Leila Tayebi,
Rahmatollah Rahimi,
Ali Reza Akbarzadeh* and
Ali Maleki
Department of Chemistry, Iran University of Science and Technology, P. O. Box: 16846-13114, Tehran, Islamic Republic of Iran. E-mail: a_akbarzadeh@iust.ac.ir
First published on 17th August 2023
During the drug release process, the drug is transferred from the starting point in the drug delivery system to the surface, and then to the release medium. Metal–organic frameworks (MOFs) potentially have unique features to be utilized as promising carriers for drug delivery, due to their suitable pore size, high surface area, and structural flexibility. The loading and release of various therapeutic drugs through the MOFs are effectively accomplished due to their tunable inorganic clusters and organic ligands. Since the drug release rate percentage (RES%) is a significant concern, a quantitative structure–property relationship (QSPR) method was applied to achieve an accurate model predicting the drug release rate from MOFs. Structure-based descriptors, including the number of nitrogen and oxygen atoms, along with two other adjusted descriptors, were applied for obtaining the best multilinear regression (BMLR) model. Drug release rates from 67 MOFs were applied to provide a precise model. The coefficients of determination (R2) for the training and test sets obtained were both 0.9999. The root mean square error for prediction (RMSEP) of the RES% values for the training and test sets were 0.006 and 0.005, respectively. To examine the precision of the model, external validation was performed through a set of new observations, which demonstrated that the model works to a satisfactory degree.
Ways to treat cancer include surgery, chemotherapy, radiation therapy, targeted therapy, immunotherapy, stem cell or bone marrow transplant, and hormone therapy.11 Generally, cancer drugs destroy the RNA or DNA responsible for replication in cell division; therefore, the cancer cells are unable to divide and die.12 Chemotherapy drugs kill cancer cells by stopping them from growing and multiplying.13 If the cells can't grow and multiply, they usually die. Some chemotherapy drugs target a specific stage of the cell cycle.14 The fluoropyrimidine 5-fluorouracil (5-FU) is an effective antimetabolite drug that is widely used for the treatment of cancer, especially colorectal cancer. The action of 5-FU is through the inhibition of thymidylate synthase (TS) and incorporation of its metabolites into RNA and DNA.15
Unfortunately, chemotherapeutic drugs in free formation always lead to adverse effects on healthy tissues and even the immune system. Nanocarriers have been intensively engineered as stimuli-responsive drug delivery systems to load and intelligently release various drug molecules. To achieve superior efficacy, the drugs need to be loaded into nanocarriers with high loading content and released at the target site in a controllable and specific-responsive manner.16 Further, various nanoparticle-based systems have been studied for drug delivery, such as liposomes, micelles, dendrimers, microbubbles, and solid particles.17 Due to their suitable pore size and diverse functional groups, as well as great loading of drugs, metal–organic frameworks (MOFs) are potentially beneficial to encapsulate drug products.18 Furthermore, MOFs show several outstanding advantages, such as facile modification of physical and chemical properties through inorganic clusters and/or organic ligands.19
The quantitative structure–activity relationship (QSAR) model is a regression model in which the relationship between chemical structure and biological action is quantitatively investigated.20 The basis of QSAR methods is the dependence on action and structure.21 Quantitative dependence on action and structure is one of the most fundamental methods of intra-computer study for biological and chemical modeling, especially in drug design, drug targeting, and drug discovery.22 The quantitative structure–property relationship (QSPR) method applies structural features of molecules to create an accurate and fast model that correlates structure-based properties of materials to their quantitative functions. Generally, there are two common categories for QSPR models, based on the type of descriptors used in modeling: theory- and experiment-based modeling. To build a theory-based QSPR model, various molecular descriptors, such as geometric, quantum mechanical, and thermodynamic quantities are used, and experiment-based QSPR models are mainly presented using experimental descriptors that express the physicochemical properties related to the structure of molecules.23 QSPR investigations on drug release from hydroxypropyl methylcellulose compounds have been conducted using structural descriptors; these have confirmed that the aqueous solubility of drugs and the size of the drug molecules are appropriate descriptors that can influence drug release from these polymers.24 Also, penetration enhancement activities of some compounds towards different drugs have been investigated, employing a QSPR study.25 This QSPR technique was developed using the molecular descriptors created by the COSMIC force field and the molecular mechanical descriptors by the NEMESIS software; which helps to better understand the mechanisms of penetration enhancement.25 A prediction of the volume of distribution has been created by Ghafourian et al. using some structural descriptors, including partitioning, quantum mechanical, molecular mechanical, and connectivity parameters.26 Selection of the proper variable was made using a genetic algorithm, and stepwise regression analyses and many models were created for acidic and basic drugs. Furthermore, QSPR analysis of many MOFs has been developed by researchers to correlate their structural features and their physical, chemical, and biological properties.27–29 To develop a QSPR/QSAR model, several mathematical methods have been applied. Multiple linear regression (MLR), partial least squares (PLS), principal component analysis (PCA), and artificial neural network (ANN) are four commonly used methods.23
In this research, based on structural variables—such as ligand fragments and metal secondary building units (SBUs)—as the adjusted parameters, we obtained the most appropriate drug release model from MOFs through the QSPR method, which was performed using 5-FU drug release. The presented procedure here investigated the relationships between the release of drugs from a large class of MOFs and their structures. This work indicates a simple computational method for the rapid calculation of drug release from MOF drug delivery systems with suitable results. Considering that 5-FU is widely used for cancer treatment, the model was specifically created for this drug. One of the challenges we face in modeling drug release from drug delivery systems is that the desired software is not available to everyone. In addition, the determination of quantum descriptors is a complex process. The advantage of the presented work is that (a) the model is performed without special software, and (b) modeling is carried out using simple and knowledge-based descriptors.
No. | MOF | nN | nO | RES+ | RES− | Exp. RES%a | IM–L | Ref. | Pred. RES%b | Dev.c | Std. dev.d | L.B. 95%e | U.B. 95%f |
---|---|---|---|---|---|---|---|---|---|---|---|---|---|
a Exp. RES%: experimental value of RES%.b Pred. RES%: predicted value of RES%.c Dev.: deviation.d Std. dev.: standard deviation.e L.B.: lower bound.f U.B.: upper bound. | |||||||||||||
Training set (54 entries) | |||||||||||||
1 | NTU-Z11 | 0.00 | 16.00 | 1.377 | 2.550 | 64.00 | −5.91 | 32 | 28.991 | 0.009 | −0.026 | 63.991 | 64.009 |
2 | CPON-1 | 1.00 | 5.00 | −0.220 | 2.811 | 25.00 | −3.27 | 33 | 23.994 | 0.006 | 0.556 | 24.989 | 25.006 |
3 | [(CH3)2NH2]2[Zn(TATAT)2/3]·3DMF | 9.00 | 12.00 | −7.698 | 4.739 | 44.00 | −9.95 | 34 | 51.994 | 0.006 | 1.055 | 43.987 | 44.004 |
4 | fa-IRMOF3 | 3.00 | 13.00 | −2.189 | 3.300 | 45.00 | −5.09 | 35 | 14.999 | 0.001 | 2.116 | 44.983 | 45.000 |
5 | [(Me2NH2)4Zn2(FDC)4]n | 4.00 | 20.00 | −5.491 | 3.664 | 29.00 | −7.70 | 36 | 25.993 | 0.007 | −1.934 | 29.000 | 29.017 |
6 | [Zn3(BTC)2(Me)(H2O)2](MeOH)13 | 0.00 | 33.00 | −4.982 | 2.627 | 18.00 | −9.95 | 37 | 31.003 | −0.003 | 0.149 | 17.991 | 18.008 |
7 | [Zn3(bdcNH2)2(dfp)2]·DMF | 4.00 | 12.00 | 0.227 | 3.712 | 89.00 | −13.05 | 38 | 51.999 | 0.001 | −1.332 | 88.997 | 89.015 |
8 | NH2(CH3)2[Zn3(L)2·3.5DMF] | 0.00 | 16.00 | −0.596 | 4.440 | 22.00 | −9.60 | 39 | 42.999 | 0.001 | 1.293 | 21.986 | 22.003 |
9 | IRMC-1 | 12.00 | 1.00 | −5.553 | 5.521 | 85.00 | −7.27 | 40 | 11.993 | 0.007 | −0.200 | 84.991 | 85.010 |
10 | [Zn2(ad)2(hmdb)(H2O)](DMF)2 | 15.00 | 12.00 | −17.118 | 2.995 | 13.00 | −19.86 | 41 | 19.992 | 0.008 | −0.216 | 12.992 | 13.010 |
11 | [Zn(FDC)]·H2O | 0.00 | 5.00 | 1.375 | 2.624 | 34.00 | −1.09 | 42 | 51.999 | 0.001 | −1.981 | 34.000 | 34.017 |
12 | [Zn(BTC)(HME)]·(DMAc)(H2O) | 7.00 | 8.00 | −6.494 | 3.260 | 31.00 | −8.48 | 43 | 22.996 | 0.004 | 1.757 | 30.984 | 31.001 |
13 | [Zn2(ad)2(fmdb)(H2O)](DMF)3 | 10.00 | 15.00 | −11.880 | 4.244 | 11.00 | −14.79 | 44 | 23.991 | 0.009 | −0.969 | 10.995 | 11.013 |
14 | [Zn3(OH)2(H2tccp)2(bpy)2](H2O)3(DMF)3 | 6.00 | 18.00 | −6.142 | 5.810 | 29.00 | −14.22 | 45 | 63.998 | 0.002 | 0.412 | 28.989 | 29.007 |
15 | [Zn8(O)2(CDDB)6(DMF)4(H2O)] | 10.00 | 31.00 | −13.260 | 3.020 | 43.00 | −17.87 | 46 | 45.991 | 0.009 | −2.038 | 43.000 | 43.017 |
16 | [Zn2(ad)2(AMDB)(H2O)](DMF)3 | 17.00 | 10.00 | −18.100 | 3.533 | 20.00 | −20.87 | 47 | 47.995 | 0.005 | 0.245 | 19.990 | 20.008 |
17 | [Zn2(bptc)(H2O)]·(DMAc)3(H2O)4 | 3.00 | 16.00 | −4.027 | 3.400 | 26.00 | −7.02 | 48 | 9.998 | 0.002 | −0.741 | 25.995 | 26.012 |
18 | [Zn(4,4-bipy)(formic acid)2(NO3)2] | 1.00 | 4.00 | −0.836 | 2.334 | 17.00 | −8.83 | 49 | 56.199 | 0.001 | 0.266 | 16.990 | 17.008 |
19 | ([Zn4O(dmcapz)3] | 6.00 | 7.00 | −2.396 | 5.965 | 52.00 | −5.40 | 50 | 39.991 | 0.009 | 0.540 | 51.989 | 52.007 |
20 | [Zn7L2(HL)2(OH–)4(H2O)2]·2H2O | 4.00 | 40.00 | −10.174 | 3.465 | 17.00 | −12.62 | 51 | 83.997 | 0.003 | −0.433 | 16.993 | 17.011 |
21 | [Zn2(fer)2] | 0.00 | 8.00 | 0.449 | 1.088 | 40.00 | −8.23 | 52 | 95.001 | −0.001 | −0.697 | 39.994 | 40.012 |
22 | [Zn2(abtc)(DMA)(H2O)2]·(DMA)4 | 3.00 | 11.00 | −1.637 | 4.194 | 41.00 | −9.12 | 53 | 78.991 | 0.009 | −0.070 | 40.992 | 41.009 |
23 | [(Me2NH2)2Zn3(fdc)4]n·DMA | 2.00 | 20.00 | −0.153 | 3.664 | 75.00 | −5.35 | 54 | 28.991 | 0.009 | −0.378 | 74.993 | 75.010 |
24 | ZIF-NP | 5.00 | 4.00 | −2.293 | 1.896 | 60.00 | −4.65 | 55 | 23.994 | 0.006 | 0.907 | 59.987 | 60.005 |
25 | ZIF-90 | 2.00 | 0.00 | 0.552 | 2.375 | 41.00 | −7.57 | 56 | 51.994 | 0.006 | −0.218 | 40.992 | 41.010 |
26 | Cu-BTC | 0.00 | 12.00 | 1.356 | 2.550 | 53.00 | −13.30 | 57 | 14.999 | 0.001 | −0.151 | 52.992 | 53.009 |
27 | [Cu(L)(4,4′-bipy)(H2O)]n·1.5nCH3CN | 3.50 | 5.00 | −3.353 | 3.235 | 15.00 | −26.65 | 58 | 25.993 | 0.007 | −1.176 | 14.996 | 15.014 |
28 | [(Cu2(L2)(H2O)2]·2.22DMA | 3.22 | 12.20 | −3.335 | 4.095 | 24.00 | −19.77 | 59 | 31.003 | −0.003 | 0.473 | 23.989 | 24.007 |
29 | GDMU-2 | 0.00 | 14.00 | −0.794 | 5.100 | 9.00 | −20.12 | 60 | 51.999 | 0.001 | 1.042 | 8.987 | 9.004 |
30 | [Cu(BTTA)]n | 6.00 | 4.00 | −4.745 | 5.334 | 15.00 | −6.93 | 61 | 42.999 | 0.001 | 0.446 | 14.989 | 15.007 |
31 | [NH2(CH3)][Cu6(L)3(OAc)(H2O)4]·xsolvent | 10.00 | 30.00 | −13.703 | 5.211 | 18.00 | −28.52 | 62 | 11.993 | 0.007 | −0.953 | 17.995 | 18.013 |
32 | [H3O][Cu6(tpta)3(DMA)4(COO)]·12H2O·7DMA | 4.00 | 30.00 | −7.078 | 3.400 | 35.00 | −26.73 | 63 | 19.992 | 0.008 | 1.097 | 34.987 | 35.004 |
33 | [Cu2(OH)bcb](DMF)2(H2O)3 | 0.00 | 9.00 | 0.993 | 4.028 | 29.00 | −20.22 | 64 | 51.999 | 0.001 | 1.010 | 28.987 | 29.004 |
34 | [Dy(BTC)(H2O)]·(H2O)(DMF) | 0.00 | 6.00 | 0.450 | 2.550 | 24.00 | −9.85 | 65 | 22.996 | 0.004 | 0.174 | 23.991 | 24.008 |
35 | [Dy(HABA)(ABA)](DMA)4] | 27.00 | 6.00 | −26.397 | 2.198 | 52.00 | −67.28 | 66 | 23.991 | 0.009 | 0.657 | 51.987 | 52.007 |
36 | [Gd(BCB)(DMF)](H2O)2 | 1.00 | 10.00 | −1.050 | 4.386 | 15.00 | −47.01 | 67 | 63.998 | 0.002 | −1.063 | 14.996 | 15.013 |
37 | [Gd2(H2O)3(SDBA)3](DMA)3] | 3.00 | 15.00 | −3.987 | 3.114 | 26.00 | −48.84 | 68 | 45.991 | 0.009 | 0.422 | 25.990 | 26.007 |
38 | [In(Hpbic)(pbic)](DMF)2 | 6.00 | 4.00 | −4.715 | 3.200 | 31.00 | −15.35 | 69 | 47.995 | 0.005 | −1.747 | 30.999 | 31.016 |
39 | [Co(SDB)(bpdh)0.5]n | 2.00 | 6.00 | 2.064 | 6.027 | 52.00 | −19.06 | 70 | 9.998 | 0.002 | −0.637 | 51.994 | 52.012 |
40 | [Ca3(TATAB)2(H2O)(MeOH)](DMF)3 | 12.00 | 14.00 | −12.910 | 1.630 | 43.00 | −18.70 | 71 | 56.199 | 0.001 | −0.814 | 42.995 | 43.012 |
41 | Mg(H2TBAPy)(H2O)3·C4H8O2 | 0.00 | 13.00 | −1.265 | 3.400 | 12.00 | −9.40 | 72 | 39.991 | 0.009 | 0.258 | 11.990 | 12.008 |
42 | [Co2(L)(4,4′-Bipy)2]·CH3CN | 6.00 | 10.00 | −5.475 | 5.418 | 20.00 | −13.87 | 73 | 83.997 | 0.003 | 0.620 | 19.989 | 20.006 |
43 | [Sr(HTATB)(H2O)2](DMF)4 | 3.00 | 7.00 | −0.290 | 3.860 | 52.00 | −9.77 | 74 | 95.001 | −0.001 | −0.585 | 51.994 | 52.011 |
44 | [Ba(HTATB)(H2O)2](DMF)4 | 7.00 | 12.00 | −7.495 | 3.860 | 23.00 | −15.84 | 75 | 78.991 | 0.009 | −0.162 | 22.992 | 23.009 |
45 | MIL-100 (Fe) | 0.00 | 24.00 | −2.918 | 2.550 | 24.00 | −7.88 | 76 | 28.991 | 0.009 | 0.988 | 23.987 | 24.005 |
46 | UiO-66 | 0.00 | 20.00 | 0.195 | 1.700 | 64.00 | −7.78 | 77 | 23.994 | 0.006 | −0.289 | 63.992 | 64.010 |
47 | MIL-101-NH2-Fe | 4.00 | 16.00 | −4.873 | 1.082 | 46.00 | −10.54 | 78 | 51.994 | 0.006 | 1.168 | 45.986 | 46.004 |
48 | MIL-88B | 0.00 | 24.00 | −0.211 | 4.564 | 48.00 | −7.44 | 79 | 14.999 | 0.001 | 0.237 | 47.990 | 48.008 |
49 | UiO-66-COOH | 1.00 | 4.00 | −1.025 | 2.922 | 10.00 | −6.36 | 80 | 25.993 | 0.007 | −0.932 | 9.995 | 10.013 |
50 | CP5-capped UiO-66-NH-Q | 7.00 | 62.00 | −14.774 | 3.377 | 56.20 | −20.31 | 81 | 31.003 | −0.003 | −0.442 | 56.192 | 56.212 |
51 | MOF-In1 | 0.00 | 20.00 | −0.646 | 3.342 | 40.00 | −8.55 | 82 | 51.999 | 0.001 | 1.074 | 39.987 | 40.004 |
52 | Mn-ZIF-90 | 4.00 | 2.00 | 1.068 | 2.380 | 84.00 | −2.09 | 83 | 42.999 | 0.001 | 0.036 | 83.991 | 84.009 |
53 | UiO-67-(NH2)2 | 12.00 | 32.00 | −13.236 | 0.464 | 95.00 | −20.00 | 84 | 11.993 | 0.007 | −0.570 | 94.993 | 95.012 |
54 | DCA-UiO-DTDP-FA | 14.00 | 36.00 | −17.144 | 0.622 | 79.00 | −22.83 | 85 | 19.992 | 0.008 | 1.759 | 78.983 | 79.002 |
RMSEP | 0.006 | ||||||||||||
Test set (13 entries) | |||||||||||||
55 | [Zn3(μ3-O)(BTC)2(DMF)]·2NH2(CH3)2·4H2O | 3.00 | 18.00 | −3.087 | 2.550 | 51.00 | −10.32 | 32 | 50.999 | 0.001 | −0.559 | 50.993 | 51.011 |
56 | [Zn(bptc)(H2O)]·(DMA)4 | 4.00 | 13.00 | −4.317 | 3.400 | 29.00 | −10.09 | 86 | 28.991 | 0.009 | 1.206 | 28.986 | 29.005 |
57 | [Zn2(L)(H2O)1.5]·5H2O | 1.00 | 9.50 | −0.476 | 4.095 | 24.00 | −7.09 | 87 | 23.995 | 0.005 | 0.405 | 23.988 | 24.009 |
58 | [Zn3(bdc)2(dfp)2]·2DMF | 2.00 | 12.00 | 0.844 | 4.330 | 63.00 | −13.64 | 38 | 62.996 | 0.004 | 0.236 | 62.988 | 63.010 |
59 | [Zn(H2O)6K2(H2BTC)2(H2O)4](H2BTC)2·2H2O | 0.00 | 36.00 | −3.904 | 2.550 | 42.00 | −8.06 | 88 | 41.993 | 0.007 | 0.819 | 41.986 | 42.008 |
60 | ZIF-8 | 5.00 | 4.00 | −3.831 | 1.896 | 38.00 | −6.19 | 89 | 37.998 | 0.002 | −0.325 | 37.991 | 38.011 |
61 | [(Zn2(L1)(DMA)]·1.75DMA | 3.75 | 10.75 | −3.975 | 4.095 | 19.00 | −7.04 | 59 | 18.998 | 0.002 | −0.830 | 18.993 | 19.013 |
62 | ZIF-90 | 2.00 | 0.00 | 0.482 | 2.375 | 40.00 | −7.64 | 90 | 39.996 | 0.004 | 0.744 | 39.988 | 40.007 |
63 | [Zn10(OH)O(BTC)5(HBTC)(DMA)2(H2O)4]·11DMA | 13.00 | 55.00 | −21.242 | 2.550 | 42.00 | −27.15 | 91 | 41.991 | 0.009 | −0.330 | 41.989 | 42.013 |
64 | [Dy2(L)2(H2O)2]n | 0.00 | 14.00 | 0.912 | 2.550 | 52.00 | −10.18 | 92 | 51.999 | 0.001 | −0.058 | 51.991 | 52.010 |
65 | FA-MOF-808 | 0.00 | 12.00 | 0.797 | 2.550 | 45.00 | −5.48 | 93 | 45.005 | −0.005 | −1.695 | 44.997 | 45.016 |
66 | FA-NH2-UiO-66 | 4.00 | 20.00 | −5.901 | 1.082 | 42.00 | −13.01 | 93 | 41.994 | 0.006 | 0.877 | 41.987 | 42.007 |
67 | MIL-88B | 0.00 | 20.00 | −2.743 | 1.700 | 22.00 | −38.24 | 94 | 21.999 | 0.001 | −0.492 | 21.991 | 22.012 |
RMSEP | 0.0052 | ||||||||||||
External validation test set (8 entries) | |||||||||||||
68 | Zn6(L)3(DMA)4]·5DMA | 9.00 | 33.00 | −10.35 | 3.400 | 72.00 | −13.61 | 95 | 71.998 | 0.002 | −0.931 | 71.986 | 72.022 |
69 | [Zn3(BTC)2(Aml)(H2O)2](MeOH)6 | 6.00 | 14.00 | −7.12 | 2.296 | 30.00 | −12.12 | 96 | 29.997 | 0.003 | −0.519 | 29.985 | 30.019 |
70 | [[Dy2(H2O)3(SDBA)3](DMA)6] | 0.00 | 21.00 | −1.72 | 3.114 | 29.00 | −12.00 | 97 | 28.990 | 0.010 | 0.551 | 28.980 | 29.015 |
71 | [Gd2(TATAB)2]·6DMF | 12.00 | 12.00 | −11.28 | 1.630 | 61.00 | −49.29 | 98 | 60.997 | 0.003 | 0.090 | 60.982 | 61.017 |
72 | [Mg3(H2O)4(5-aip)2(5-Haip)2]·4DMA | 8.00 | 24.00 | −9.00 | 1.082 | 69.00 | −13.89 | 99 | 68.991 | 0.009 | 0.869 | 68.979 | 69.014 |
73 | [Ca3(TATB)2(H2O)](DMF)4(H2O) | 6.00 | 13.00 | −2.78 | 3.860 | 78.00 | −12.06 | 100 | 77.994 | 0.006 | 0.671 | 77.979 | 78.015 |
74 | NanoHKUST-1 | 0.00 | 12.00 | 2.06 | 2.550 | 63.00 | −3.65 | 101 | 62.996 | 0.004 | −0.167 | 62.985 | 63.017 |
75 | Fe-MIL-53-NH2 | 1.00 | 4.00 | 2.37 | 1.082 | 72.00 | −3.70 | 102 | 71.999 | 0.001 | −0.565 | 71.985 | 72.020 |
RMSEP | 0.0054 |
The statistical coefficients, R2 (coefficient of determination) and Radj2 (the adjusted R-squared), were calculated as follows (eqn (1) and (2)):
(1) |
(2) |
(3) |
(4) |
(5) |
(6) |
(7) |
After the BMLR model has been developed with the original dataset, the new observations (the new set of compounds) investigate the model's validity by computing Q(Ext)2, Q(Ext)F12, Q(Ext)F22, Q(Ext)F32, and Q(Ext)CCC2.
RES% = 20.135 + 15.157nN + 2.675nO − 7.300RES− + 14.296RES+ | (8) |
According to our previous works,30,31 to estimate the important properties of materials, simple group-contribution methods can be employed, and the values of RES− were determined based on this technique. This study found a reliable contribution between various particular molecular fragments of the linker and the drug release rate from MOFs, RES%. Table 2 lists different RES− values; these values have been determined for several molecular fragments of linkers, which are the result of the core correlation. In Table 2, for the substituents containing nitrogen or oxygen attached to one or more rings, the ring symbol is used for simplicity.
As mentioned above, RES+ represents one of the descriptors that increase the RES%. It is obtained from eqn (9) and consists of two parts: RESM and IM–L. The RESM results from eqn (10) and is calculated by considering the molecular weight of MOF and the atomic mass of oxygen and nitrogen, as well as the impact of d-orbitals of the metal center. IM–L describes the interaction between the d-orbitals of the metal center and the valence orbitals of heteroatoms of linkers. The IM–L value resulted from our experimental inorganic chemistry knowledge and can be applied to a variety of interactions. Fig. 1 represents the molecular orbital diagram resulting from the interaction of metal d-orbitals and the heteroatoms of linkers for an octahedral geometry of SBU, as an example.
RES+ = RESM + IM–L | (9) |
RESM = [(MOFMw)/(nOmO + nNmN)] × ∑Ed(SBU) | (10) |
Fig. 1 Molecular orbital diagram indicating the interaction of metal d-orbitals and the heteroatoms of linkers. |
The energies of the d-orbitals for the metal center are considered through the Krishnamurthy and Schaap findings.103 Hence, the relative energies of d orbitals in crystal fields of different metal center geometries were calculated based on Krishnamurthy and Schaap's approach (Table 3).
Coordination number | Metal center configuration | Relative energy of d-orbitals in units of Dq | ||||
---|---|---|---|---|---|---|
dz2 | dx2–y2 | dxy | dxz | dyz | ||
1 | ML (z) | 5.14 | −3.14 | −3.14 | 0.57 | 0.57 |
2 | ML2 (XY) | −2.41 | 6.14 | 1.14 | −2.57 | −2.57 |
4 | ML4 (Td) | −2.67 | −2.67 | 1.78 | 1.78 | 1.78 |
In other words, first, RESM is calculated by considering the total energies of d-orbitals of metal SBUs using Krishnamurthy and Schaap's approach, then the corresponding interaction between metal and linker heteroatom (IM–L value) is added to the result in the RES+. The values of RES+ and IM–L for the training and test sets are listed in Table 1.
In this work, the geometries of the metal centers (SBUs) of MOFs were diverse, including octahedral, trigonal bipyramid, tetrahedral, square planar, square pyramidal, pentagonal bipyramid, square antiprism, and triangular dodecahedral. If the metal center is six-coordinated in octahedral coordination geometry, the d orbitals split into two sets, as shown in Table 4, first row. According to Table 3, the field for ML6 will be ML6 (Oh) = 2ML2(XY) + 2ML(Z), and the total energies of the d-orbitals for octahedral geometry are obtained as ∑Ed(Oh) = 2 Dq. The d-orbitals of the metal center under a tetrahedral crystal field are split in e and t2 orbitals (dz2, dx2–y2) (dxy, dxz, dyz). Regarding Table 3, the summation of d-orbital energies for tetrahedral geometry is ∑Ed(Td) = −0.89 Dq (Table 4, first row). Whenever the metal SBU is connected to five adjacent ligands to afford the square pyramidal environment, it causes the d orbitals to split into four groups with different energies, as listed in Table 4, second row. Considering Table 3, a square pyramidal field with C4V symmetry is considered as ML5 (C4V) = 2ML2(XY) + ML(Z), then the sum of d-orbital energies for square pyramidal configuration is derived by ∑Ed(C4V) = 4.57 Dq. The square planar geometry of metal centers with D4h symmetry creates a d-orbital splitting, shown in Table 4, second row. Its corresponding field is twice that of the ML2(XY) field, ML4(S.P.) = 2ML2(XY), and the sum of d-orbital energies is equal to 5.14 Dq. The metal d-orbital splitting diagram for trigonal bipyramidal metal SBU geometry is illustrated in Table 4, third row. For T.B.Py. with symmetry D3h, the respective field is The total energy of d-orbitals for trigonal bipyramidal geometry is ∑Ed(D3h) = 3.53 Dq, and the corresponding RES+ variables are calculated. For metal SBUs having pentagonal bipyramidal (D5h), the crystal field splitting is displayed in Table 4, third row, and its field is considered as The consequent energies of the d orbitals is ∑Ed = −2.47 Dq. When the metal center is eight-coordinate, it can form square antiprism geometry with D4d symmetry. The d-orbital splitting is considered in Table 4, fourth row, and concerning Table 3, its field results from ML8 = 2ML4 (Td), but considering that in a cube, four ligands in the upper plate rotate 45°; the energy value of the dxy and dx2–y2 orbitals equal the average energy of the two orbitals in the cube configuration. Afterward, the resultant energies of the d orbitals are obtained by ∑Ed(D4d) = −2.67 Dq. The last studied metal SBU has triangular dodecahedral geometry with D2d symmetry. The metal d-orbital splitting diagram for this type of metal center geometry is exhibited in Table 4, fourth row. Its field is considered as therefore, according to Table 3, the total energy of the d orbitals is ∑Ed = −10.68. As mentioned above, the respective RES+ is acquired from eqn (9), and Table 1 presents the corresponding RES+ values.
To validate the proposed QSPR model, an external validation method was employed using new data points and the statistical parameters obtained from the model for the external set, proving the accuracy and reliability of the proposed model. From the resulting BMLR model (eqn (8)), R2 and adjusted R2 values both are 0.9999 for the training and test sets. As shown in Table 5, correlation parameters for the test set, including QF12, QF22, QF32, and QCCC2 of the model yielded 0.9999. These correlation parameters for the external validation test set were acquired at 0.9999 as well, which demonstrated that the model is very credible and robust.
R2 and Q2 tests | ||||||||
---|---|---|---|---|---|---|---|---|
Method | Sets | R2 | Radj2 | Q2 | QF12 | QF22 | QF32 | QCCC2 |
Eqn (8) | Training set | 0.9999 | 0.9999 | — | — | — | — | — |
Test set | 0.9999 | 0.9999 | 0.9999 | 0.9999 | 0.9999 | 0.9999 | 0.9999 | |
External validation test set | 0.9999 | 0.9999 | 0.9999 | 0.9999 | 0.9999 | 0.9999 | 0.9999 |
The root mean square error for prediction (RMSEP) values were 0.006, 0.0052, and 0.0054 for the training, test, and external validation test sets, respectively. Also, the mean absolute percentage errors (MAPE) were 0.012, 0.0073, and 0.0044 as shown in Table 6, which are low values for RMSEP and MAPE; thus, the model is suitable to estimate the drug release rate values from MOF materials.
Eqn (8) | No. of MOFs | RMSEP | MSE | MAPE | F statistic | Significance F |
---|---|---|---|---|---|---|
Training set | 54 | 0.0063 | 0.000 | 0.012 | 373493505.6 | 1.109 × 10−182 |
Test set | 13 | 0.0052 | 0.000 | 0.0073 | 35334456.7 | 5.1323 × 10−29 |
External validation test set | 8 | 0.0054 | 0.000 | 0.0044 | 34571821.9 | 7.988 × 10−12 |
The predicted and experimental values of drug release rate percentage for the training and test sets are shown in Fig. 2. It well proves that the predicted values of drug release rate percentage are fitted on the experimental values.
Fig. 2 Predicted values of drug release rate for the training and test sets versus the experimental values of drug release rate. |
As can be observed from Table 7, the standard error (SE) for all descriptors are low values, which confirms that the proposed model is appropriate and robust. The probability values (p-values) of the descriptors are very small, confirming that the data could have occurred under the null hypothesis. Other parameters, such as t-test, significance level, and lower and upper bound values for descriptors are presented in Table 7. It can be concluded from Table 7 that all variables in eqn (8) have large effects on the resulting model. The VIF and tolerance for these descriptors are near 1, showing that there is no intercorrelation among the variables.
Equation | Des.a | Coef.b | S.E.c | P-Value | t-Test | Sig.d | L.B.e (95%) | U.B.f (95%) |
---|---|---|---|---|---|---|---|---|
a Descriptor.b Coefficients.c Standard error.d Significance level.e Lower bound.f Upper bound.g Intercept. | ||||||||
Eqn (8) | Int.g | 20.135 | 0.0021 | 1.563 × 10−155 | 9662.987 | <0.0001 | 20.139 | 20.130 |
nN | 15.157 | 0.0004 | 5.7733 × 10−184 | 36759.32 | <0.0001 | 15.158 | 15.156 | |
nO | 2.675 | 0.0001 | 2.76 × 10−180 | 30922.6 | <0.0001 | 2.675 | 2.675 | |
RES+ | −7.301 | 0.0005 | 1.4903 × 10−166 | −16219 | <0.0001 | −7.300 | −7.302 | |
RES− | 14.296 | 0.0004 | 9.219 × 10−184 | 36409.89 | <0.0001 | 14.297 | 14.296 |
MOF design and RES calculation are accomplished through the descriptors in eqn (8) and also by considering the “mean effect”. Two parameters are involved the “mean effect”: (a) the coefficient of descriptors and (b) the nature of descriptors. The value assigned to the nature of descriptors may be positive or negative (Table 1); the coefficient of descriptors can also be positive or negative (the coefficients that appear in eqn (8)). After putting the values of the descriptors in eqn (8), the MOF design can be performed.104
For further assessment, the cross-validation method was used to make sure overfitting did not occur in modeling.105 Therefore, leave-one-out (LOO) and y-randomization (yrand) procedures were employed as cross-validation techniques. The values of RLOO2 and Ryrand2 were obtained at 0.999 and 0.206, respectively. The resulting values confirm the model's accuracy in predicting the release rate percentage (RES%) from MOFs. Also, Ryrand2 > 0.5 indicated that there is no chance correlation in the model. Moreover, the Durbin–Watson (DW) statistic of the proposed model was obtained at 2.453, which indicates that there is no autocorrelation in the residuals from the BMLR model. The acceptable range of DW is 1.50–2.50.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3ra00070b |
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