**AFM Measurements to Investigate Particulates and Their Interactions with Biological Macromolecules**

L. Latterini and L. Tarpani

*Department of Chemistry, Center of Excellence for Nanostructured and Innovative Materials, University of Perugia Italy* 

#### **1. Introduction**

In recent years much attention has been paid to the development of metrology methods to investigate particulate matter and its interaction with bio-molecules. This interest is triggered by the potential applications of nanoparticle-biomolecule hybrid systems in different areas such as bio-sensing, catalysis, target delivery, selective recognition, etc. (Amelia et al., 2010; Bellezza et al., 2009; Latterini & Amelia, 2009; Joralemon et al., 2005; Nehilla et al., 2005; Rosi & Mirkin, 2005). Furthermore, a better understanding of the interactions between particles and biomolecules could help to optimize the ability to reduce the exposure to particulate matter in working environments.

In the last decade AFM methods based on a vibrating tip to explore a surface topography experienced a significant transformation which allowed them to reach nm-resolution imaging and become sensitive tools to investigate tip-sample interactions down to sub-nm resolution (García & Pérez, 2002). Hence the chance is to develop quantitative procedures to study material properties with high spatial resolution even without affecting the softest samples. These achievements have shown that AFM methods can be used as a valid alternative to other well established techniques (such as electron microscopies) in the study of nanostructured materials. The good spatial resolution of AFM measurements can be achieved without any sample pre-treatments thus overcoming the limitations in the sample preparation involved in electron microscopies. AFM imaging appears particularly attractive to characterize particulate matter based on organic materials with high spatial resolution without any concerns about scattering cross sections and sample treatment procedures. Extremely interesting in this context is the possibility to use AFM to characterize particles conjugated to biological macromolecules. Indeed, AFM scanning showed a good accuracy to obtain size distributions for colloidal particle samples comparable to dynamic light scattering techniques or even better if the samples were polydispersed (Hoo et al., 2008)

In the present contribution, particulate matter, either intentionally prepared with designed dimensional, morphological and chemical properties or produced in working environments during the phases of metal processing or combustion processes, were dimensionally characterized and information on their surface morphology were obtained.

AFM Measurements to Investigate Particulates

and Their Interactions with Biological Macromolecules 89

Fig. 1. 3-D topography images of CdS nanocrystal refluxed with thioglycerol for 30' (a) and 5

the diffusion of the seeds on the nuclei surface is quite rapid, and therefore it leads to a very broad size. Furthermore, the difficulties to control the growth lead to the development of defects in the crystal structures as confirmed by luminescence studies which show trap

hours (b) together with their relative height distributions (c, d respectively)

states emission (Latterini & Amelia, 2009).

The characterization of particulates or colloidal nanoparticles in the presence of protein was used to obtain valuable information on the nanoparticle-protein interactions and eventually on the disposition of the macromolecules with respect to the particles. The presented results will be discussed in terms of experimental conditions to enhance or to quench the particulate-biomolecule interaction in order to control the stability of hybrid materials.

## **2. Results**

Wet chemical synthesis for colloidal nanoparticle preparation have recently attracted much attention with the aim to optimize the procedures to work in mild conditions (atmospheric pressure, temperature below 100°C); in these conditions, the colloidal samples can be easily characterized by polydisperse size distributions and non-homogeneous shapes. AFM imaging can provide a fast investigation tool to characterize nanoparticle preparations without a prior knowledge of the size distributions and shape. Furthermore, the acquisition of AFM data can give valuable information on the thickness of the stabilizer shell, which has to be necessarily used to control the nanoparticle growth in solution and it is worth to be taken into account as particle constituent. For nanomaterials, the size distribution, surface area, shape, aggregation state and composition strongly affect their biological activity since these properties have an influence on their interactions with biomolecules. AFM in tapping mode has been used to study nanoparticles deposited on mica and to investigate their interactions with proteins and DNA.

#### **2.1 Dimensional characterization of colloidal nanoparticles and particulates**

AFM topography imaging was helpful to obtain information on the growth mechanism of CdS nanocrystals prepared in water by thermolysis of a single precursor ((2,2' bpy)Cd(SC{O}Ph2)) and the thioglycerol at a constant molar ratio of 1:2.5 and at different refluxing times (from 30' to 5 hours). In particular, the size distribution in the different samples was monitored by AFM measurements. In Figure 1, AFM images recorded on the samples with shortest and longest reaction times, respectively, are reported together with the related size distribution analysis, based on gaussian functions. For the sample refluxed for 30', an average size of 2.2±0.1 nm was determined. On the other hand, for the sample obtained with longer refluxing times, the size distribution appears more complex and two populations can be found: the first with the average size centered at 3.1±0.1 nm and the second (although with lower frequency) having the mean diameter at 4.8±0.3 nm. The size distribution analysis confirmed that the nanocrystal dimensions increased with the refluxing time and underlined that different populations are formed during the nanocrystal growth. In fact, the size histograms showed that, during the growth, the mean diameter increased together with an impressive change in the distribution width. The sample obtained after 30' refluxing presented a broad size distribution (width 2.2 nm), while in the sample obtained with longer refluxing times the most frequent distribution becomes much narrower (width 1.2 nm) and a very broad nanocrystal population (width 6.3 nm) appeared. Since the samples were obtained from the same preparation procedure and contained the same capping agent concentration, the dimension change cannot be attributed to a stabilizer effect. This behaviour can be explained considering that the nanocrystal growth is controlled by surface processes. Most likely the growth is because

The characterization of particulates or colloidal nanoparticles in the presence of protein was used to obtain valuable information on the nanoparticle-protein interactions and eventually on the disposition of the macromolecules with respect to the particles. The presented results will be discussed in terms of experimental conditions to enhance or to quench the particulate-biomolecule interaction in order to control the stability of hybrid

Wet chemical synthesis for colloidal nanoparticle preparation have recently attracted much attention with the aim to optimize the procedures to work in mild conditions (atmospheric pressure, temperature below 100°C); in these conditions, the colloidal samples can be easily characterized by polydisperse size distributions and non-homogeneous shapes. AFM imaging can provide a fast investigation tool to characterize nanoparticle preparations without a prior knowledge of the size distributions and shape. Furthermore, the acquisition of AFM data can give valuable information on the thickness of the stabilizer shell, which has to be necessarily used to control the nanoparticle growth in solution and it is worth to be taken into account as particle constituent. For nanomaterials, the size distribution, surface area, shape, aggregation state and composition strongly affect their biological activity since these properties have an influence on their interactions with biomolecules. AFM in tapping mode has been used to study nanoparticles deposited on mica and to investigate their

**2.1 Dimensional characterization of colloidal nanoparticles and particulates** 

AFM topography imaging was helpful to obtain information on the growth mechanism of CdS nanocrystals prepared in water by thermolysis of a single precursor ((2,2' bpy)Cd(SC{O}Ph2)) and the thioglycerol at a constant molar ratio of 1:2.5 and at different refluxing times (from 30' to 5 hours). In particular, the size distribution in the different samples was monitored by AFM measurements. In Figure 1, AFM images recorded on the samples with shortest and longest reaction times, respectively, are reported together with the related size distribution analysis, based on gaussian functions. For the sample refluxed for 30', an average size of 2.2±0.1 nm was determined. On the other hand, for the sample obtained with longer refluxing times, the size distribution appears more complex and two populations can be found: the first with the average size centered at 3.1±0.1 nm and the second (although with lower frequency) having the mean diameter at 4.8±0.3 nm. The size distribution analysis confirmed that the nanocrystal dimensions increased with the refluxing time and underlined that different populations are formed during the nanocrystal growth. In fact, the size histograms showed that, during the growth, the mean diameter increased together with an impressive change in the distribution width. The sample obtained after 30' refluxing presented a broad size distribution (width 2.2 nm), while in the sample obtained with longer refluxing times the most frequent distribution becomes much narrower (width 1.2 nm) and a very broad nanocrystal population (width 6.3 nm) appeared. Since the samples were obtained from the same preparation procedure and contained the same capping agent concentration, the dimension change cannot be attributed to a stabilizer effect. This behaviour can be explained considering that the nanocrystal growth is controlled by surface processes. Most likely the growth is because

materials.

**2. Results** 

interactions with proteins and DNA.

Fig. 1. 3-D topography images of CdS nanocrystal refluxed with thioglycerol for 30' (a) and 5 hours (b) together with their relative height distributions (c, d respectively)

the diffusion of the seeds on the nuclei surface is quite rapid, and therefore it leads to a very broad size. Furthermore, the difficulties to control the growth lead to the development of defects in the crystal structures as confirmed by luminescence studies which show trap states emission (Latterini & Amelia, 2009).

AFM Measurements to Investigate Particulates

and Their Interactions with Biological Macromolecules 91

Fig. 2. (upper panel) AFM images in topography (a) and phase (b) mode of gold

nanoparticles upon interaction with bacterial DNA.

panel) 2-D (c) and 3-D (d) topography images of gold nanoparticles prepared with

nanoparticles stabilized by citrate cations prepared with [Au(III)]/[citrate] of 1:14; (middle

[Au(III)]/[citrate] of 1:7; (lower panel) AFM images in topography (e) and phase (f) of gold

In the case of metal nanoparticles suspensions, the comparison between topography and phase images allowed us to make the hypothesis that the stabilizer shell dimensions cannot be neglected. Gold nanoparticles were prepared in water upon in-situ reduction of Au(III) by citrate anions, which play the double role of reduction agent and stabilizer. AFM images showed isolated nanoparticles with a spherical shape (Figure 2a). The phase images (Figure 2b), recorded simultaneously with the topography images, have shown different contrast for every single grain; indeed a brighter spot corresponding to a higher oscillation phase was observed inside every grain in the phase imaging mode. Similar differences in contrast were not observed in the topography images, suggesting that the grain is actually a nanocomposite material having components which interact differently with the AFM tip. Thus a hypothesis was made that in the chemical composition of colloidal nanoparticles an important component is the organic stabilizer. This hypothesis was further supported by TEM images and from the comparison between AFM and TEM size distribution, an estimate of the stabilizer shell thickness of few nm, depending on the experimental conditions during the synthesis, can be obtained.

In order to explore the effect of citrate ion concentration on the properties of particles, preparations were carried out keeping constant the Au(III) amount and reducing to one half the citrate concentration. AFM images indicated that with lower citrate concentrations the average particles size was smaller (12±0.3 nm compared to 20±0.2 nm obtained by doubling the citrate content) and the distribution of the dimensions was narrower. These observations indicated that the increase of citrate concentration induced a faster and more efficient nucleation process and allowed better control of the particle growth through a diffusion controlled process, although a thickening of the stabilizer shell cannot be excluded.

Silica nanoparticles prepared via the Stöber method could be easily visualized and characterized through AFM scanning, once the suspension was spin-coated on a mica support (Figure 3a). AFM acquisitions show the spherical shape of the nanoparticles with an averaged diameter of 70 nm as a result of a quite narrow distribution. Additionally, the nanoparticle surface appeared regular and without roughness (Figure 3b). The lack of observing pores on the nanoparticle surface by AFM scanning was most likely because the cavities are smaller than the AFM tips (about 1 nm). Generally the void particles appear well separated on mica, indicating that the surface charges act as efficient capping agents. When the silica particle surface is covalently functionalized with organic dyes, such as fluorescein or 9-aminoacridine, the particle height resulted increased by a factor of two or three (Figure 3c) and the grains do not appear isolated any more, as already observed for similar systems (Latterini & Amelia, 2009). These morphology changes were attributed to the presence of the aromatic dye molecules on the particle surface which reduce the net charge and are able to form aggregate species stabilized by π-π stacking. The occurrence of these aggregate species might strongly be reduced in suspension samples for the presence of solvation interactions, but they are predominant in solid state and can strongly affect the chemical-physical behaviour of the samples. Thus attention should be paid in the detection of these aggregated species when devices are prepared from suspensions. AFM is one of the few methods which allows one to visualize the formation of these assemblies.

The particulates produced in working environments during material processing were collected through a standard device which was designed to collect and separate aerosol through dimensional properties. Briefly, a Sioutas Cascade Impactor provides a five step

In the case of metal nanoparticles suspensions, the comparison between topography and phase images allowed us to make the hypothesis that the stabilizer shell dimensions cannot be neglected. Gold nanoparticles were prepared in water upon in-situ reduction of Au(III) by citrate anions, which play the double role of reduction agent and stabilizer. AFM images showed isolated nanoparticles with a spherical shape (Figure 2a). The phase images (Figure 2b), recorded simultaneously with the topography images, have shown different contrast for every single grain; indeed a brighter spot corresponding to a higher oscillation phase was observed inside every grain in the phase imaging mode. Similar differences in contrast were not observed in the topography images, suggesting that the grain is actually a nanocomposite material having components which interact differently with the AFM tip. Thus a hypothesis was made that in the chemical composition of colloidal nanoparticles an important component is the organic stabilizer. This hypothesis was further supported by TEM images and from the comparison between AFM and TEM size distribution, an estimate of the stabilizer shell thickness of few nm, depending on the experimental conditions during

In order to explore the effect of citrate ion concentration on the properties of particles, preparations were carried out keeping constant the Au(III) amount and reducing to one half the citrate concentration. AFM images indicated that with lower citrate concentrations the average particles size was smaller (12±0.3 nm compared to 20±0.2 nm obtained by doubling the citrate content) and the distribution of the dimensions was narrower. These observations indicated that the increase of citrate concentration induced a faster and more efficient nucleation process and allowed better control of the particle growth through a diffusion

Silica nanoparticles prepared via the Stöber method could be easily visualized and characterized through AFM scanning, once the suspension was spin-coated on a mica support (Figure 3a). AFM acquisitions show the spherical shape of the nanoparticles with an averaged diameter of 70 nm as a result of a quite narrow distribution. Additionally, the nanoparticle surface appeared regular and without roughness (Figure 3b). The lack of observing pores on the nanoparticle surface by AFM scanning was most likely because the cavities are smaller than the AFM tips (about 1 nm). Generally the void particles appear well separated on mica, indicating that the surface charges act as efficient capping agents. When the silica particle surface is covalently functionalized with organic dyes, such as fluorescein or 9-aminoacridine, the particle height resulted increased by a factor of two or three (Figure 3c) and the grains do not appear isolated any more, as already observed for similar systems (Latterini & Amelia, 2009). These morphology changes were attributed to the presence of the aromatic dye molecules on the particle surface which reduce the net charge and are able to form aggregate species stabilized by π-π stacking. The occurrence of these aggregate species might strongly be reduced in suspension samples for the presence of solvation interactions, but they are predominant in solid state and can strongly affect the chemical-physical behaviour of the samples. Thus attention should be paid in the detection of these aggregated species when devices are prepared from suspensions. AFM is one of the few methods which

The particulates produced in working environments during material processing were collected through a standard device which was designed to collect and separate aerosol through dimensional properties. Briefly, a Sioutas Cascade Impactor provides a five step

controlled process, although a thickening of the stabilizer shell cannot be excluded.

allows one to visualize the formation of these assemblies.

the synthesis, can be obtained.

Fig. 2. (upper panel) AFM images in topography (a) and phase (b) mode of gold nanoparticles stabilized by citrate cations prepared with [Au(III)]/[citrate] of 1:14; (middle panel) 2-D (c) and 3-D (d) topography images of gold nanoparticles prepared with [Au(III)]/[citrate] of 1:7; (lower panel) AFM images in topography (e) and phase (f) of gold nanoparticles upon interaction with bacterial DNA.

AFM Measurements to Investigate Particulates

and Their Interactions with Biological Macromolecules 93

collected in environments where blade are used (such as for wood processing) presented particles with quite sharp edges. Since the recent literature evidenced that the particle shape and size can affect their delivery and toxicity (Lewinski et al., 2008), the creation of a database containing the characterization of particulates produced in industrial working locations is particularly important to reduce the negative effects to personnel from exposure to these particulates within the working environment. Furthermore, the dimensional characterization has to be investigated in deeper details and AFM imaging provides a fast investigation tool which can give high resolution information. AFM topography images showed that the micron-size particulates collected in places where digging operations are carried out, or during metal processing, are constituted by smaller particles with dimensions between 15 and 100 nm. Even the samples desorbed from the collection filters with higher dimensional cut (Figure 4a, b and d) are constituted by smaller nanoparticles which form agglomerates with bigger dimensions. However, within the agglomerates, the nanostructure is maintained, as shown by the jagged linescan (Figure 4c) which presents steps about 25 nm

height and can be attributed to the single nanoparticles composing the agglomerate.

Fig. 4. (upper panel) AFM images representing the topography (a,b) and x-scan line (c) of nanoparticulate collected during digging operations (cut-off filter = 0.25 µm); (lower panel)

AFM images representing the topography of nanoparticulate collected during metal welding operations (cut-off filter = 0.25 µm) in the absence (d) and in the presence of bacterial DNA (e) together with x-scan line graph (f) taken from the image (e).

**2.2 Investigations of the interactions between nanoparticles and biomolecules** 

The interactions between colloidal nanoparticles and biomolecules were investigated by AFM through an analysis of the grain dimensions and morphology and the data in the absence of the biomolecules compared to those obtained in the presence of biomolecules.

Fig. 3. (upper panel) AFM images in topography (a) and x-scan line (b) of void silica nanoparticles; (lower panel) AFM images in topography of fluorescein-functionalized silica nanoparticles (c) and void silica nanoparticles (d) in the presence of BSA.

collection which corresponds to the following 50% cut-point of 2.5 µm, 1.0 µm, 0.5 µm, 0.25 µm (filters A, B, C and D, respectively) on a 25 mm PTFE filter. The Impactor has a final step to collect the particles below the < 0.25 µm cut – point on a 37 mm PTFE filter (filter AF) equipped with a sample pump capable of maintaining a constant flow rate (about 9 l/min). For the morphological/dimensional characterization of the particulate through AFM imaging, the collected particulate was desorbed from the collection filters, since the latter presented a very rough surface which did not allow to have enough resolution. Each filter was transferred in 10 mL vials; in each vial 5 mL of water were added. The vials were then sealed and the desorption was carried out by ultrasonication for 20 minutes at room temperature. The morphological analysis was carried out upon deposition of the obtained suspensions on mica. The AFM images were collected in tapping mode in order to avoid sample degradation or removal. The AFM images show that the shape of the particulates formed is influenced by the nature of the working processes taking place during the sample collection, as well as the environmental conditions (temperature, pressure, material concentration). In particular, spherical objects were observed from the samples collected in places where digging process were carried out or where metals were treated at high temperatures, while the samples

Fig. 3. (upper panel) AFM images in topography (a) and x-scan line (b) of void silica nanoparticles; (lower panel) AFM images in topography of fluorescein-functionalized silica

collection which corresponds to the following 50% cut-point of 2.5 µm, 1.0 µm, 0.5 µm, 0.25 µm (filters A, B, C and D, respectively) on a 25 mm PTFE filter. The Impactor has a final step to collect the particles below the < 0.25 µm cut – point on a 37 mm PTFE filter (filter AF) equipped with a sample pump capable of maintaining a constant flow rate (about 9 l/min). For the morphological/dimensional characterization of the particulate through AFM imaging, the collected particulate was desorbed from the collection filters, since the latter presented a very rough surface which did not allow to have enough resolution. Each filter was transferred in 10 mL vials; in each vial 5 mL of water were added. The vials were then sealed and the desorption was carried out by ultrasonication for 20 minutes at room temperature. The morphological analysis was carried out upon deposition of the obtained suspensions on mica. The AFM images were collected in tapping mode in order to avoid sample degradation or removal. The AFM images show that the shape of the particulates formed is influenced by the nature of the working processes taking place during the sample collection, as well as the environmental conditions (temperature, pressure, material concentration). In particular, spherical objects were observed from the samples collected in places where digging process were carried out or where metals were treated at high temperatures, while the samples

nanoparticles (c) and void silica nanoparticles (d) in the presence of BSA.

collected in environments where blade are used (such as for wood processing) presented particles with quite sharp edges. Since the recent literature evidenced that the particle shape and size can affect their delivery and toxicity (Lewinski et al., 2008), the creation of a database containing the characterization of particulates produced in industrial working locations is particularly important to reduce the negative effects to personnel from exposure to these particulates within the working environment. Furthermore, the dimensional characterization has to be investigated in deeper details and AFM imaging provides a fast investigation tool which can give high resolution information. AFM topography images showed that the micron-size particulates collected in places where digging operations are carried out, or during metal processing, are constituted by smaller particles with dimensions between 15 and 100 nm. Even the samples desorbed from the collection filters with higher dimensional cut (Figure 4a, b and d) are constituted by smaller nanoparticles which form agglomerates with bigger dimensions. However, within the agglomerates, the nanostructure is maintained, as shown by the jagged linescan (Figure 4c) which presents steps about 25 nm height and can be attributed to the single nanoparticles composing the agglomerate.

Fig. 4. (upper panel) AFM images representing the topography (a,b) and x-scan line (c) of nanoparticulate collected during digging operations (cut-off filter = 0.25 µm); (lower panel) AFM images representing the topography of nanoparticulate collected during metal welding operations (cut-off filter = 0.25 µm) in the absence (d) and in the presence of bacterial DNA (e) together with x-scan line graph (f) taken from the image (e).

#### **2.2 Investigations of the interactions between nanoparticles and biomolecules**

The interactions between colloidal nanoparticles and biomolecules were investigated by AFM through an analysis of the grain dimensions and morphology and the data in the absence of the biomolecules compared to those obtained in the presence of biomolecules.

AFM Measurements to Investigate Particulates

and Their Interactions with Biological Macromolecules 95

Fig. 5. AFM images representing the topography (a) of polystyrene NPs deposited on mica

Fig. 6. (upper panel) AFM images representing the topography (a) and phase (b) of

polystyrene NP surface before (c) and after (d) BSA adsorption.

polystyrene NPs deposited on mica after BSA adsorption; (lower panel) 3-D AFM image of a

and relative size distribution built up from AFM images in (b).

Generally for all the colloidal nanoparticles under investigation, a marked increase in grain dimensions was observed upon interaction with protein or bacterial DNA. In particular gold nanoparticles bearing citrate ions on the surface interact efficiently with bacterial DNA. The interaction is so strong to be optically visualized by colour changes of the gold suspensions; the well know, intense red colour of gold suspensions turns to an intense blue upon addition of DNA (about 10-4 M in base pair). This behaviour is obviously due to modifications of the Surface Plasmon Resonance (SPR) of the gold colloids, which is a deeply investigated phenomenon due to the potential application for sensing and labelling (Latterini & Tarpani, 2011). However, a much weaker effect can be observed when the single DNA base or mixtures of bases are added to gold colloids, thus the effect has to be related to DNA structure. AFM images recorded on gold-DNA complex deposited on mica (Figure 2ef) show that the colloids are no longer detectable as individuals, but the samples are instead characterized by supramolecular architectures whose dimensions can reach the μm scale. This observation, together with the SPR shift to longer wavelength, suggested that DNA strands tend to accumulate around the metal particles likely replacing, at least in part, the citrate anions leading to micron-size aggregates formation. Inside these aggregates, gold colloids come into closer contact, as highlighted by the SPR shift, which is in agreement with literature data (Ghosh & Pal, 2007). The lack of clearly detecting the metal nanostructure even in phase mode is probably due to the fact that they are buried inside the biological layer which is estimated to be tens of nm thick if the average diameter of the pristine gold nanoparticles (12±0.3 nm) is taken into account.

A similar aggregation phenomenon was observed also when bacterial or calf thymus DNA solutions were added to the suspensions of particulates collected from metal welding operations. In this case the metal nanoparticles are not intentionally prepared and stabilized thus interactions with DNA strands are enhanced to reach a better stabilization in the water media. As a results, particles with dimensions below 25 nm (Figure 4d) in the presence of DNA form aggregate structures with an overall dimension in the order of hundreds of nm.

A clustering effect was observed for silica nanoparticles when they were topographically imaged in the presence of Bovine Serum Albumine (BSA). In particular, the grain dimensions increased when the void silica nanoparticles were deposited in the presence of BSA; for 80 nm diameter particle, an increase by a factor of 4 was observed in the height and a larger effect was observed in the width (Figure 3d). These effects have been attributed to the adsorption of the protein on the surface of the silica nanoparticles, as previously observed for similar systems (Bellezza et al., 2009; Latterini & Amelia, 2009). Indeed, the net negative charge present on the void silica nanoparticles in aqueous neutral media can have an important role in controlling the adsorption of the protein which presents a positive net surface charge in the same pH conditions. This adsorption process resulted in a shielding effect from the negative charges which stabilized the naked particle and maintained isolation; thus the silica nanoparticles with BSA adsorbed on the surface tend to form clustered structures. However, no clear evidence was obtained by AFM to determine the conformation of the protein on the surface of the particles.

AFM can be also a valid means to study and comprehend the mechanism behind the interaction between organic nanomaterials and biomolecules. The protein Bovine Serum Albumin (BSA) is used as model biomolecule to investigate its interaction with polystyrene nanoparticles (PS NPs) synthesized in our group.

Generally for all the colloidal nanoparticles under investigation, a marked increase in grain dimensions was observed upon interaction with protein or bacterial DNA. In particular gold nanoparticles bearing citrate ions on the surface interact efficiently with bacterial DNA. The interaction is so strong to be optically visualized by colour changes of the gold suspensions; the well know, intense red colour of gold suspensions turns to an intense blue upon addition of DNA (about 10-4 M in base pair). This behaviour is obviously due to modifications of the Surface Plasmon Resonance (SPR) of the gold colloids, which is a deeply investigated phenomenon due to the potential application for sensing and labelling (Latterini & Tarpani, 2011). However, a much weaker effect can be observed when the single DNA base or mixtures of bases are added to gold colloids, thus the effect has to be related to DNA structure. AFM images recorded on gold-DNA complex deposited on mica (Figure 2ef) show that the colloids are no longer detectable as individuals, but the samples are instead characterized by supramolecular architectures whose dimensions can reach the μm scale. This observation, together with the SPR shift to longer wavelength, suggested that DNA strands tend to accumulate around the metal particles likely replacing, at least in part, the citrate anions leading to micron-size aggregates formation. Inside these aggregates, gold colloids come into closer contact, as highlighted by the SPR shift, which is in agreement with literature data (Ghosh & Pal, 2007). The lack of clearly detecting the metal nanostructure even in phase mode is probably due to the fact that they are buried inside the biological layer which is estimated to be tens of nm thick if the average diameter of the pristine gold

A similar aggregation phenomenon was observed also when bacterial or calf thymus DNA solutions were added to the suspensions of particulates collected from metal welding operations. In this case the metal nanoparticles are not intentionally prepared and stabilized thus interactions with DNA strands are enhanced to reach a better stabilization in the water media. As a results, particles with dimensions below 25 nm (Figure 4d) in the presence of DNA form aggregate structures with an overall dimension in the order of hundreds of nm. A clustering effect was observed for silica nanoparticles when they were topographically imaged in the presence of Bovine Serum Albumine (BSA). In particular, the grain dimensions increased when the void silica nanoparticles were deposited in the presence of BSA; for 80 nm diameter particle, an increase by a factor of 4 was observed in the height and a larger effect was observed in the width (Figure 3d). These effects have been attributed to the adsorption of the protein on the surface of the silica nanoparticles, as previously observed for similar systems (Bellezza et al., 2009; Latterini & Amelia, 2009). Indeed, the net negative charge present on the void silica nanoparticles in aqueous neutral media can have an important role in controlling the adsorption of the protein which presents a positive net surface charge in the same pH conditions. This adsorption process resulted in a shielding effect from the negative charges which stabilized the naked particle and maintained isolation; thus the silica nanoparticles with BSA adsorbed on the surface tend to form clustered structures. However, no clear evidence was obtained by AFM to determine the

AFM can be also a valid means to study and comprehend the mechanism behind the interaction between organic nanomaterials and biomolecules. The protein Bovine Serum Albumin (BSA) is used as model biomolecule to investigate its interaction with polystyrene

nanoparticles (12±0.3 nm) is taken into account.

conformation of the protein on the surface of the particles.

nanoparticles (PS NPs) synthesized in our group.

Fig. 5. AFM images representing the topography (a) of polystyrene NPs deposited on mica and relative size distribution built up from AFM images in (b).

Fig. 6. (upper panel) AFM images representing the topography (a) and phase (b) of polystyrene NPs deposited on mica after BSA adsorption; (lower panel) 3-D AFM image of a polystyrene NP surface before (c) and after (d) BSA adsorption.

AFM Measurements to Investigate Particulates

particles with dimensions between 15 and 100 nm.

providing the samples collected in working environments.

*25*, pp 10918–10924, ISSN 0743-7463

to establish the BSA orientation.

**4. Acknowledgment** 

**5. References** 

and Their Interactions with Biological Macromolecules 97

nanoparticles indicated that the growth could occur through a diffusion controlled process. Interestingly, the comparison between topography and phase images allowed us to make the hypothesis that the stabilizer shell around the particles has a dimension of few nm thus colloidal nanoparticles can be better regarded as nanocomposites. Silica nanoparticles prepared through a sol-gel method were successfully imaged in topography mode and

AFM appears to be a valid tool also for a fast and high resolution analysis of particulates collected in working environments. Thus AFM imaging can be useful for the creation of a database on dimension and morphology of particulates produced in different working environments in order to evaluate their toxicity in relation to the tools and the conditions used. AFM topography images showed that the micron-size particulates collected in places where digging or welding operation are carried out are actually constituted by smaller

AFM is a valid mean to study and comprehend the interactions between nanomaterials and biomolecules. Generally for all the investigated nanoparticles, a marked increase in grain dimensions was observed upon interaction with protein or DNA. AFM images recorded on nanoparticle-biomolecule conjugates demonstrated that the effect is due to the formation of supramolecular architectures whose dimensions can reach the μm scale, in which electrostatic interactions might have an important role. Only in the case of polystyrene particles with 220 nm diameter, the BSA molecules adsorbed on their surface are arranged in an ordered conformation. The line-scan analysis through topographic images allowed us

This work is supported both by the University of Perugia and the Department of the University for the Scientific and Technological Research (MIUR-Rome). Authors are grateful to INAIL for financial support through a research agreement (May 2010-2012) and for

Amelia, M.; Flamini, R.; Latterini L. (2010). Recovery of CdS nanocrystal defects through conjugation with proteins. *Langmuir*, Vol. *26*, pp 10129–10134, ISSN 0743-7463 Bellezza, F.; Cipiciani, A.; Latterini, L.; Posati, T.; Sassi,P. (2009). Structure and Catalytic

Dedecker, P.; Hotta, J.I.; Flors, C.; Sliwa, M.; Uji-I, H.; Roeffaers, M.B.J.; Ando, R.; Mizuno,

*Soc.,* Vol.129, No.51, (December 2007), pp. 16132-16141, ISSN 0002-7863 García, R. & Pérez, R. (2002). Dynamic atomic force microscopy methods. *Surface Science* 

*Reports,* Vol.47, No.6-8, (April 2002), pp. 197-301, ISSN 0167-5729

Behaviour of Myoglobin adsorbed onto Nanosized Hydrotalcites. *Langmuir*, Vol.

H.; Miyawaki, A. & Hofkens, J. (2007). Subdiffraction imaging through the selective donut-mode depletion of thermally stable photoswitchable fluorophores: numerical analysis and application to the fluorescent protein Dronpa. *J. Am. Chem.* 

appeared well dispersed, with a narrow size distribution and a smooth surface.

AFM topography images of a PS NPs sample deposited on mica by spin-coating demonstrate the presence of spherical particles with a smooth surface (Figure 5a). The height histogram built up from the AFM images (taking into account at least 500 particles) indicates that the nanoparticles are quite polydisperse with a mean diameter of about 230 nm (Figure 5b). A 10-3 M aqueous solution of BSA was then added to the synthesized PS NPs and AFM topography images were collected after deposition on mica. Upon interaction with the protein, the images clearly show the formation of aggregates with an elongated shape but the same Z-height of the single nanoparticles (Figure 6a-b). The data seem to indicate that the adsorbed protein acts as a linker between the nanostructures binding them together in groups of three or four. It is known in literature (Yoon et al., 1996) that BSA can be adsorbed on a surface according to two different orientations: side-on, in which the longer side (14 nm) adheres to the surface or end-on, in which the shorter side (4 nm) is involved in the adsorption. A schematic representation of these two types of interaction is shown in Figure 7b. In this particular case, topography images in high resolution of the PS NPs surface were taken after BSA adsorption. The resulting 3-D topographic images demonstrate that upon interaction with BSA (Figure 6d) there is an increase of the surface roughness and the formation of a single protein layer adsorbed on the polystyrene nanoparticles. As shown by the x-scan profile (Figure 7a), this layer has a height of about 4 nm, thus confirming that BSA is adsorbed onto the polymeric NPs in the side-on orientation.

Fig. 7. (a) X-scan line graph of polystyrene NPs surface before (gray line) and after (black line) BSA adsorption; (b) Scheme of the possible orientations of BSA adsorbed on a solid surface

#### **3. Conclusions**

AFM scanning has been used to characterize, from a dimensional and morphological point of view, colloidal nanoparticles prepared intentionally with designed properties and particulates collected in working environments. The data obtained from AFM topography imaging, once statistically analyzed, were helpful to obtain information on the growth mechanism of CdS nanocrystals and gold nanoparticles. Indeed, a broadening of size distribution of CdS colloids suggested that the growth was mainly controlled by surface processes; on the other hand, the narrowing of dimensional populations for gold

AFM topography images of a PS NPs sample deposited on mica by spin-coating demonstrate the presence of spherical particles with a smooth surface (Figure 5a). The height histogram built up from the AFM images (taking into account at least 500 particles) indicates that the nanoparticles are quite polydisperse with a mean diameter of about 230 nm (Figure 5b). A 10-3 M aqueous solution of BSA was then added to the synthesized PS NPs and AFM topography images were collected after deposition on mica. Upon interaction with the protein, the images clearly show the formation of aggregates with an elongated shape but the same Z-height of the single nanoparticles (Figure 6a-b). The data seem to indicate that the adsorbed protein acts as a linker between the nanostructures binding them together in groups of three or four. It is known in literature (Yoon et al., 1996) that BSA can be adsorbed on a surface according to two different orientations: side-on, in which the longer side (14 nm) adheres to the surface or end-on, in which the shorter side (4 nm) is involved in the adsorption. A schematic representation of these two types of interaction is shown in Figure 7b. In this particular case, topography images in high resolution of the PS NPs surface were taken after BSA adsorption. The resulting 3-D topographic images demonstrate that upon interaction with BSA (Figure 6d) there is an increase of the surface roughness and the formation of a single protein layer adsorbed on the polystyrene nanoparticles. As shown by the x-scan profile (Figure 7a), this layer has a height of about 4 nm, thus confirming that BSA is adsorbed onto the polymeric NPs in the side-on orientation.

Fig. 7. (a) X-scan line graph of polystyrene NPs surface before (gray line) and after (black line) BSA adsorption; (b) Scheme of the possible orientations of BSA adsorbed on a solid

AFM scanning has been used to characterize, from a dimensional and morphological point of view, colloidal nanoparticles prepared intentionally with designed properties and particulates collected in working environments. The data obtained from AFM topography imaging, once statistically analyzed, were helpful to obtain information on the growth mechanism of CdS nanocrystals and gold nanoparticles. Indeed, a broadening of size distribution of CdS colloids suggested that the growth was mainly controlled by surface processes; on the other hand, the narrowing of dimensional populations for gold

surface

**3. Conclusions** 

nanoparticles indicated that the growth could occur through a diffusion controlled process. Interestingly, the comparison between topography and phase images allowed us to make the hypothesis that the stabilizer shell around the particles has a dimension of few nm thus colloidal nanoparticles can be better regarded as nanocomposites. Silica nanoparticles prepared through a sol-gel method were successfully imaged in topography mode and appeared well dispersed, with a narrow size distribution and a smooth surface.

AFM appears to be a valid tool also for a fast and high resolution analysis of particulates collected in working environments. Thus AFM imaging can be useful for the creation of a database on dimension and morphology of particulates produced in different working environments in order to evaluate their toxicity in relation to the tools and the conditions used. AFM topography images showed that the micron-size particulates collected in places where digging or welding operation are carried out are actually constituted by smaller particles with dimensions between 15 and 100 nm.

AFM is a valid mean to study and comprehend the interactions between nanomaterials and biomolecules. Generally for all the investigated nanoparticles, a marked increase in grain dimensions was observed upon interaction with protein or DNA. AFM images recorded on nanoparticle-biomolecule conjugates demonstrated that the effect is due to the formation of supramolecular architectures whose dimensions can reach the μm scale, in which electrostatic interactions might have an important role. Only in the case of polystyrene particles with 220 nm diameter, the BSA molecules adsorbed on their surface are arranged in an ordered conformation. The line-scan analysis through topographic images allowed us to establish the BSA orientation.

### **4. Acknowledgment**

This work is supported both by the University of Perugia and the Department of the University for the Scientific and Technological Research (MIUR-Rome). Authors are grateful to INAIL for financial support through a research agreement (May 2010-2012) and for providing the samples collected in working environments.

#### **5. References**


**5** 

Taiji Ikawa

*Japan* 

**AFM Imaging of Biological Supramolecules by** 

Biologically derived molecules (biomolecules) are extremely diverse in their physical sizes, chemical and structural properties. They form supramolecular assemblies *in vivo*/*vitro* through noncovalent interactions (e.g., hydrogen bonding, hydrophobic interactions, π-π interactions, and/or electrostatic). The structures of the supramolecular assemblies change with the concentrations of salts and the biomolecules itself. Efficient immobilization of various biomolecules and their assemblies is a key aspect of many applications including microarray technologies, (Kambhampati (Ed.), 2003; Schena (Ed.), 2004) biotechnology in

Structures and functions of the biomolecules and their assemblies are susceptible to physical and chemical surface properties and nanotopography of the substrate, and such interfacial forces effect a nanoscale change in molecular shape and structure. (Ostuni, et al., 2001; Ramsden, 1993; Wahlgren & Arnebrant, 1993) The first problem to be overcome is the tendency for biomolecules to denature on contact with the substrate surfaces. Extensive approaches have been developed, using either covalent attachment or noncovalent affinity binding (Mayers, 2002). The covalent coupling process can achieve stable coupling, but it needs complexity and cost of derivation steps, and limited sites for attachment leads to shorter lifetime. The process has a possibility of denaturation by the chemical treatment. On the other hand, the noncovalent affinity binding process is the simplest approach to the immobilization but it tends not to be stable, and activity of biomolecule is often lost in timedependent structural changes (Ramsden, 1993). For example, mica surface provides an atomically flat surface, but the surface repels most of the biomolecules due to its negative charge. Multivalent cation or chemical modification process are used to avoid repulsion (Bezanilla et al.,1995; Hansma, 2001; Lamture et al., 1994), however, the structures of the supramolecular assemblies changed with the concentrations of salts (Wong et al., 2003).

A recent study for the noncovalent affinity binding process has been directed toward the selective adsorption of biomolecules using nanopatterned surfaces (Cunin et al., 2001; Curtis & Eilkinson, 2001; Shi et al.,1999) and/or molecularly imprinted polymers (Alexander et al., 2003; Haupt, 2003) so as to hold the 3-dimensional structure of the biomolecules. However, these approaches have met with limited success due to their complicated chemical processes

and the often expensive facilities required for nanofabrication.

general (Mayers, 2002; Whitesides, 2001) and structural analysis based on AFM.

**1. Introduction** 

**a Molecular Imprinting-Based Immobilization** 

**Process on a Photopolymer** 

*Toyota Central Research and Development Laboratories, Inc.* 

