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Boron Nitride Nanotube as an Antimicrobial Peptide Carrier: A Theoretical Insight

Authors Zarghami Dehaghani M, Bagheri B, Yousefi F, Nasiriasayesh A, Hamed Mashhadzadeh A, Zarrintaj P, Rabiee N, Bagherzadeh M, Fierro V, Celzard A, Saeb MR, Mostafavi E

Received 22 December 2020

Accepted for publication 18 February 2021

Published 4 March 2021 Volume 2021:16 Pages 1837—1847

DOI https://doi.org/10.2147/IJN.S298699

Checked for plagiarism Yes

Review by Single anonymous peer review

Peer reviewer comments 3

Editor who approved publication: Professor Israel (Rudi) Rubinstein


Maryam Zarghami Dehaghani,1,* Babak Bagheri,2,* Farrokh Yousefi,3 Abbasali Nasiriasayesh,4 Amin Hamed Mashhadzadeh,5 Payam Zarrintaj,6 Navid Rabiee,7 Mojtaba Bagherzadeh,7 Vanessa Fierro,8 Alain Celzard,8 Mohammad Reza Saeb,5 Ebrahim Mostafavi9,10

1School of Chemical Engineering, College of Engineering, University of Tehran, Tehran, Iran; 2Department of Chemical and Biomolecular Engineering, Korea Advanced Institute of Science and Technology (KAIST), Daejeon, Republic of Korea; 3Department of Physics, University of Zanjan, Zanjan, 45195-313, Iran; 4Industrial Management Institute, Tehran, Iran; 5Center of Excellence in Electrochemistry, School of Chemistry, College of Science, University of Tehran, Tehran, 14155-6455, Iran; 6School of Chemical Engineering, Oklahoma State University, Stillwater, OK, 74078, USA; 7Department of Chemistry, Sharif University of Technology, Tehran, Iran; 8Université De Lorraine, CNRS, IJL, Epinal, 88000, France; 9Stanford Cardiovascular Institute, Stanford, CA, USA; 10Department of Medicine, Stanford University School of Medicine, Stanford, CA, USA

*These authors contributed equally to this work

Correspondence: Ebrahim Mostafavi
Stanford Cardiovascular Institute, Stanford University School of Medicine, Stanford, CA, USA
Email [email protected]
Amin Hamed Mashhadzadeh
Center of Excellence in Electrochemistry, School of Chemistry, College of Science, University of Tehran, Tehran, 14155-6455, Iran
Email [email protected]

Introduction: Nanotube-based drug delivery systems have received considerable attention because of their large internal volume to encapsulate the drug and the ability to penetrate tissues, cells, and bacteria. In this regard, understanding the interaction between the drug and the nanotube to evaluate the encapsulation behavior of the drug in the nanotube is of crucial importance.
Methods: In this work, the encapsulation process of the cationic antimicrobial peptide named cRW3 in the biocompatible boron nitride nanotube (BNNT) was investigated under the Canonical ensemble (NVT) by molecular dynamics (MD) simulation.
Results: The peptide was absorbed into the BNNT by van der Waals (vdW) interaction between cRW3 and the BNNT, in which the vdW interaction decreased during the simulation process and reached the value of − 142.7 kcal·mol− 1 at 4 ns.
Discussion: The increase in the potential mean force profile of the encapsulated peptide during the pulling process of cRW3 out of the nanotube showed that its insertion into the BNNT occurred spontaneously and that the inserted peptide had the desired stability. The energy barrier at the entrance of the BNNT caused a pause of 0.45 ns when half of the peptide was inside the BNNT during the encapsulation process. Therefore, during this period, the peptide experienced the weakest movement and the smallest conformational changes.

Keywords: boron nitride nanotube, drug delivery, antimicrobial peptide, molecular dynamic simulation, encapsulation

Introduction

Since the introduction of the first antimicrobial drug in the 1960s, penicillin, tremendous progress has been made in the treatment of infections.1 However, many obstacles have been encountered in the healing of microbial infections, even with the application of antimicrobial peptides.2 For example, pathogens are believed to be resistant to the specified antibiotic, making scientific research unprofitable.3 In this regard, the field of antimicrobial drug delivery has emerged to pave the way for the treatment of infections.4,5 Through drug delivery systems, the benefits of delivery are maintained and targeted to overcome side effects,6–9 delaying antimicrobial drug resistance,10,11 and protecting the drug against oxidation and catalysis by free radicals and enzymes, respectively.12,13

Nanoparticle-based antimicrobial drug delivery systems consist of biocompatible and non-toxic nanoparticles with a hydrodynamic diameter in the range of 10 to 100 nm that contain encapsulated or attached antimicrobial drugs.14–17 These drug delivery nano-systems are generally classified into six main groups, including solid nanoparticles, polymeric micelles, polymeric nanoparticles, liposomes, viral nanoparticles, and dendrimers.18–21 In addition to the mentioned advantages of drug delivery systems, nanocarriers would provide the benefits of a highly reactive area and the ability to penetrate cells, tissues, and bacteria.22–25

Nanotubes, as fascinating nanovectors, have attracted a lot of attention as drug carriers due to their distinct features such as having an inner volume large enough for drug encapsulation26 and surface functionalization.27–29 In recent decades, carbon nanotubes (CNTs) have been widely used as drug carriers.30 However, the possible cytotoxicity of CNTs has restricted their use in biomedical applications.30,31 Therefore, boron nitride nanotubes (BNNTs) have been introduced as alternatives because of their non-toxicity and biocompatibility due to their structural stability and chemical inertness.32–36 Moreover, because of their higher partial charges than CNTs, BNNTs demonstrate higher water permeation coefficients due to polarisation.37

In this respect, several types of research have been performed to investigate the performance of BNNTs as drug carriers. For example, Mortazavifar et al38 have verified the drug delivery performance of OH-functionalised BNNT using density functional theory (DFT) calculations and molecular dynamic (MD) simulations. According to the adsorption energy calculated by DFT, it was observed that the anticancer drug carmustine (CMT) was bound to the surface of the BNNT via hydrogen bonding with hydroxyl groups on the surface of the nanotube. In addition, they reported that increased CMT concentration and temperature resulted in a higher van der Waals force between OH-functionalised BNNT and the drug molecule. In another work by Roosta et al,39 the encapsulation of gemcitabine in BNNT (18, 0) and the drug release performance using the heterofullerene (C48B12) releasing agent were studied using MD simulations. With regard to encapsulation, the drug was spontaneously located in the center of the BNNT over its entire length due to the negative interaction energy value of −0.9 kcal mol−1. With regard to the release of the encapsulated drug, the C48B12 releasing agent is added to the system and entered the BNNT, resulting in the release of the drug with a total potential energy difference of −140.1 kcal mol−1.

There are critical works in the literature regarding the use of different solvents for potential biomedical applications of BNNTs. Mirhaji et al40 verified the effect of the solvent containing water and ethanol on the encapsulation process of the anticancer drug docetaxel in a BNNT (13, 13) using MD simulations. According to the calculated van der Waals energies, solutions containing 60% and 75% ethanol had a negative effect on the interaction between docetaxel and BNNT. The penetration rate of the carboplatin drug in BNNT and BNNT having 18 hydroxyl groups on one edge was compared in the research of Khatti et al.41 It was observed that the hydroxyl groups facilitated the entry of the drug into the nanotube cavity. Xu et al42 compared the adsorption process of two anticancer drugs, temozolomide (TMZ) and CMT, in the presence of a BNNT (6, 6) as nanovector by DFT calculation. They reported that the energies of drug adsorption on the inner wall of the BNNT were remarkably higher than on the outer wall. Moreover, TMZ was absorbed on the surface of the nanotube with both π–π and electrostatic interactions, which resulted in higher adsorption energy compared to the CMT/BNNT system with only electrostatic interactions.

MD simulation is considered a promising tool for predicting the performances of the systems containing nanostructures in various fields.43,44 In addition to evaluating the mechanical and thermal properties of nanomaterials,45–53 this computational approach provides the ability to evaluate the interatomic interactions in nanoparticle-based complex systems having biomolecules.54 Therefore, in the current work, this method has been applied to study the atomic interactions and conformational changes of the peptide during the insertion process into the BNNT. According to previous research on the encapsulation of drugs in BNNT, the interaction between the nanotube and the drug is a key parameter in the encapsulation process. The drug should indeed pass the potential barrier at the nanotube entrance and, then stabilized via encapsulation process into the deep interior potential. Hence, to evaluate the performance of BNNT as a nanocarrier, it is very important to calculate the Van der Waals interaction between the drug and the nanotube during the encapsulation process, as well as the potential of mean force (PMF) of the encapsulated drug. In this manner, the selected drug, cRW3, is a small cationic antimicrobial peptide and has cyclic structure behavior in the BNNT, as nanocarrier, in an aqueous environment for drug delivery purposes. This effect has been verified by using MD simulations. Followed by that, the drug’s encapsulation in the BNNT was evaluated by estimating the Van der Waals interaction between the drug and the BNNT. In addition, the stability of the drug in the BNNT was investigated by calculating the PMF of the encapsulated drug.

Computational Details

In the present work, the MD calculation was applied using the Large-Scale Atomic/Molecular Simulator (LAMMPS) software55 to verify the encapsulation process of the drug cRW3 in a boron nitride nanotube (BNNT) and, subsequently, the stability of the encapsulated drug in the nanotube. The visualization was obtained using VMD.56 In accordance with the size of cRW3, an armchair BNNT (12,12) with a length of 30 Ȧ has been chosen as the nanocarrier for the drug. The axial direction of the nanotube was taken as the z-axis considered for the simulation box. The drug cRW3 was selected from the protein data bank (ID code 2OTQ). The chemical structure of cRW3 (cyclo-(Arg-Arg-Trp-Phe-Trp-Arg)) is shown in Figure 1. The aromatic groups (tryptophane side chain) are responsible for the hydrophobic feature, while arginine groups are responsible for the hydrophilic part of cRW3.57,58

Figure 1 Amino acids at the basis of the chemical structure of the drug cRW3.

At the beginning of the simulation, cRW3 was placed at the initial distance of 2 Ȧ from the BNNT. The complex of BNNT and cRW3 was immersed in the simulation box consisting of TIP3P water molecules with the periodic boundary condition. Counter ions were then introduced into the simulation box to neutralize the simulated solution. Tersoff potential was applied to study the interaction between boron and nitrogen.59 All MD simulations were performed using the CHARMM27 force field.60 For the verification of the drug encapsulation process, first, the system was minimized in the NVT ensemble at 300 K while the BNNT was fixed. Second, the MD runs were performed in the NPT ensemble for 4 ns with a time step of 1 fs. For the vdW interaction, the inner and outer cut-off distances for the Lennard–Jones potential and Coulombic potential were 8 and 12 Ȧ, respectively. The Lorentz–Berthelot combination rule was applied to estimate the parameters of the Lennard–Jones potential for vdW interactions between non-bonded atoms.61 The vdW interaction between cRW3 and the BNNT can be obtained as:56

(1)

where is the vdW interaction between cRW3 and the BNNT, corresponds to the vdW interaction of cRW3 combined with the BNNT, and and refer to the vdW energies of cRW3 and the BNNT, respectively.

Regarding the stability of the drug encapsulated in the BNNT, an external force was applied to the encapsulated cRW3 along the z-axis of the nanotube to pull it out from the BNNT in the opposite direction to the penetrating process. The pulling velocity and spring constant k were 0.005 Ȧ ps−1 and 15 kcal mol−1 Ȧ−2, respectively.62 The pulling process was repeated ten times to obtain the potential of mean force (PMF) profile according to Jarzynski’s equality:60

(2)

where ΔG and W respectively represent the difference in free energy between two states and the work done on the system. β is equal to (T)−1 where refers to the Boltzmann constant.

Langevin dynamics was considered to ensure 300 K as simulation temperature. The Langevin piston Nose’-Hoover method was also used to fix the atmospheric pressure.

Results and Discussion

Localisation of cRW3 Within the Peptide-BNNT Complex

The encapsulation of cRW3 into the BNNT (12,12) was monitored through MD simulation, and snapshots taken by the VMD software at different times are shown in Figure 2. As can be seen, cRW3 was successfully inserted into the nanotube and remained stable up to 4 ns. Figure 3A shows the normalized center of mass (CoM) distance between the peptide and the BNNT, d/d0 where d0 equals 23.43 Å, as a function of the simulation time. The fluctuation and the decrement of d/d0 value at the beginning of the simulation confirmed that the peptide adjusted automatically during its entry into the BNNT. After the complete entry of the peptide into the nanotube cavity at 0.9 ns, the CoM distance between the peptide and the BNNT remained approximately stable until the end of the simulation at 4 ns.

Figure 2 Representative snapshots of the insertion of the cationic antimicrobial peptide cRW3 into an armchair (12,12) BNNT at different times. For the sake of clarity, the water molecules are not shown.

Figure 3 (A) d/d0 (normalized CoM distance where d0 is the initial CoM distance) between the cationic antimicrobial peptide cRW3 and the boron nitride nanotube as a function of simulation time; (B) vdW interaction between cRW3 and the BNNT (12,12) as a function of simulation time. The yellow regions illustrate the encapsulation period.

Due to the neutralized nature of the BNNT, the value of coulombic interactions (including hydrogen bonding, and dipole–dipole interactions) between the BNNT and the peptide was zero. Therefore, the vdW interaction energy (such as π-π interactions between the aromatic rings of the peptide and the BNNT) is supposed as an absorbance energy of the peptide into the cavity of the BNNT.

For determining the role of the vdW interaction energy between the peptide and BNNT during the encapsulation process, the variation of the cRW3-BNNT vdW interaction energy with the simulation time was estimated, and the result was plotted as a curve shown in Figure 3B. As expected, the vdW interaction energy of the cRW3-BNNT complex decreased with the decrement of d/d0 value during the encapsulation process and reached the value of −142.7 kcal·mol−1 after the complete insertion of the peptide into the nanotube cavity at the time of 4 ns. The same downward trend in the vdW energy of spontaneous insertion of DNA oligonucleotides and collagen-like peptides into CNTs has been reported by Huajian et al63 and Kang et al,64 respectively. In another research performed by Maleki et al,65 the vdW and electrostatic interactions between the Doxorubicin (DOX) and CNT were investigated. They demonstrated that due to the zero value of electro-static interactions, the absorbance of the DOX on the CNT was due to the vdW interactions with a favorable negative value.

The vdW interaction energy decreased rapidly until 0.34 ns when half of the peptide entered the BNNT. Then, for 0.45 ns, the peptide did not move in the nanotube and remained approximately static (with no decrease in CoM distance), and the peptide-BNNT vdW interaction energy did not change significantly. It can be explained that this phenomenon is related to the period when the peptide passed the maximum barrier energy at the entrance of the BNNT when half of the peptide was inserted inside the nanotube cavity.62 The yellow regions in Figure 3 illustrate this period of the encapsulation process. After crossing this energy barrier, the peptide was rapidly absorbed into the nanotube.

Free Energy Calculation from MD Simulation

After the complete insertion of cRW3 inside the BNNT at 4 ns, the PMF profile of the encapsulated peptide was obtained by pulling it out through the MD simulation at the speed of 0.005 Ȧ ps−1, which was chosen according to the speed of the encapsulation process. This simulation was repeated ten times to compute the average value of work (W) at each pulling distance, which is represented as a PMF profile in Figure 4. Moreover, the peptide positions along the z-axis corresponding to the BNNT are illustrated. It was observed that the free energy of this simulated system was increased during the pulling process and reached the value of 89.7 kcal·mol−1 at the pulling distance of 34 Å. This is in excellent agreement with the way the encapsulation process occurred spontaneously with the free energy of −89.7 kcal·mol−1. This observation is in good agreement with the results obtained in work done by Veclani et al66 so that the negative value of free energy (ΔG=−9.5 kcal·mol−1) for the adsorption process of ciprofloxacin on the surface of CNT.

Figure 4 Potential of mean force (PMF) computed from ten pullings by MD simulation. The images represent the positions of the cationic antimicrobial peptide cRW3 corresponding to the z-coordinate along the BNNT at some key position.

When half of the peptide entered the BNNT, the small barrier energy was detected in the PMF profile of the cRW3-BNNT system, which is an enthalpic phenomenon. A similar resistance corresponding to the potential energy barrier at the entrance of the carbon nanotube during the insertion of water molecules was reported.67 It was explained that the peptide was absorbed toward the BNNT cavity due to the vdW interaction, which overcame the hydrogen bonding between the water molecules. By decreasing the distance between the BNNT and cRW3, the higher accumulation of hydrogen bonding networks near and within the BNNT resulted in a 0.45 ns pause during the encapsulation process. However, the cRTW3–BNNT vdW interaction destroyed these hydrogen-bonding networks and overcame the energy barrier, which then allowed the favorable encapsulation process of the peptide inside the nanotube.62

Variations in the Conformation of the Peptide

Figure 5A depicts the changes in the peptide structure at 0 and 4 ns of MD simulation. The left image of Figure 5A is attributed to the peptide immersed in water molecules in its natural form at 0 ns. The image on the right represents the conformation of the peptide adjusted to the BNNT structure at 4 ns, demonstrating that the conformation of the peptide has adapted to the geometry of the BNNT after its complete insertion in the cavity of the nanotube. Similar changes in the configuration and arrangement of DOX encapsulated within the single-walled carbon nanotube in accordance with the diameter and chirality of the nanotube have been reported by Zhang et al.68

Figure 5 (A) Axial views of the cationic antimicrobial peptide cRW3 at 0 ns and 4 ns in the MD simulation. For clarity, water molecules were not shown. (B) Root mean square deviation (RMSD) of cRW3 as a function of simulation time. (C) Gyration radius of cRW3 as a function of simulation time. The yellow regions illustrate the encapsulation period.

Figure 5B shows the root mean square deviation (RMSD), which reveals the variations in the peptide conformation as a function of simulation time. As seen in this figure, the RMSD varied significantly by 0.34 ns, showing that changes in the peptide conformation are affected by the high cRW3-BNNT vdW interaction. The yellow region corresponds to the time during which half of the peptide was inserted into the BNNT, and the encapsulation process was interrupted for 0.45 ns. It was observed that, during this period, not only did the peptide not move toward the BNNT, but also that the changes in the configuration of the peptide were not significant, which is due to the energy barrier in the vicinity of the BNNT. However, after that, the RMSD fluctuated within the specified range, which shows the self-adjustment of the peptide to the inner geometry of the BNNT. Moreover, due to the small size and cyclic structure of the peptide, all hydrophobic and hydrophilic parts were equally influenced by the hydrophilic solvent and the hydrophobic nanotube, so that the distinct phase separation between hydrophobic and hydrophilic groups was not observed. Nevertheless, the different affinity of the hydrophobic and the hydrophilic groups for the solvent and the nanotube would be observed in the system containing larger biomolecules such as proteins.69

Considering the changes in the gyration radius of the peptide during the encapsulation process (Figure 5C), it was observed that the peptide was stretched by the cRTW3–BNNT vdW interaction until 0.34 ns of simulation time, which resulted in an increase in the gyration radius of the peptide. Then, for a period of 0.45 s (the yellow region in which half of the peptide was in the BNNT), the gyration radius reached its minimum value, showing the adjustment process during which the size of the peptide changed to match the movement towards the entrance hole of the BNNT. Subsequently, the configuration of the peptide changed to a more stable state with a higher gyration radius of about 6.1 Å. The variation in the distance between the central axis of the BNNT and the CoM of the peptide cRW3 during the simulation process is shown in Figure 6A. At 0 ns, the peptide was located at the specified location in the simulation box so that the CoM of the peptide was adjusted on the central axis of the BNNT. The peptide was then transferred to one side of the BNNT wall in relation to the initial reorientation of the peptide by the vdW interaction so that the cRW3-axis distance increased to 2.6 Å at 0.11 ns. However, this conformation of the peptide was also altered by adsorption to other sidewalls of the BNNT, which then probably caused the cRW3-axis distance to decrease. In other words, the hydrophobic groups in the structure of the peptide are strongly affected by the vdW interaction between the BNNT and the peptide, so that the CoM location of the peptide alternately changed towards the sidewall of the nanotube, appearing as the fluctuation of the cRW3-axis distance curve during the encapsulation procedure.

Figure 6 (A) Distance between the CoM of cRW3 and the central axis of the BNNT; and (B) potential energy of cRW3 as a function of simulation time, both as a function of simulation time. The yellow region illustrates the encapsulation period.

Figure 6A and B illustrates the potential energy changes of cRW3 during the simulation process. As can be seen, the potential energy of cRW3 was increased undesirably at the beginning of the encapsulation process, corresponding to a low-stability conformation. During the period of time when half of the peptide was placed in the BBNT cavity, and the pause in the encapsulation process occurred (the yellow region in Figure 6B), the potential energy of the peptide reached its minimum value, which is favorable for the continuation of the insertion process after this pause in the encapsulation process. The decrease in the potential energy of the peptide was due to the adjustment of the conformation of the peptide and was compensated by the energy of the system. After this time, the cRTW3–BNNT vdW interaction overcame the energy barrier, and the potential energy of the peptide increased again. The potential energy fluctuation of the peptide completely inserted into the BNNT was attributed to the continuous changes in conformation, as discussed above.

For a deeper understanding of the conformational changes (self-adjustment) of the peptide during the encapsulation process, especially during the time period in which the peptide was entering the cavity of the BNNT, the distance of each residue in the structure of the peptide cRTW3 from the central axis of the BNNT was calculated. As can be seen in Figure 7, at the beginning of the simulation, the variations in the distances of residues from the central axis of the BNNT were intensive, corresponding to the movement freedom of the peptide structure in its natural state. However, by approaching the peptide to the cavity of the BNNT, these changes became more smooth in a way that at the end of yellow region, where half of the peptide was inserted inside the BNNT, up to the end of the simulation all distances fluctuated in the narrow regions. These observations confirmed the stability of the encapsulated peptide under the effect of vdW interaction energy between the peptide residues and the interior wall of the BNNT.

Figure 7 The distance of residues in the structure of the drug cRW3 from the central axis of the BNNT (20, 20). The yellow regions illustrate the encapsulation period.

In other words, the conformational changes of the peptide residues within the yellow region made a great contribution to the encapsulation process so that the peptide could pass the energy barrier in the vicinity of the BNNT. During this period: 1) the peptide did not move in the direction toward the cavity of the BNNT, 2) the vdW energy between the BNNT and the peptide did not experience the reduction, 3) the potential energy of the peptide decreased in favour of the insertion process, 4) the gyration radius of the peptide reached the minimum, 5) the changes of the RMSD were not significant. At the end of this period, the peptide was appropriately adjusted to the geometry of the interior wall of the BNNT associated with the minimum value of the potential and vdW energies which confirmed the stability of the encapsulated peptide.

Conclusion

In the present work, the encapsulation process of the antimicrobial peptide cRW3 in a boron nitride nanotube (BNNT) in an aqueous medium was explored by MD simulation. It was observed that the peptide-BNNT vdW interaction energy and the normalized center of mass (CoM) distance between the peptide and the BNNT, d/d0, decreased during the encapsulation process and reached values of −142.7 kcal·mol−1 and 0, respectively. The calculation of the potential mean force, which was performed through a pulling process, revealed that the encapsulation process occurred spontaneously with the free energy of −89.7 kcal·mol−1. For a period of 0.45 ns, when half of the peptide was inserted into the BNNT cavity, the encapsulation process was interrupted due to the energy barrier caused by the hydrogen bonding networks accumulated in the vicinity of the nanotube. During this period, it was revealed that:

  1. d/d0 and the vdW interaction energy between the peptide and the BNNT did not change significantly.
  2. Based on the changes in root mean square deviation and gyration radius of the peptide, the latter did not undergo significant conformational changes and had the lowest gyration radius.
  3. The decrease in the potential energy of the peptide occurred due to the conformational adjustment of the peptide.

BNNT possesses promising features such as large internal volume, ability to penetration into tissues, biocompatibility, chemical inertness, non-toxicity, and acceptable water solubility, which makes it newly emerged nanocarriers in drug-based therapies. In addition, in accordance with obtained results, it was demonstrated that the cationic antimicrobial peptide cRW3 was successfully encapsulated spontaneously into BNNT through the desired vdW interactions between the peptide and the BNNT. Owing to the aforementioned factors, the BNNT-based drug delivery systems can be considered as an effective approach to delaying antimicrobial drug resistance. As a result, there is a need for further investigation on the performance of BNNT both theoretically and experimentally to achieve significant progress in the field of nanomedicine.

Data Sharing Statement

All data reported here can be made available on request by the corresponding authors.

Disclosure

The authors report no conflicts of interest in this work.

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