a diameter of 30 nm and silver nanowires with a length of 1μm and 50 nm in diameter, respectively.Light absorption by metallic silver results from a collective excitation of electrons known as plasmons. Silver nanoparticles have a transverse plasmon mode while a longitudinal plasmon mode can be observed in the spectrum of silver nanowires. Simulations of the absorption spectrum of wires and particles provided insight about the electronic excitations that contribute to the absorption spectrum of the nanofibers. The inserts (b) and (c) in Figure4 illustrate computer simulations using Mie theory of the light absorption of particles and wires, respectively [36]. The simulation assumes wires with a length and diameter of 1 μm and 50 nm, respectively. The diameter of the spheres used in the simulation is 30 nm. The light absorbed by the wires is predicted to decrease with wavelength between 200 and 300 nm and to exhibit a sharp increase at 310 nm until it peaks at 360 nm. The amount of light absorbed by the wires is predicted to decrease gradually with wavelength from 360 nm up to 1000 nm. The spectrum simulated for the spheres, on the other hand, has a well-defined absorption band centered on 380 nm. The absorption spectrum of the nanofibers is remarkably similar to the one simulated for the wires. Thus, the tail toward long absorption wavelengths observed in the spectrum of the nanofibers results from excitations of the longitudinal plasmon mode in silver. This interpretation highlights the metallic character of the nanofibers that result from coupling silver through molecular interactions among the thiol molecules. The absorption of light between 200 and 360 nm in the experimental spectrum likely results from the presence of thiol molecules in the sample.


## 3.2. Electron Microscopy Measurements

SEM measurements were performed to establish the morphology of the nanofibers grown on the surface of the blood vessel walls. A representative image of a region of the interior surface of blood vessels is labeled (a) on the upper left hand side of Figure5. Representative images of areas of blood vessel surfaces where we have grown the nanofibers are labeled (b), (c), and (d) on Figure 5. The deposit of the nanofibers resembles a mesh of the order of several microns in the SEM image labeled (b). The nanofibers that compose the mesh can be identified in images obtained at slightly higher magnifications, like in Figures 5(c) and 5(d). The diameter and length distribution of the nanofibers grown on the surface of the blood vessels are summarized on Figures 5(e) and 5(f), respectively. The nanofibers are (120 ± 30) nm in diameter and have lengths of the order of (2.7 ± 0.8) μm.Representative SEM images of (a) the control blood vessel. Images of the surface of a blood vessel where the silver nanofibers were grown are labeled (b), (c), and (d). The diameter and length distribution of the one dimensional nanostructures grown on the surface of the blood vessels are illustrated in (e) and (f), respectively.
(a)
(b)
(c)
(d)
(e)
(f)


## 3.3. Effect of Silver Nanofibers on the Deformation of the Blood Vessel Tissue

The squares and circles in Figure6 represent the displacement of the blood vessel surface as a function of the applied force in a control and nanofiber modified blood vessel, respectively. The deformation of the blood vessel is measured from the displacement of a pin head that exerts the indicated force on a 1.5 mm2 area. There is an initial tension due to the procedure employed to hold the tissues that is taken to be the same on both types of tissue samples; thus, our results must be taken by comparison among the control and modified tissue samples and should not be considered to represent absolute numbers. There is a region where no displacement is detected upon the application of an external force. This region is evident in the data summarized in the insert on the right hand side of Figure 6. The onset of displacement in the control and nanofiber treated blood vessel are observed around 3 × 10−3 and 3.4 × 10−1 N, respectively. We conclude that the resistance of the blood vessels toward deformation is increased by the presence of the nanofibers. This is further supported by analysis of the initial slope in the rise of the displacement with applied force. The slope of the initial rise in displacement with applied force is markedly different in both cases. The slopes of the rise in displacement with force are 0.15 and 0.003 m/N for the control and nanofibers modified tissue, respectively. The smaller slope in the deformation curve of the blood vessels modified by the nanofibers lead us to conclude that these nanostructures increase the resistance to deform the tissue.Figure 6
Dependence of the displacement, in meters (m), on the applied force, in newtons (N).


## 4. Discussion

Metallic silver nanofibers form on the internal surface of blood vessel tissues from a silver-thiol dispersion. The silver nanofibers grown on the blood vessel surface are arranged in a mesh-like structure. We estimate a density of silver nanofibers of about 2 nanofibers/μm2 from the SEM measurements. This number is in close agreement to the average length of (2.7 ± 0.8) μm as well as with the peak in the distribution of lengths displayed on Figure 5.Thetunica intima is the layer of blood vessels closest to the blood. It is composed of a thin layer of endothelial cells, an internal elastic lamina and collagen fibers. Bundles of collagen fibrils and collagen fibers are found in thetunica media andtunica adventitia. The collagen fibers have an anisotropic arrangement and are an important element in providing resistance to the pressure load in blood vessels. Collagen is synthesized as pre procollagen, which is a primary structure containing specific regions of glycine, proline, and lysine residues.Blood vessels modified by the silver nanofibers have a higher resistance toward deformation than control tissues. This is evidenced by the deformation measurements as a function of force. The initial slope of the deformation as a function of applied pressure in blood vessels modified with the silver nanofibers and the control are 0.003 m/N and 0.15 m/N, respectively. Thus, a given force will deform the modified tissue by a smaller amount than the control. This represents an increase in the resistance towards deformation of a factor of 50. This is clinically significant if we consider that blood pressure increases by factors slightly larger than one in the human body.The blood vessels modified by the silver nanofibers are tissue that can carry the pressure load better than the tissue found in animals and humans. The Young’s modulus or elastic modulus is a measure of the stiffness of a material. The elastic modulus(
E
) is directly proportional to the ratio of the applied force (
F
) per unit area (
A
)and inversely proportional to the displacement (
Δ
L
) relative to the length (
L
o
) of a material:
(1)
E
=
(
F
/
A
)
(
Δ
L
/
L
o
)
.
An estimate of the elastic modulus of the system composed by the nanofibers on the blood vessel can be obtained from the slope of the dependence of the deformation on applied force. We estimate an elastic modulus between 1 and 3 × 103 N/m2 and 0.15 × 103 N/m2 for the blood vessels modified with the silver nanofibers and control, respectively. These values fall within the elastic modulus reported for blood vessels [37, 38]. The smaller displacement found in the tissue modified silver nanofibers as compared to the original material is consistent with the formation of stiff areas in the modified blood vessels. The risk of rupture of the blood vessel wall is reduced by the resistance towards deformation exhibited by the silver nanofibers treated blood vessel.The measurements reported here were performed under static conditions and outside the physiological environment where blood vessels are found in humans. Further work in the use of this nanotechnology requires measurements of the effect of pressure on deformation of silver-nanofiber modified blood vessels in a dynamic and pulsed flow set up similar to the one found in physiologically relevant environments and with tools to measure the deformation of the blood vesselsin vivo [39]. Such experiments are currently outside the reach of our experimental setup and scope, yet this study advances the development of new nanotechnologies based on the use of silver nanostructures to prevent the rupture of aneurysms.



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*Source: 853120-2014-05-15.xml*