The geometric structure of the penicillin molecule
Figure 1 shows the optimized spatial structure of penicillin molecules. It can be seen from the figure that the tension of the four-atom β-lactam ring and the five-atom tetrahydrothiazole ring is very high, resulting in the torsion of the structure. Thus, the penicillin molecule is not a simple planar structure, but a complex three-dimensional structure.
The results of configuration optimization and frequency calculation of penicillin molecules are shown in Table 1. According to the table, the maximum force change is 0.00004 a.u., the root mean square (RMS) of force change is 0.00001 a.u., the maximum displacement is 0.000573 a.u., and the root mean square value of displacement is 0.000150 a.u.. All of them meet the convergence standard and have no virtual frequency. This indicates that the molecular structure of penicillin is optimized to a stable structure with a local minimum energy value, and the structural optimization is reasonable. The energy of the optimized penicillin molecule is -1429.44Hartree.
Table 1
Optimization results of penicillin molecular geometry configuration
Maximum force change
|
RMS of force change
|
Maximum displacement
|
RMS of displacement
|
0.000004a.u.
|
0.00001a.u.
|
0.000573a.u.
|
0.000150a.u.
|
convergence
|
convergence
|
convergence
|
convergence
|
The properties of excited states
The highest occupied molecular orbital (HOMO) and the lowest unoccpied molecular orbital (LUMO) of penicillin are the 88th and 89th electron orbital, respectively. The excited state properties of penicillin are shown in Table 2. It can be seen from Table 2that the contribution of the electron transition to the excited state is not only related to the HOMO and LUMO, but also related to the orbital adjacent to the HOMO and LUMO. These are the frontier orbits of penicillin molecules (Parr et al. 1984).
Table 2
Properties of excited states of penicillin molecules
Excited state
|
wavelength (nm)
|
Energy(eV)
|
Oscillator strength (a.u.)
|
Orbital transitions
|
Contribution weight (%) (> 10%)
|
2
|
235.09
|
5.28
|
0.018
|
88→92
|
24.37%
|
88→90
|
19.42%
|
85→92
|
12.43%
|
85→89
|
11.47%
|
4
|
226.88
|
5.47
|
0.101
|
87→90
|
49.34%
|
83→90
|
12.97%
|
9
|
214.33
|
5.79
|
0.034
|
88→93
|
29.14%
|
88→90
|
26.77%
|
11
|
209.08
|
5.93
|
0.028
|
85→89
|
21.03%
|
87→92
|
18.49%
|
82→89
|
14.69%
|
12
|
208.17
|
5.96
|
0.028
|
87→90
|
19.41%
|
86→91
|
16.77%
|
87→92
|
16.38%
|
3.3 Ultraviolet spectrum
On the basis of configuration optimization of penicillin molecule, 25 excited states of penicillin molecule in aqueous solution were calculated by using B3LYP method and Gaussian09 software based on TD-DFT. The threshold value of vibrator intensity is set as 0.01a.u., and the excited state with vibrator intensity lower than 0.01a.u. is not considered. Five excited states with vibrator intensity greater than 0.01a.u. of penicillin molecule can be obtained. The UV spectrum was drawn by Origin2017 software, as shown in Fig. 2, where S0 represents the ground state in UV excitation, and Sx represents the x state in UV excitation. The ultraviolet spectrum of penicillin molecule is mainly formed by the electron transition from the ground state S0 to the excited states S2, S4, S9, S11 and S12. The theoretical calculation results of UV spectrum agree well with experiment (Qian 2002; Sun et al. 2012; Faith et al. 1977; Martínez et al. 2009).
As can be seen from Fig. 2, the maximum absorption peak of penicillin molecule is located at 220.89nm, and its molar absorption coefficient is 6960.18L/mol/cm. The contribution of the main excited state transition of penicillin molecule to the maximum absorption peak of ultraviolet spectrum is shown in Table 3.
Table 3
Contribution of different transitions to UV spectrum
transition
|
Molar absorption coefficient(L/mol/cm)
|
Contribution (%)
|
S0→S2
|
360.77
|
5.18%
|
S0→S4
|
3575.26
|
51.37%
|
S0→S9
|
1146.89
|
16.48%
|
S0→S11
|
595.83
|
8.56%
|
S0→S12
|
543.30
|
7.81%
|
Active site
Fukui function method
Three states of penicillin molecule were calculated with Gaussian09 respectively: uncharged state, a positive charge state and a negative charge state, that is, N, N + 1 and N-1 states. The isosurface of the molecule is set to 0.003a.u., and the Fukui function (Fukui 1970) in the software Multiwfn3.7 is used for calculation. The isosurface of the value of the Fukui function is obtained as shown in Fig. 3 and Fig. 4 respectively, where the green area of the isosurface is the positive part, and the blue area of the isosurface is the negative part. In general, the Fukui function value of the active site of molecular chemical reaction is large, that is, the higher the electron cloud density on an atom or group, the more likely that atom or group will be the active site of the molecular chemical reaction (Fu et al. 2014; Cao et al. 2015). On the f + isosurface, the density of electron cloud is the highest around C35 atom, that is, C35 atom may be the nucleophilic site of this molecule. On the f − isosurface, the electron cloud density around the atom S25 is the highest, that is, the atom S25 may be the electrophilic site of the molecule.
3.4.2 Frontier orbital theory
Hirshfeld method was used to calculate the contribution of each atom to HOMO and LUMO, and only the top 10 contributing atoms were listed, as shown in Table 4. It can be seen from Table 4 that the atom S25 makes the largest contribution to HOMO, with a contribution rate of 55.46%. It is vulnerable to electrophilic reaction due to electrophilic reagent attack, that is, it may be the electrophilic site of penicillin. Atom C35 has the largest contribution to LUMO, with a contribution rate of 22.05%. It is vulnerable to attack by nucleophile and nucleophile reaction occurs, that is, it is most likely to be the nucleophile site of penicillin. The active sites predicted by frontier orbit are consistent with those predicted by Fukui function.
Table 4
Contribution of each atom to the frontier orbital
Atomic number
|
Contribution to HOMO
|
Atomic number
|
Contribution to LUMO
|
25S
|
55.46%
|
35C
|
22.05%
|
20C
|
3.93%
|
25S
|
19.57%
|
16N
|
3.80%
|
36O
|
15.11%
|
6C
|
3.04%
|
26C
|
6.69%
|
18C
|
2.99%
|
37O
|
6.43%
|
22O
|
2.94%
|
23C
|
6.28%
|
3C
|
2.86%
|
24N
|
3.65%
|
41O
|
2.67%
|
20C
|
3.47%
|
26C
|
2.57%
|
40H
|
2.28%
|
31C
|
2.17%
|
19C
|
2.23%
|