Al-shimaa S. M. Radya,
Peter A. Sidhom
b,
Lamiaa A. Mohamed
a,
Khalid Elfaki Ibrahim
c,
Shahzeb Khan
d and
Mahmoud A. A. Ibrahim
*aef
aComputational Chemistry Laboratory, Chemistry Department, Faculty of Science, Minia University, Minia 61519, Egypt. E-mail: m.ibrahim@compchem.net
bDepartment of Pharmaceutical Chemistry, Faculty of Pharmacy, Tanta University, Tanta 31527, Egypt
cDepartment of Zoology, College of Science, King Saud University, P.O. Box 2455, Riyadh 11451, Saudi Arabia
dCentre for Pharmaceutical Engineering Science, Faculty of Life Science, School of Pharmacy and Medical Sciences, University of Bradford, BD7 1DP, UK
eDepartment of Engineering, College of Engineering and Technology, University of Technology and Applied Sciences, Nizwa 611, Sultanate of Oman
fSchool of Health Sciences, University of KwaZulu-Natal, Westville Campus, Durban 4000, South Africa
First published on 10th September 2025
Cyclodextrins (CDs) have emerged as a promising strategy for the targeted drug delivery process. Herein, the potential of β-cyclodextrin (β-CD) as a drug delivery system for the Ampyra (AMP) drug was extensively investigated. By means of the molecular dynamics (MD) simulation technique, the inclusion process of AMP with β-CD was first examined and consequently subjected to clustering analysis. Upon the obtained five configurations (A↔E) of AMP⋯β-CD complex, extensive density functional theory (DFT) calculations were executed. The favorability of the quested encapsulation process was affirmed by negative adsorption and interaction energies of the selected configurations A↔E affirmed the occurrence of the quested encapsulation process. In particular, configuration A is more energetically preferred compared to other analogs. The insights from SAPT analysis verified the dominant role of electrostatic and dispersion forces in the interactions within the studied configurations A↔E. From QTAIM and NCI analyses, the occurrence and nature of intermolecular interactions within the studied configurations A↔E were illustrated. As per the electronic analysis, the effect of the AMP encapsulation process on the electronic features of β-CD was emphasized. The enhancing impact of the aqueous medium on the studied configurations A↔E was verified by negative adsorption and solvation energies. Moreover, the calculated recovery time values pinpointed the separation potential of AMP from β-CD at the target cell. Overall, the obtained outcomes provided insights into the potential application of β-CD as a drug delivery system, particularly for AMP drug.
In the extending field of drug delivery systems, self-assembled nanoparticles of amphiphilic molecules have been utilized in different drug delivery processes.10–12 Among amphiphilic molecules, cyclodextrins (CDs) have been extensively applied owing to their exceptional features.13 CDs are natural cyclic oligosaccharides that are made of several glucose units.14 The advent of CDs has sparked a lot of attention due to their paramount importance in medicinal chemistry, biology, and pharmaceuticals.15,16
Further, the engagement of CDs in the drug delivery process has obviously enhanced the subsequent physicochemical properties of drugs.17,18 Compared to the other drug delivery systems, CDs with a unique toroidal structure are able to encapsulate drug molecules, which in turn enhance the bioavailability, water solubility, and therapeutic potential of drugs.19
In the scope of CDs, three main structures, namely, α-cyclodextrin (α-CD), β-cyclodextrin (β-CD), and γ-cyclodextrin (γ-CD), were identified, containing six, seven, and eight molecules of glucopyranose, respectively. Of all applied CDs, the β-CD has been particularly adopted as a favorable drug delivery system due to its low toxicity.20 Several strategies were employed to enhance the performance of β-CD as a drug delivery system.21,22 Indeed, the hydrophobic cavity of β-CD allows the encapsulation of diverse bioactive molecules.23,24 Such an encapsulation process enhances the physical, chemical, and biological characteristics of the drugs.25 By means of molecular dynamics (MD) simulation and density functional theory (DFT) calculations, the potential of β-CD to encapsulate various drugs was previously investigated.26,27 Further, the preparation of drug-β-CD complexes was experimentally conducted.28,29
Ampyra (AMP), known as dalfampridine or 4-aminopyridine, is the first FDA-approved drug for the treatment of multiple sclerosis (MS) disease.30,31 AMP, with the chemical formula of C5H6N2, is also used as an anticancer drug to remedy lung, leukemia, skin, and bladder cancers.32 Nevertheless, the ineffective AMP delivery strategies cause side effects that increase with high doses.33,34 In the quest to overcome the side effects of the AMP delivery process, silica surfaces and graphene nanosheets were proposed as delivery systems.35,36 Indeed, many strategies in the drug delivery process are available; however, a more preferable option is the utilization of natural nanocarriers. To the best of our knowledge, no comprehensive study has been performed to investigate the inclusion process of AMP with β-CD. Therefore, the current investigation aimed to evaluate the potential of β-CD as a natural drug delivery system for AMP. Toward the inclusion process of AMP with β-CD, MD simulation was performed over 10 ns. Consequently, the clustering analysis of the MD course was executed, followed by performing DFT calculations for the selected configurations A↔E of AMP⋯β-CD complex. Based on the selected configurations, the electrostatic potential (ESP), frontier molecular orbitals (FMOs), and total density of states (TDOS) analyses were also executed. For further investigation, quantum theory of atoms in molecules (QTAIM) and symmetry-adapted perturbation theory (SAPT) analyses were performed. The impact of the aqueous medium on the studied configurations A↔E was further examined. The current study would aid in the prospective application of β-CD as a promising drug delivery system, especially for AMP drug.
Toward complex formation, MD simulation was performed over 10 ns to investigate the structure and dynamics of the 1:
1 inclusion AMP⋯β-CD complex. MD was performed for the optimized AMP complexed with β-CD using AMBER 20 software.43 In this regard, the general AMBER force field (GAFF2) was utilized to parameterize the β-CD and AMP, as previously recommended.44,45 For atomic charge calculations, the restraint electrostatic potential (RESP) approach was applied to the optimized structures of AMP and β-CD molecules at HF/6-31G* level of theory.46 The AMP⋯β-CD complex was immersed in an octahedron box with TIP3P water molecules at 1.2 nm marginal radiuses. To eliminate the unsuitable geometries or steric clashes, the minimization step was carried out for 5000 cycles utilizing combined steepest descent and conjugate gradient algorithms. Following, the obtained systems were gradually heated to 310 K. Afterward, the investigated systems were equilibrated for 1 ns. The equilibrated complex was finally subjected to production phases for 10 ns. Snapshots were collected every 10 ps, giving 1000 snapshots over the 10 ns MD simulation. Based on the collected snapshots, water molecules were removed, and clustering analysis was performed with an RMSD value of 2.0 Å. With the help of CPPtraj,43 clustering analysis was performed, where five clusters were obtained. Subsequently, the average structure from each cluster was obtained, giving five configurations (A↔E).
For the selected configurations A↔E, geometrical optimization was performed at the M06-2X/6-311+G** level of theory (Fig. 1). As such, the favorability of the optimized configurations was evaluated by calculating the adsorption (Eads) and interaction (Eint) energies using eqn (1) and (2), respectively.
Eads = EAMP⋯β-CD − (EAMP + Eβ-CD) + EBSSE | (1) |
Eint = EAMP⋯β-CD − (EAMP in complex + Eβ-CD in complex) + EBSSE | (2) |
![]() | ||
Fig. 1 Optimized AMP and β-CD structures with their related MEP maps. The color of MEP maps ranged from +0.01 au (blue) to −0.01 au (red). |
By incorporating SAPT analysis, energy decomposing was performed with the help of the PSI4 package.50 For the complex under investigation, SAPT0 level51 was applied to obtain total energy along with its four components as follows:
ESAPT0 = Eelst + Eexch + Eind + Edisp | (3) |
Eelst = Eelst(10) | (4) |
Eexch = Eexch(10) | (5) |
Eind = Eind, resp(20) + Eexch-ind,resp(20) + δEHF,resp(2) | (6) |
Edisp = Edisp(20) + Eexch-disp(20) | (7) |
From the above-mentioned equations, the ESAPT0 introduces the total energy and Eelst illustrates the electrostatic force. In addition, Eexch, Eind, and Edisp refer to exchange, induction, and dispersion forces, respectively. To illustrate the intermolecular interactions within the studied configurations, the quantum theory of atoms in molecules (QTAIM) analysis was applied. Inspired by QTAIM, the generation of bond paths and bond critical points (BPs and BCPs, respectively) within the interacted species was performed. Afterward, the noncovalent interaction (NCI) index analysis was carried out, and the 3D NCI plots were generated with a color range according to (λ2)ρ values from blue (−0.035 au) to red (0.020 au). Overall, the Multiwfn 3.7 software42 and the Visual Molecular Dynamics (VMD) program52 were applied for performing and visualizing the QTAIM/NCI analyses, respectively.
Turning to the electronic features, the frontier molecular orbitals (FMOs) theory was carried out on the studied systems. Within FMOs analysis, maps of HOMO and LUMO, along with their energies (EHOMO and ELUMO, respectively), were obtained. In accordance, the values of energy gap (Egap) and Fermi level (EFL) were evaluated by considering the EHOMO and ELUMO values, as described below:
Egap = ELUMO − EHOMO | (8) |
![]() | (9) |
Inspired by EHOMO, the ionization potential (IP) was calculated, while from ELUMO, the electron affinity (EA) was evaluated as follows:
IP ≈ −EHOMO | (10) |
EA ≈ −ELUMO | (11) |
![]() | (12) |
![]() | (13) |
![]() | (14) |
![]() | (15) |
Φ = VeL(+∞) − EFL | (16) |
On the basis of the Egap values, the electrical conductivity (σ) could be determined using the following formula:
σ ∝ exp(−Egap/kT) | (17) |
According to the above equation, k introduces Boltzmann's constant while T is the adopted temperature. For further electronic investigation, TDOS analysis was executed for the optimized β-CD molecule and its combined complex with the AMP drug by applying the GaussSum software.53 To conceive the water impact on the considered encapsulation process, the integral equation formalism-polarizable continuum model (IEF-PCM) solvation model within the Gaussian 09 software was applied, as previously recommended.54–57 Regarding the IEF-PCM, geometrical optimization followed by energy calculations (Eadssolvent) was performed using the M06-2X/6-311+G** level of theory. Further, solvation (ΔEsolv) energies of all studied configurations were calculated as follows:
ΔEsolv = Esolvent − Egas | (18) |
τ = v−1exp(−ΔEads/kT) | (19) |
The optimized structure of β-CD, as shown in Fig. 1, is a polysaccharide that contains hydrogen, carbon, and oxygen atoms throughout its triple-helix conformation. According to the MEP map of β-CD, red-colored regions (i.e., negative ESP) were concentrated around O atoms, while the blue-colored regions (i.e., positive ESP) were shown above H/C atoms. Illustratively, the Vs,min and Vs,max values were found with values up to −55.1 and 84.9 kcal mol−1, respectively.
In the case of the AMP, the N atoms were surrounded by a red-colored region, while H atoms were encircled by a blue one. From a quantitative point of view, the Vs,min and Vs,max were found with values up to −50.4 and 57.6 kcal mol−1, respectively. Subsequently, the positive/negative regions around H/N atoms of AMP and H/O atoms of β-CD proposed the preferable formation of hydrogen bonding interactions within the proposed AMP⋯β-CD complex, respectively. In summary, ESP analysis offered explicit detail about active sites over β-CD and AMP molecules, which offered insight into the proposed inclusion process through various configurations.
![]() | ||
Fig. 2 Representation of inclusion process of AMP with β-CD: (i) encapsulation and (ii) adsorption models. |
Complex | Configuration | Bond parameters | Eint | Eads | |
---|---|---|---|---|---|
Distance (r, Å) | Angles (θ, °) | ||||
AMP⋯β-CD | A | N⋯H (2.02) | N⋯H–O (151.91) | −26.21 | −20.10 |
H⋯O (2.19) | N–H⋯O (157.29) | ||||
H⋯O (2.26) | N–H⋯O (154.41) | ||||
B | H⋯O (2.05) | N–H⋯O (158.35) | −24.21 | −18.95 | |
H⋯O (2.23) | N–H⋯O (127.11) | ||||
C | H⋯O (2.03) | N–H⋯O (149.55) | −22.69 | −13.21 | |
H⋯O (2.06) | N–H⋯O (156.14) | ||||
D | H⋯O (2.16) | N–H⋯O (148.20) | −20.25 | −9.56 | |
H⋯O (2.34) | N–H⋯O (154.39) | ||||
E | H⋯O (2.00) | N–H⋯O (165.13) | −19.24 | −11.63 |
According to Fig. 3, the favorable encapsulation of AMP into β-CD through different configurations was illustrated by relative small r values ranging from 2.00 to 2.34 Å. Substantial negative Eint and Eads values were found for the optimized configurations A↔E, verifying that the studied encapsulation process was energetically preferred (Table 1). Of all studied configurations, the most negative Eint and Eads values (i.e., −26.21 and −20.10 kcal mol−1, respectively) were noticed for configuration A. Notably, the Eint was observed to follow a decreasing order of A > B > C > D > E. Illustratively, configurations A, B, C, D, and E exhibited Eint with values of −26.21, −24.21, −22.69, −20.25, and −19.24 kcal mol−1, respectively. In general, the Eads values were found to follow the same order as Eint. In the core of the energy affirmations, the obtained Eint and Eads values highlighted the potential of β-CD as a potent drug delivery system for the AMP drug.
Complex | Configuration | ESAPT0 | Eelst | Eind | Edisp | Eexch |
---|---|---|---|---|---|---|
AMP⋯β-CD | A | −30.13 | −28.62 | −9.22 | −26.00 | 33.70 |
B | −26.91 | −23.60 | −6.37 | −29.17 | 32.23 | |
C | −24.84 | −26.17 | −6.98 | −31.01 | 39.32 | |
D | −23.27 | −19.87 | −5.41 | −25.80 | 27.81 | |
E | −21.55 | −19.69 | −5.96 | −22.63 | 26.73 |
Considering the data in Table 2, negative ESAPT0 values were obtained for all studied configurations A↔E, which in turn affirmed the ability of β-CD to encapsulate AMP drug. Notably, the ESAPT0 values were observed to follow the same order as Eint (Table 1). Numerically, Eint/ESAPT0 was −26.21/−30.13, −24.21/−26.91, −22.69/−24.84, −20.25/−23.27, and −19.24/−21.55 kcal mol−1 of configurations A, B, C, D, and E, respectively. In the scope of force contribution, Edisp force was observed with higher negative values compared to other forces, affirming its dominant role in total interactions within the studied configurations B↔E. Besides, the Eelst and Eind forces were also noticed with negative values, ensuring their significant contribution to the total energy (ESAPT0). Meanwhile, the Eexch force exhibited positive values, indicating its unfavorable impact on the studied encapsulation process. For instance, Eelst, Edisp, Eind, and Eexch were −23.60, −29.17, −6.37, and 32.23 kcal mol−1, respectively, of configuration B. Meanwhile, Eelst had the most dominant role in the case of configuration A, where Eelst, Edisp, Eind, and Eexch were −28.62, −26.00, −9.22, and 33.70 kcal mol−1, respectively. In summary, SAPT findings revealed the potential application of β-CD as a drug delivery system for AMP.
As shown in Fig. 4 and S1, it was clear from QTAIM plots that the β-CD linked to AMP through various BPs and BCPs, illustrating the occurrence of interactions within the studied configurations A↔E. Particularly, additional BPs and BCPs linked the H/N atoms of AMP with the O/H atoms of β-CD, verifying the promising role of hydrogen bonding interactions in the investigated encapsulation process.
Regarding NCI plots, colored isosurfaces were observed between the AMP and β-CD, elucidating the occurrence of the considered encapsulation process within the studied configurations. In studying NCI plots, the blue- and green-colored isosurfaces indicated more and less attractive interactions, respectively. Notably, the green-colored isosurfaces were found between AMP and β-CD, affirming the attractive nature of interactions within the studied configurations A↔E.
As illustrated in 2D NCI plots in Fig. S2, the studied configurations A↔E had values less than 0.01 au of the sign (λ2)ρ, affirming the attractive nature of interactions within the studied configurations. To sum up, QTAIM and NCI affirmations highlighted the favorability of the AMP encapsulation process into β-CD that was supported by hydrogen bonding interactions.
System | Configuration | EHOMO | ELUMO | Egap | EFL |
---|---|---|---|---|---|
β-CD | −8.85 | −0.74 | 8.11 | −4.80 | |
AMP | −7.68 | 0.11 | 7.79 | −3.79 | |
AMP⋯β-CD | A | −7.93 | −0.47 | 7.46 | −4.20 |
B | −7.59 | −0.35 | 7.24 | −3.97 | |
C | −7.66 | −0.56 | 7.10 | −4.11 | |
D | −7.57 | −0.83 | 6.73 | −4.20 | |
E | −7.75 | −0.48 | 7.28 | −4.12 |
As displayed in Fig. 5, notable changes in the distribution of HOMO/LUMO levels were observed as a consequence of the encapsulation process within the studied configurations A↔E. Further, the different arrangements of HOMO and LUMO levels within the studied configurations highlighted the occurrence of charge transfer between AMP and β-CD.67 Upon FMOs analysis, the encapsulation process of AMP into β-CD within the studied configurations A↔E was affirmed.
Upon data gathered in Table 3, the values of EHOMO and ELUMO of isolated AMP and β-CD were significantly varied after the encapsulation process within the studied configurations A↔E. From these alterations, the impact of the AMP on the electronic nature of β-CD was highlighted. Illustratively, the EHOMO/ELUMO of β-CD was −8.85/−0.74 eV and altered to −7.93/−0.47 eV of configuration A. In accordance with changes in EHOMO/ELUMO, the Egap of β-CD was further altered after the AMP encapsulation process. Numerically, the Egap of β-CD was 8.11 eV and changed to 7.46 eV in configuration A. Besides, Egap has a significantly role in determining the chemical reactivity and electronic charge transfer features.68 Notably, relative small Egap for the studied configurations affirmed their chemical reactivity. The decrement in the Egap value of β-CD after the encapsulation of AMP was correlated with an enhancement in the charge transfer process, chemical reactivity, and electrical conductivity of β-CD. In summary, changes in the calculated electronic descriptors verified the promising application of β-CD as a drug delivery system for AMP.
System | Configuration | IP (eV) | EA (eV) | μ (eV) | η (eV) | S (eV−1) | ω (eV) | Φ (eV) |
---|---|---|---|---|---|---|---|---|
β-CD | 8.85 | 0.74 | −4.80 | 4.06 | 0.25 | 2.84 | 4.80 | |
AMP | 7.68 | −0.11 | −3.79 | 3.90 | 0.26 | 1.84 | 3.79 | |
AMP⋯β-CD | A | 7.93 | 0.47 | −4.20 | 3.73 | 0.27 | 2.36 | 4.20 |
B | 7.59 | 0.35 | −3.97 | 3.62 | 0.28 | 2.18 | 3.97 | |
C | 7.66 | 0.56 | −4.11 | 3.55 | 0.28 | 2.38 | 4.11 | |
D | 7.57 | 0.83 | −4.20 | 3.37 | 0.30 | 2.62 | 4.20 | |
E | 7.75 | 0.48 | −4.12 | 3.64 | 0.27 | 2.33 | 4.12 |
From the data summarized in Table 4, the calculated descriptors of β-CD were obviously changed after the encapsulation of AMP, pointing to the impact of AMP on the electronic nature of β-CD. For example, the IP/EA of β-CD was 8.85/0.74 eV and changed to 7.93/0.47 eV in configuration A. As previously documented, the obtained IP and EA were correlated with EHOMO and ELUMO.69 Notably, the η and S values of β-CD were decreased and enhanced, respectively, as the encapsulation process occurred through the optimized configurations A↔E. For numerical evidence, the η/S values of β-CD were 4.06 eV/0.25 eV−1 and varied to 3.73 eV/0.27 eV−1 of configuration A. Further, the AMP encapsulation process led to a noticeable decrease in Φ values. For instance, the Φ value of β-CD was 4.80 eV and decreased to 4.20 eV in configuration A. To sum up, the calculated electronic features before and after the AMP encapsulation process into β-CD highlighted the AMP influence on the β-CD electronic nature.
From the plots in Fig. 6, changes in extracted plots of β-CD were observed after the encapsulation process, ensuring the favorability of β-CD to encapsulate the AMP. In this regard, new peaks emerged near −8 eV for all configurations A↔E, illustrating the impact of AMP on the electronic nature of the β-CD. Further, the AMP encapsulation process into β-CD resulted in notable variations of the Egap of β-CD, which was in the same line with the electronic parameters in Table 3. Upon the TDOS plots, the encapsulation process within the studied configurations A↔E was elucidated from an electronic point of view.
Complex | Configuration | Eadssolvent (kcal mol−1) | ΔEsolv (kcal mol−1) |
---|---|---|---|
AMP⋯β-CD | A | −5.38 | −40.77 |
B | −6.17 | −42.71 | |
C | −6.94 | −49.22 | |
D | −6.97 | −52.90 | |
E | −7.14 | −51.00 |
As tabulated in Table 5, the studied configurations A↔E exhibited negative Eadssolvent values, affirming the superiority of the studied encapsulation process in water. From the obtained data, the Eadssolvent values ranged from −5.38 to −7.14 kcal mol−1. Obviously, negative ΔEsolv values were noticed for the optimized configurations with values of up to −51.00 kcal mol−1. Overall, the aqueous medium notably impacted the structures of the studied configurations, leading to changes in the adsorption energies. In conclusion, the obtained negative energy values affirmed the favorability of β-CD to encapsulate the AMP in an aqueous medium.
Complex | Configuration | T1 | T2 | T3 |
---|---|---|---|---|
AMP⋯β-CD | A | 5.16 × 102 | 1.39 × 102 | 8.30 × 101 |
B | 7.43 × 101 | 2.16 × 101 | 1.33 × 101 | |
C | 4.67 × 10−3 | 1.97 × 10−3 | 1.41 × 10−3 | |
D | 9.95 × 10−6 | 5.33 × 10−6 | 4.17 × 10−6 | |
E | 3.26 × 10−4 | 1.53 × 10−4 | 1.13 × 10−4 |
From the reported data in Table 6, the separation of AMP from β-CD at the target site was affirmed through significant τ values of the studied configurations A↔E. Illustratively, an association was observed between the τ and Eads values, where the higher negative Eads require longer τ values to release from the β-CD at the target site. Evidently, configuration A had the highest negative Eads value of −20.10 kcal mol−1 and the longest τ value of 5.16 × 102 μs at room temperature. Further, the τ values were correlated with temperature; an increase in temperature was accompanied by a decrease in τ values. For configuration A, τ values were 5.16 × 102, 1.39 × 102, and 8.30 × 101 μs at 298.15, 310.15, and 315.15 K, respectively. Overall, suitable τ values affirmed the potential of β-CD as a promising drug delivery system for AMP.
This journal is © The Royal Society of Chemistry 2025 |