

乳酸配合物(NH4)2[Sr(C3H5O3)4]的晶体结构、Hirshfeld表面分析和溶液化学性质
English
Crystal structure, Hirschfeld surface analysis and solution chemical properties of lactate complex (NH4)2[Sr(C3H5O3)4]
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0. Introduction
At present, the chemical research on lactic acid has gradually shifted from industrial and pharmaceutical applications to basic theoretical research. The research on the coordination of lactic acid with metals is an important aspect[1]. Lactic acid molecules contain adjacent hydroxyl and carboxyl groups. When coordinated with metal, one oxygen atom in the hydroxyl group and two oxygen atoms in the carboxyl group can participate in coordination. Therefore, metal complexes of lactic acid have the characteristics of many coordination sites, large coordination numbers, and various coordination forms. The molecular structure of lactic acid is small and there is no conjugation in the molecule, so the coordination has little effect on the chemical properties. Lactic acid is often used as a filler to react with other macrocyclic ligands with rare earth to form mixed complexes[1-4]. In addition, a series of physical properties such as metal solubility can be changed through the water solubility and other properties of lactic acid. Although there are many reports on the synthesis and application of metal complexes of lactic acid[5-8], these reports mainly focused on food additives and nutrients, such as the effect of zinc lactate additives on protein solubility[9]. There are few reports on their structural chemistry, thermochemistry, and solution chemistry in the literature, especially the accurate study of lactate electrolyte aqueous solution by isoperibol solution - reaction calorimeter. To deeply understand the thermodynamic regularity between the structure and properties of these complexes[10-14], it is necessary to study the coordination mode of lactic acid with metal ions and the thermodynamic properties of their interaction in solution.
The idea of this work is to characterize the structure of the complex by X-ray single crystal diffractometer and to determine its composition and crystal space structure. With the aid of the solution reaction calorimeter, the change of thermal effect in the dissolution process of the complex was accurately measured. According to the theories and methods of solution chemistry, the interaction regularity of complex in solution was deeply studied. It provides data reference for the further study of metal complexes of lactic acid.
1. Experimental
1.1 Synthesis
Details of the reaction reagents are listed in Table 1. D/L - lactic acid, ammonia, and strontium hydroxide react in a molar ratio of 4:2:1. Lactic acid and strontium hydroxide were weighed respectively according to the molar ratio, dissolved in ultra - pure water, and mixed. The mixture was added into a round bottom flask, and the pH value of the solution was adjusted with approximately a molar amount of ammonia (the pH value was controlled at about 9.0) to make the reaction proceed in an ultra-positive direction. After refluxing for two hours, anhydrous ethanol was added while hot until slightly turbid, and the mixture was filtered while hot. After standing for three weeks, the colorless acicular crystals were precipitated. The resulting equation can be expressed as:
Table 1
Chemical name Chemical formula Source Purity (mass fraction)* CAS No. D/L-lactic acid C3H6O3 Budweiser Chemical Technology Co., Ltd. 90.00% 50-21-5 Strontium hydroxide Sr(OH)2 Tianjin Fengchuan Chemical Reagent Technology Co., Ltd. 99.99% 18480-07-4 Absolute ethanol C2H5OH Tianjin Fengchuan Chemical Reagent Technology Co., Ltd. 99.99% 64-17-5 Ammonia NH3·H2O Budweiser Chemical Technology Co., Ltd. 25% 1336-21-6 Potassium chloride KCl Budweiser Chemical Technology Co., Ltd. 99.99% 7447-40-7 Ultra-pure water H2O Laboratory self-made 99.99% — *The purity was provided by the supplier. $ \mathrm{Sr}(\mathrm{OH})_2+2 \mathrm{NH}_3 \cdot \mathrm{H}_2 \mathrm{O}+4 \mathrm{C}_3 \mathrm{H}_6 \mathrm{O}_3= \\ \quad\quad\quad\quad\quad\quad \left(\mathrm{NH}_4\right)_2\left[\mathrm{Sr}\left(\mathrm{C}_3 \mathrm{H}_5 \mathrm{O}_3\right)_4\right]+4 \mathrm{H}_2 \mathrm{O} $ The target complex synthesized was (NH4)2[Sr(C3H5O3)4]. After suction filtration and recrystallization three times, the product was dried in a vacuum drying oven for 12 hours, and then it was put into a clean weighing bottle and placed in the drying oven for testing.
The sample was placed in a vacuum desiccator at 298 K to dry in a vacuum for six days, then it was put into the weighing bottle and preserved in a desiccator. The actual mass fraction of the sample was more than 90% by a chromatographic method (HPLC) and ion chromatography (for each ion). Through calculation, the yield of the reaction was more than 90%. It should be noted that the yield of the reaction was not the most critical factor, because we had to recrystallize the primary product of the reaction. The X - ray diffraction (XRD) pattern of the sample is shown in Fig. 1. The instrument was an XD - 2700 X - ray diffractometer (Cu Kα1, λ =0.154 06 nm) with a voltage of 40 kV, current of 35 mA, and scanning range (2 θ) of 5°-45°. The mass fraction (purity) of Sr in the complex was determined by chemical analysis. C, N, and H were determined using element analysis (model: PE-2400, Perkin-Elmer, USA). Elemental analysis Calcd. for (NH4)2[Sr(C3H5O3)4](%): Sr, 18.33; C, 30.01; N, 5.82; H, 5.83. Found(%): Sr, 18.25; C, 30.03; N, 5.84; H, 5.88.
Figure 1
1.2 X-ray crystallography
The crystal with a size of 0.23 mm×0.20 mm×0.18 mm was glued to the fine glass fibers and then mounted on the Bruker Smart-1000 CCD diffractometer with Mo Kα radiation (λ=0.071 073 nm). The intensity data were collected in the φ-ω scan mode at T=298 K. The structure was solved by the direct method and the differential Fourier synthesis, and all non-hydrogen atoms were refined anisotropically on F2 by the full - matrix least-squares method. All calculations were performed with the SHELXTL program package. The program used in the building structure was Diamond 3.2 software.
1.3 Quantum chemical calculation
The graphics software selected for quantum chemical calculation in this experiment was CrystalExplorer17.5[15]. CrystalExplorer17.5 provides a new way of visualizing molecular crystals using the full suite of Hirshfeld surface tools[16]. Hirshfeld surface is the isosurface with a weight coefficient, w(r), equal to 0.5. The average charge density of molecules inside the isosurface should exceed the average charge density of all surrounding molecules (w(r) < 0.5 within the isosurface, w(r)≥0.5 outside the isosurface). This ratio was also approximately the ratio of the charge density of real molecules to that of real crystals. Hirshfeld surface[16] is a new definition of molecular surface. Hirshfeld surface analysis can get real and continuous 3D visualization, and 2D fingerprint is the 2D representation of Hirshfeld surface analysis.
1.4 Isoperibol solution-reaction calorimetry
The model of the isoperibol solution-reaction calorimeter used in this work is SRC - 100. This model of the calorimeter was developed and improved by Yu and Dong et al.[17] based on summing up years of experience in thermochemistry and calorimetry and referring to the work of their counterparts at home and abroad. It has the characteristics of simple operation and high precision. To obtain a certain experimental accuracy, the SRC-100 requires a sample mass of 0.2-0.6 g each time. The total mass of each sample was 1 - 3 g when calculated five times in parallel according to each group of experiments. After weighing the sample, we dissolved it in a Dewar bottle filled with 100 mL of ultra - pure water. The Dewar bottle needed to be preheated in a constant-temperature water bath for several minutes before the test. The test process might produce a certain degree of uncertainty. This uncertainty was a comprehensive uncertainty considering factors such as mass weighing, electric energy calibration (including current, resistance, time), and temperature rise change. The precision and accuracy of the instrument needed to be checked and corrected by chemical calibration. In this experiment, the KCl calibrator was dissolved in ultra-pure water for calibration. The details were as follows: an electronic balance with an accuracy of more than 0.001 g was used to weigh 0.365 g of treated highpurity KCl, and the KCl was dissolved in 100 mL of ultra - pure water and then measured. The enthalpy of dissolution of KCl obtained was (17.602±0.014) kJ·mol-1, as shown in Table 2. This result was close to the literature value[18] of (17.597±0.017) kJ·mol-1.
Table 2
No. m / g n / mmol ΔsHm/(kJ·mol-1) 1 0.374 7 5.026 2 17.559 2 0.374 7 5.026 2 17.628 3 0.374 8 5.027 5 17.580 4 0.375 2 5.032 9 17.629 5 0.374 6 5.0248 17.612 1.5 Differential thermal analysis
The detection instrument used for thermogravimetric (TG) and differential thermogravimetric (DTG) analysis was the DTA - 1700 differential thermal analyzer. The measurement was taken in the Al2O3 crucible with the sample mass of 5 mg under air atmosphere (40 mL·min-1). Dynamic scans were performed at the heating rate of 10 ℃ ·min-1 in a temperature range of 20-800 ℃. From the TG curve, relevant data such as thermal stability and thermal analysis product of the sample could be obtained, and the relationship between the sample mass change rate and temperature could also be obtained.
2. Results and discussion
2.1 Description of crystal structure
Table 3 shows that the crystal of (NH4)2[Sr(C3H5O3)4] is monoclinic, and the space group is C2/c. The selected bond lengths and angles of the complex are listed in Table 4. The information on hydrogen bonds is shown in Table 5.
Table 3
Parameter (NH4)2[Sr(C3H5O3)4] Empirical formula C12H28SrN2O12 Formula weight 479.98 Crystal system Monoclinic Space group C2/c a / nm 1.799 02(16) b / nm 1.047 00(11) c / nm 1.074 31(13) β/(°) 93.581 0(10) Volume / nm3 2.019 6(4) Z 4 Dc / (g·cm-3) 1.579(2) Absorption coefficient / mm-1 2.73 F(000) 992 θ range for data collection / (°) 2.25-25.02 Limiting indices -21 ≤ h≤ 21, -12 ≤ k≤ 10, -12 ≤ l≤ 9 Reflection collected, unique 5 061, 1 793 (Rint=0.051 5) Completeness to θ=25.02°/ % 99.9 Absorption correction Semi-empirical from equivalents Max. and min. transmission 0.639 3 and 0.448 3 Data, restraint, number of parameters 1 793, 0, 155 Goodness-of-fit on F2 1.037 Final R indices [I > 2σ(I)] R1=0.042 0, wR2=0.108 0 R indices (all data) R1=0.051 4, wR2=0.112 2 (Δρ)max and (Δρ)min / (e·nm-3) 714 and -514 Table 4
Sr1—O1 0.256 3(3) Sr1—O6 0.2540(3) Sr1—O3 0.257 0(3) Sr1—O4 0.251 2(3) O5—C4 0.130 6(11) O6—C5 0.143 2(19) O1—C1 0.123 0(5) C1—C2 0.1527(5) O2—C1 0.125 7(4) C2—C3 0.151 4(7) O3—C2 0.1427(4) C4—C5 0.150(2) O4—C4 0.119 5(5) O1—Sr1—O1ⅰ 91.20(13) O1ⅰ—Sr1—O3 94.29(9) O6ⅰ—Sr1—C4ⅰ 44.56(10) O4ⅰ—Sr1—O4 78.68(15) O6—Sr1—C4ⅰ 97.58(11) O4—Sr1—O6ⅰ 82.77(10) C4ⅰ—Sr1—C1ⅰ 157.69(11) O1—Sr1—O3 59.84(8) O4—Sr1—O6 61.71(9) C1—O1—Sr1 122.9(2) C2—O3—Sr1 121.0(2) O1ⅰ—Sr1—C1ⅰ 17.73(9) C4—O4—Sr1 124.5(3) O1—Sr1—C1ⅰ 99.88(9) O4—Sr1—C1ⅰ 84.64(10) C5—O6—Sr1 124.1(8) O1—Sr1—C4ⅰ 92.95(11) O4ⅰ—Sr1—C1ⅰ 163.05(10) O1—C1—O2 124.9(4) O1ⅰ—Sr1—C4ⅰ 175.00(11) O4—Sr1—C4ⅰ 78.31(12) O1—C1—C2 119.3(3) O3—Sr1—O3ⅰ 144.41(15) O3ⅰ—Sr1—C1ⅰ 44.28(9) O4ⅰ—Sr1—C4ⅰ 17.15(10) O2—C1—C2 115.8(3) O3—Sr1—C1ⅰ 112.01(10) O6—Sr1—O1 133.67(8) O3—C2—C1 106.8(3) O3—Sr1—C4ⅰ 90.20(11) O6ⅰ—Sr1—O1 81.49(10) O3—C2—C3 111.1(4) O3ⅰ—Sr1—C4ⅰ 117.01(10) O6—Sr1—O1ⅰ 81.49(10) C3—C2—C1 110.0(4) O4—Sr1—O1ⅰ 96.99(10) O6—Sr1—O3 119.64(9) O4—C4—O5 122.2(8) O4—Sr1—O1 163.83(9) O6—Sr1—O3 75.08(9) O4—C4—C5 123.6(8) O4—Sr1—O3 132.84(10) O6—Sr1—O6ⅰ 134.37(13) O5—C4—C5 113.4(8) O4—Sr1—O3ⅰ 78.04(10) O6ⅰ—Sr1—C1ⅰ 119.36(9) O6—C5—C4 106.1(12) C4—C5—C6 105.1(13) O6—Sr1—C1ⅰ 86.70(9) O6—C5—C6 106.7(10) Symmetry code: ⅰ -x, y, -z+1/2. Table 5
D—H…A d(D—H) /nm d(H…A) /nm d(D…A) /nm ∠(DHA)/(°) O6—H6…O1ⅱ 0.082 0.194 0.275 5(4) 174.8 O3—H3…O2ⅲ 0.082 0.190 0.270 1(4) 164.8 Symmetry codes: ⅱ x, -y+1, z+1/2; ⅲ -x+1/2, -y+1/2, -z. Fig. 2 shows the molecular structure of (NH4)2 [Sr(C3H5O3)4]. Strontium ion (Sr2+) coordinates with the oxygen atom of carboxyl and the hydroxyl oxygen atom of four lactic acid molecules to form an eight-coordinated complex with a triangular dodecahedron configuration (Fig. 3). Four fivemembered ring structures are formed around Sr2+. Four five - membered rings form an axial symmetric suspension structure to increase the stability of the complex. It can be seen that some carbon and oxygen atoms are disordered in the molecule. It can be seen from Table 4 that the bond length of the Sr—O is not the same, and Sr2+ and oxygen in the coordination group form an irregular coordination triangular dodecahedron of the inner orbit type. Fig. 4 is the crystal cell diagram of (NH4)2 [Sr(C3H5O3)4]. The molecules of (NH4)2 [Sr(C3H5O3)4] are mainly combined by coordination bonds, and the molecules are arranged regularly in space mainly by intermolecular hydrogen bonds. Hydrogen bonds O6—H6…O1ⅱ, O3—H3…O2ⅲ (Table 5) and van der Waals forces exist simultaneously in the crystal to stabilize the structure. NH4+ plays no role in coordination, and its main role is to balance the charge of the whole system.
Figure 2
Figure 3
Figure 4
2.2 Hirshfeld surface analysis
The Hirshfeld surface and 2D fingerprint plot of the complex were created using CrystalExplorer17.5 software. de and di in the 2D fingerprint plot represent the length from the Hirshfeld surface to the outer distance of the nearest atom and from the surface to the inner distance of the nearest atom, respectively. dnorm is the normalized contact distance calculated from de and di[16]. All of them represent intermolecular interactions of the complex. Fig. 5a-5c show the Hirishfeld surface drawn according to dnorm, de, and di, respectively. Among them, the red region and orange region represent the region with the strongest intermolecular force. It can be seen from Fig. 5a-5c that the title compound is a metal complex with more active sites. Fig. 5d is a 2D fingerprint plot corresponding to Fig. 5a. Fig. 6 shows how the breakdown of the 2D fingerprint plot can be used to identify the patterns associated with specific interactions (H…H, H…O, etc.). Fig. 6a and 6b show the close interaction of H…H (accounting for 46.5%), indicating that the intermolecular interaction of the complex mainly depends on hydrogen bond. Fig. 6c and 6d show the H…O interaction (accounting for 20.3%), which is part of the hydrogen bond. It can be seen from the 2D fingerprint plot that the hydrogen bond donor is located inside the Hirshfeld surface. Fig. 6e and 6f show the O…H interaction (accounting for 30.9%), which is part of the hydrogen bond. It can be seen from the 2D fingerprint plot that the hydrogen bond donor is located outside the Hirshfeld surface. The two interactions of H…O and O…H lead to distinct red - spotted areas on the Hirshfeld surface of the complex, which is consistent with the data in Table 5. The intermolecular interaction of the complex mainly depends on O—H…O hydrogen bonding. The Hirshfeld surface and 2D fingerprint plots reveal that the complex has many coordination sites and strong coordination activity. More coordination sites and stronger activity enhance the solubility and chemical reactivity of the complex.
Figure 5
Figure 6
2.3 Calculation of lattice potential energy
The lattice energy of the complex was calculated by the following formula[19]:
$ U_{\text {РОT }}=\left|z_{+}\right|\left|z_{-}\right| v\left(\alpha^{\prime} / V_m^{1 / 3}+\beta^{\prime}\right) $ (1) where z+ and z- are the valences of cations and anions respectively, v represents the total number of anions and cations in each molecule, Vm represents the molecular volume of the complex (Vm can be calculated by the formula VmNA=Mm/ρ, where NA is Avogadro constant, Mm is the relative molar mass, ρ is the density, the values of Mm and ρ can be obtained from Table 1), and α' and β' are fitting coefficients. The charge ratio of cation to the anion of the di-valence metal salt of lactic acid is 1:2, z+=3, z-=1, v=4, α'=133.5 kJ·mol-1·nm, β'=60.9 kJ·mol-1. The lattice energy of the samples could be deduced from the crystallographic data of the metal complex of lactic acid. In addition, for a salt of molecular formula MpXq,
$ V_{\mathrm{m}}\left(\mathrm{M}_p \mathrm{X}_q\right)=p_1 V_{1+}+p_2 V_{2+}+q V_{-} $ (2) where V1+, V2+, and V- are the volumes of the metal cation (M2+), ammonium ion (NH4+), and lactate ion (C3H5O3-), p1 =1, p2=2, and q=4 for (NH4)2[Sr(C3H5O3)4]. According to relevant literature reports[20], VSr2 + and VNH4+ are 0.020 1, 0.021 3 nm3 respectively. When substituted into Eq. 2, the volume size of the anion (C3H5O3-) was 0.103 1 nm3. The values of lattice energy and volumes of anion and cation were listed in Table 6.
Table 6
Complex Vm / nm3 UPOT / (kJ·mol-1) V+ / nm3 V- / nm3 (NH4)2[Sr(C3H5O3)4] 0.504 7 2 742.9 0.092 5 0.103 1 2.4 Molar enthalpies of dissolution at infinite dilution and Pitzer parameters
The molar enthalpies of dissolution of lactate at different concentrations at 298 K were determined by an isoperibol solution - reaction calorimeter, and the molar enthalpy of dissolution of the lactate complex can be expressed as[21]:
$ \Delta_{\mathrm{s}} H_{\mathrm{m}}=\Delta_{\mathrm{s}} H_{\mathrm{m}}^{\infty}+{ }^{\varPhi} L $ (3) Where ΔsHm∞ represents the infinite dilution molar dissolution enthalpy of the sample and ΦL is the apparent relative molar enthalpy. For 2:1 lactate complexes (i.e. divalent metal complexes), the aqueous solution can be represented by Pitzer's electrolyte solution theory[21-23]:
$ { }^{\varPhi} L=2.5 A_{\mathrm{H}} \ln \left(1+1.2 I^{1 / 2}\right)-\\4 R T^2\left[m\left(\beta_{\mathrm{MX}}^{(0) L}+y^{\prime} \beta_{\mathrm{MX}}^{(1) L}\right)+1.4 m^2 1.4 m^2 C_{\mathrm{MX}}^{\varPhi_L}\right] $ (4) $ \beta_{\mathrm{MX}}^{(0) L}=\left(\partial \beta_{\mathrm{MX}}^{(0)} / \partial T\right)_P $ (5) $ \beta_{\mathrm{MX}}^{(1) L}=\left(\partial \beta_{\mathrm{MX}}^{(1)} / \partial T\right)_P $ (6) $ C_{\mathrm{MX}}^{\varPhi_L}=\left(\partial C_{\mathrm{MX}}^{\varPhi} / \partial T\right)_P $ (7) Among them, βMX(0)L and βMX(1)L represent various short-range forces between ions and the three - ion action term, and CMXΦL only shows its important role when the solution concentration is high. The values of βMX(0)L, βMX(1)L, and CMXΦL can be obtained by fitting the measured data in this experiment by the least square method. AH represents the Debye - Huckel parameter of enthalpy, AH=1 986 J·mol-1 at 298 K. m represents the mass molar concentration of the sample (mol·kg-1). For general electrolytes, the absolute values of the βMX(0)L and βMX(1)L parameters are very small (between 10-2 and 10-4), and there is a tendency to increase with the increase of the volume and number of ions.
After substituting Eq.4 into Eq.3 and rearranged, the equation can be derived as follows:
$ \begin{aligned} Y & =\left[\Delta_{\mathrm{s}} H_{\mathrm{m}}-2.5 A_{\mathrm{H}} \ln \left(1+1.2 I^{1 / 2}\right)\right] /\left(2 R T^2\right) \\ & =\alpha_0-2 m \beta_{\mathrm{MX}}^{(0) L}-2 m y^{\prime} \beta_{\mathrm{MX}}^{(1) L} \end{aligned} $ (8) where Y represents the extrapolation function, which can be calculated from experimental data, and α0 and y' are respective:
$ \alpha_0=\Delta_{\mathrm{s}} H_{\mathrm{m}}^{\infty} /\left(2 R T^2\right) $ (9) $ y^{\prime}=\left[1-\left(1+2 I^{1 / 2}\right) \exp \left(-2 I^{1 / 2}\right)\right] /(2 I) $ (10) The experimental value of ΔsHm∞ is subjected to multivariate linear fitting according to Eq. 8, then parameters α0, βMX(0)L, βMX(1)L, and fitted standard deviation s are obtained. The infinite dilution molar dissolution enthalpy ΔsHm∞ of lactate complex in water was calculated by Eq.9.
The relative partial molar enthalpies (L1 and L2) of the solvent and the solute are important thermodynamic data of the electrolyte solution. Generally speaking, there are many ways to determine the relative partial molar enthalpy. The equations used in this article are as follows:
$ \bar{L}_1=-M_{\mathrm{H}_2 \mathrm{O}} m^2\left(\partial^{\varPhi} L / \partial m\right)_{T, P} $ (11) $ \bar{L}_2={ }^{\varPhi} L+m\left(\partial^{\varPhi} L / \partial m\right)_{T, P} $ (12) Under constant temperature and pressure, the partial derivative of Eq.4 for concentration was obtained:
$ \left(\partial^{\Phi} L / \partial m\right)_{T, P}=2.6 A_{\mathrm{H}} /\left(m^{1 / 2}+2.08 m\right)- \\ 4 R T^2\left[\beta_{\mathrm{MX}}^{(0) L}+\beta_{\mathrm{MX}}^{(1) L} \exp \left(-3.46 m^{1 / 2}\right)+2.8 m C_{\mathrm{MX}}^{\varPhi_L}\right] $ (13) The relative partial molar enthalpy L1 of solvent water and the relative partial molar enthalpy L2 of the sample were calculated. The details are listed in Table 7.
Table 7
Table 7. Summary of the molar dissolution enthalpya (ΔsHm), relative partial molar enthalpyb (L1) and (L2) of (NH4)2[Sr(C3H5O3)4] in water at 298 Kmc/(mol·kg-1) ΔsHm/(kJ·mol-1) (∂ΦL/∂m)T, Pd L1 / (J·mol-1) L2 / (kJ·mol-1) 0.66×10-4 110.919 -1.141 11×109 -2.620 5.269 2.31×10-4 104.031 -1.080 41×109 9.323 -3.221 3.80×10-4 98.844 -1.030 67×109 26.534 -9.763 6.12×10-4 92.472 -9.616 2×108 64.334 -18.113 7.70×10-4 89.161 -9.196 5×108 96.959 -22.719 9.18×10-4 86.705 -8.834 7×108 131.999 -26.382 1.048×10-3 84.997 -8.538 0×108 165.980 -29.176 1.225×10-3 83.250 -8.160 0×108 216.474 -32.488 1.483×10-3 81.667 -7.647 1×108 297.308 -36.681 1.669×10-3 81.068 -7.293 1×108 359.689 -39.541 1.957×10-3 80.745 -6.746 9×108 460.699 -44.297 2.245×10-3 80.853 -6.172 6×108 564.085 -50.205 2.847×10-3 81.31 -4.729 3×108 772.909 -70.036 3.468×10-3 80.964 -2.619 9×108 950.814 -107.942 4.285×10-3 79.250 -1.692 7×108 1 070.059 -199.092 a The ratio of the enthalpy of dissolution of the complex to the amount n of the substance under standard pressure is called their standard molar enthalpy of dissolution, written as ΔsHm; b The relative partial molar enthalpies of solvent and solute are expressed as L1 and L2 respectively, which are important thermodynamic parameters of electrolyte solution. The formula used in this work is as follows: L1=-MH2Om2(∂ΦL/∂m)T, P and L2=ΦL+m(∂ΦL/∂m)T, P; c m is the mass molar concentration; d (∂ΦL/∂m)T, P is the partial derivative of relative partial molar enthalpy to m, and its formula is expressed as Eq.13. Fig. 7 shows the tendency of molar enthalpy of dissolution of the complex with concentration. The fitting function expression of molar enthalpy of dissolution is y=112.337 1-40 110.8x+15 766 900x2-1 924 210 000x3, where the fitting similarity is equal to 0.991 5. It can be seen from the curve that its molar enthalpy of dissolution ΔsHm was positive, indicating that the dissolution of the complex is an endothermic process. The infinite dilution molar enthalpy of dissolution ΔsHm∞ of the complex is listed in Table 8, which was (114.01±0.04) kJ·mol-1, considering the relative standard deviation of fitting s. The 3D structure diagram of the extrapolation function Y of the complex varying with -2m and -2my' is drawn in Fig. 8, indicating that the extrapolation function Y has a good linear fitting relationship with the mass molar concentration m. the value of m was brought into Eq. 11, 12, and 13 respectively to calculate the relative partial molar enthalpy sum of solvent and solute, which are listed in Table 7.
Figure 7
Table 8
Table 8. Summary of infinite dilution molar enthalpy of solution and Pitzer's parameters of the complex at 298 KComplex α0 βMX(0)L βMX(1)L s ΔsHm∞/(kJ·mol-1) (NH4)2[Sr(C3H5O3)4] 0.077 17 -8.394 105.196 1.999×10-6 114.01±0.04 Figure 8
Pitzer's theory was used to obtain the parameters α0, βMX(0)L, βMX(1)L, and the fitting standard deviation s. The data were listed in Table 8. It can be seen from Table 7 that the dissolution enthalpy of the complex was positive, indicating that the dissolution process is entropydriven endothermic. This is mainly due to the need to break the coordinate bond (lattice energy) and hydrogen bonds in the complex during the dissolution process, so a large amount of heat needs to be absorbed. In the complex, βMX(0)L was negative, i.e. (∂βMX(0)/∂T)P < 0, indicating that the value of βMX(0)L decreases with the increase of temperature. This indicates that the repulsion force decreases between ions with the increase in temperature. Pitzer parameters (βMX(0)L and βMX(1)L) of the complex were much larger than those of ordinary electrolytes (mostly in a range of 10-4-10-2). This is mainly because the volume of salt ions in the complex is much larger than that of ordinary electrolytes in this work, which also indicates that there is a strong short-range interaction between positive and negative ions in the solution.
2.5 Enthalpy of hydration
The thermodynamic cycle in Scheme 1 was to calculate the hydration enthalpy of the complex. The thermal effect of the formation of C3H5O3- (aq), NH4+ (aq), and Sr2+ (aq) in solution comes from the sum of the hydration enthalpies of the corresponding gaseous ions C3H5O3- (g), NH4+ (g), and Sr2+ (g). According to the thermochemical cycle, the calculation formula of hydration enthalpy of the complex of lactic acid is expressed as[24]:
$ \Delta_{\mathrm{s}} H_{\mathrm{m}}^{\infty}=U_{\mathrm{POT}}+2 R T+\Delta H_{+}+\Delta H_{-} $ (14) Scheme 1
In the formula, ΔH+ is the hydration enthalpy of cations, ΔH- is the hydration enthalpy of anions, and (ΔH++ ΔH-) is the sum of the hydration enthalpies of corresponding ions. Substituting the values of infinite dilution molar enthalpy and lattice energy of the complex into Eq. 14, it can be deduced that the sum of hydration enthalpies of cation and anion in (NH4)2[Sr(C3H5O3)4] was calculated to be -2 633.85 kJ·mol-1. According to the literature[25], the enthalpies of hydration of Sr2+ and NH4+ were -1 470 and -329 kJ·mol-1, respectively. Substituting the lattice energy of the complex and the hydration enthalpy of the corresponding metal cations into Eq. 14, the hydration enthalpy of D/L - lactate ion of (NH4)2[Sr(C3H5O3)4] was calculated to be -834.85 kJ·mol-1.
2.6 TG/DTG analysis
The TG curve (Fig. 9) shows that the non-isothermal degradation, in a dynamic air atmosphere, of the sample occurred through three successive decomposition processes accompanied by mass losses. The weight loss rate from 70 to 230 ℃ was about 7.32%, which is caused by the decomposition of two ammonium ions in the complex and the decomposition of a small number of solvent molecules. From 250 to 520 ℃, the weight loss rate of this process was about 35.41%, which was close to the proportion of lactate ions coordinated by two molecules in the complex structure. From 550 to 750 ℃, the weight loss rate of this process was about 36.32%, which was close to the proportion of lactate ions coordinated by two molecules in the complex structure. There were three obvious peaks in the DTG curve. The corresponding temperatures of the bottoms of the three peaks were 162, 350, and 645 ℃, respectively. This also indirectly proves that the decomposition of the complex is a three continuous decomposition process. It's strong evidence to prove the molecular structure of the complex.
Figure 9
3. Conclusions
The five-memberedring structure is the basic unit of (NH4)2[Sr(C3H5O3)4], and the suspension structure strongly enhancesthe stability of the complex. The metalion Sr2+ of the complex coordinate with the oxygen atoms of the lactate ion to form an eight-coordinated structure. The Hirshfeld surface and 2D fingerprint plot reveal thatthe complex has many coordination sites and strong coordination activity. The lattice energy of the complex wasderived to be 2 742.9 kJ·mol-1. The volume of the D/L - lactate ion was 0.103 1 nm3. The molar enthalpy of dissolution ΔsHm of the complex of lactic acid was positive, indicating that the dissolution process of the complex is entropy-driven and endothermic. The infinite dilution molar enthalpy of dissolution ΔsHm∞ and Pitzer's parameters (βMX(0)L and βMX(1)L) of the complex were calculated and obtained at 298 K. The hydration enthalpy of the complex and its D/L - lactate ion was determined to be -834.85 kJ·mol-1.
Acknowledgments: This work was financially supported by the National Natural Science Foundations of China (Grant No.21873063). -
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[1]
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Table 1. Provenance and purity of the reagents
Chemical name Chemical formula Source Purity (mass fraction)* CAS No. D/L-lactic acid C3H6O3 Budweiser Chemical Technology Co., Ltd. 90.00% 50-21-5 Strontium hydroxide Sr(OH)2 Tianjin Fengchuan Chemical Reagent Technology Co., Ltd. 99.99% 18480-07-4 Absolute ethanol C2H5OH Tianjin Fengchuan Chemical Reagent Technology Co., Ltd. 99.99% 64-17-5 Ammonia NH3·H2O Budweiser Chemical Technology Co., Ltd. 25% 1336-21-6 Potassium chloride KCl Budweiser Chemical Technology Co., Ltd. 99.99% 7447-40-7 Ultra-pure water H2O Laboratory self-made 99.99% — *The purity was provided by the supplier. Table 2. Molar enthalpy of solution of KCl in water at 298 K
No. m / g n / mmol ΔsHm/(kJ·mol-1) 1 0.374 7 5.026 2 17.559 2 0.374 7 5.026 2 17.628 3 0.374 8 5.027 5 17.580 4 0.375 2 5.032 9 17.629 5 0.374 6 5.0248 17.612 Table 3. Crystallographic data of the complex
Parameter (NH4)2[Sr(C3H5O3)4] Empirical formula C12H28SrN2O12 Formula weight 479.98 Crystal system Monoclinic Space group C2/c a / nm 1.799 02(16) b / nm 1.047 00(11) c / nm 1.074 31(13) β/(°) 93.581 0(10) Volume / nm3 2.019 6(4) Z 4 Dc / (g·cm-3) 1.579(2) Absorption coefficient / mm-1 2.73 F(000) 992 θ range for data collection / (°) 2.25-25.02 Limiting indices -21 ≤ h≤ 21, -12 ≤ k≤ 10, -12 ≤ l≤ 9 Reflection collected, unique 5 061, 1 793 (Rint=0.051 5) Completeness to θ=25.02°/ % 99.9 Absorption correction Semi-empirical from equivalents Max. and min. transmission 0.639 3 and 0.448 3 Data, restraint, number of parameters 1 793, 0, 155 Goodness-of-fit on F2 1.037 Final R indices [I > 2σ(I)] R1=0.042 0, wR2=0.108 0 R indices (all data) R1=0.051 4, wR2=0.112 2 (Δρ)max and (Δρ)min / (e·nm-3) 714 and -514 Table 4. Selected bond lengths (nm) and angles (°) of the complex
Sr1—O1 0.256 3(3) Sr1—O6 0.2540(3) Sr1—O3 0.257 0(3) Sr1—O4 0.251 2(3) O5—C4 0.130 6(11) O6—C5 0.143 2(19) O1—C1 0.123 0(5) C1—C2 0.1527(5) O2—C1 0.125 7(4) C2—C3 0.151 4(7) O3—C2 0.1427(4) C4—C5 0.150(2) O4—C4 0.119 5(5) O1—Sr1—O1ⅰ 91.20(13) O1ⅰ—Sr1—O3 94.29(9) O6ⅰ—Sr1—C4ⅰ 44.56(10) O4ⅰ—Sr1—O4 78.68(15) O6—Sr1—C4ⅰ 97.58(11) O4—Sr1—O6ⅰ 82.77(10) C4ⅰ—Sr1—C1ⅰ 157.69(11) O1—Sr1—O3 59.84(8) O4—Sr1—O6 61.71(9) C1—O1—Sr1 122.9(2) C2—O3—Sr1 121.0(2) O1ⅰ—Sr1—C1ⅰ 17.73(9) C4—O4—Sr1 124.5(3) O1—Sr1—C1ⅰ 99.88(9) O4—Sr1—C1ⅰ 84.64(10) C5—O6—Sr1 124.1(8) O1—Sr1—C4ⅰ 92.95(11) O4ⅰ—Sr1—C1ⅰ 163.05(10) O1—C1—O2 124.9(4) O1ⅰ—Sr1—C4ⅰ 175.00(11) O4—Sr1—C4ⅰ 78.31(12) O1—C1—C2 119.3(3) O3—Sr1—O3ⅰ 144.41(15) O3ⅰ—Sr1—C1ⅰ 44.28(9) O4ⅰ—Sr1—C4ⅰ 17.15(10) O2—C1—C2 115.8(3) O3—Sr1—C1ⅰ 112.01(10) O6—Sr1—O1 133.67(8) O3—C2—C1 106.8(3) O3—Sr1—C4ⅰ 90.20(11) O6ⅰ—Sr1—O1 81.49(10) O3—C2—C3 111.1(4) O3ⅰ—Sr1—C4ⅰ 117.01(10) O6—Sr1—O1ⅰ 81.49(10) C3—C2—C1 110.0(4) O4—Sr1—O1ⅰ 96.99(10) O6—Sr1—O3 119.64(9) O4—C4—O5 122.2(8) O4—Sr1—O1 163.83(9) O6—Sr1—O3 75.08(9) O4—C4—C5 123.6(8) O4—Sr1—O3 132.84(10) O6—Sr1—O6ⅰ 134.37(13) O5—C4—C5 113.4(8) O4—Sr1—O3ⅰ 78.04(10) O6ⅰ—Sr1—C1ⅰ 119.36(9) O6—C5—C4 106.1(12) C4—C5—C6 105.1(13) O6—Sr1—C1ⅰ 86.70(9) O6—C5—C6 106.7(10) Symmetry code: ⅰ -x, y, -z+1/2. Table 5. Hydrogenbond parameters of the complex
D—H…A d(D—H) /nm d(H…A) /nm d(D…A) /nm ∠(DHA)/(°) O6—H6…O1ⅱ 0.082 0.194 0.275 5(4) 174.8 O3—H3…O2ⅲ 0.082 0.190 0.270 1(4) 164.8 Symmetry codes: ⅱ x, -y+1, z+1/2; ⅲ -x+1/2, -y+1/2, -z. Table 6. Lattice energy (UPOT) and volumes (Vm) of anion and cation of the complex
Complex Vm / nm3 UPOT / (kJ·mol-1) V+ / nm3 V- / nm3 (NH4)2[Sr(C3H5O3)4] 0.504 7 2 742.9 0.092 5 0.103 1 Table 7. Summary of the molar dissolution enthalpya (ΔsHm), relative partial molar enthalpyb (L1) and (L2) of (NH4)2[Sr(C3H5O3)4] in water at 298 K
mc/(mol·kg-1) ΔsHm/(kJ·mol-1) (∂ΦL/∂m)T, Pd L1 / (J·mol-1) L2 / (kJ·mol-1) 0.66×10-4 110.919 -1.141 11×109 -2.620 5.269 2.31×10-4 104.031 -1.080 41×109 9.323 -3.221 3.80×10-4 98.844 -1.030 67×109 26.534 -9.763 6.12×10-4 92.472 -9.616 2×108 64.334 -18.113 7.70×10-4 89.161 -9.196 5×108 96.959 -22.719 9.18×10-4 86.705 -8.834 7×108 131.999 -26.382 1.048×10-3 84.997 -8.538 0×108 165.980 -29.176 1.225×10-3 83.250 -8.160 0×108 216.474 -32.488 1.483×10-3 81.667 -7.647 1×108 297.308 -36.681 1.669×10-3 81.068 -7.293 1×108 359.689 -39.541 1.957×10-3 80.745 -6.746 9×108 460.699 -44.297 2.245×10-3 80.853 -6.172 6×108 564.085 -50.205 2.847×10-3 81.31 -4.729 3×108 772.909 -70.036 3.468×10-3 80.964 -2.619 9×108 950.814 -107.942 4.285×10-3 79.250 -1.692 7×108 1 070.059 -199.092 a The ratio of the enthalpy of dissolution of the complex to the amount n of the substance under standard pressure is called their standard molar enthalpy of dissolution, written as ΔsHm; b The relative partial molar enthalpies of solvent and solute are expressed as L1 and L2 respectively, which are important thermodynamic parameters of electrolyte solution. The formula used in this work is as follows: L1=-MH2Om2(∂ΦL/∂m)T, P and L2=ΦL+m(∂ΦL/∂m)T, P; c m is the mass molar concentration; d (∂ΦL/∂m)T, P is the partial derivative of relative partial molar enthalpy to m, and its formula is expressed as Eq.13. Table 8. Summary of infinite dilution molar enthalpy of solution and Pitzer's parameters of the complex at 298 K
Complex α0 βMX(0)L βMX(1)L s ΔsHm∞/(kJ·mol-1) (NH4)2[Sr(C3H5O3)4] 0.077 17 -8.394 105.196 1.999×10-6 114.01±0.04 -

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