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Rotational Spectra of Adducts of Formaldehyde with Freons Qian Gou, 1 Gang Feng, 1 Luca Evangelisti, 1 Montserrat Vallejo-López, 2 Alberto Lesarri, 2 Walther Caminati, 1 Emilio J. Cocinero 3 1 Dipartimento di Chimica “G. Ciamician” dell’Università, Via Selmi 2, I-40126 Bologna, Italy 2 Departamento de Química Física y Química Inorganica, Facultad de Ciencias, Universidad de Valladolid, E- 47011 Valladolid, Spain 3 Departamento de Quimica Fisica, Facultad de Ciencia y Tecnologia, Universidad del Pais Vasco,E-48080 Bilbao, Spain. 2013.06.18. Columbus
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2 Introduction With formaldehyde Angew. Chem. Int. Ed., 2011, 50, 7871. Angew. Chem. Int. Ed., 2006, 45, 2438. J. Am. Chem. Soc. 1999, 121, 10098.
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3 I.Difluoromethane − Formaldehyde CH 2 F 2 − H 2 CO Phys. Chem. Chem. Phys., 2013, 15, 6714.
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MP2/6-311++G** calculated spectroscopic parameters of the plausible conformers of CH 2 F 2 – H 2 CO Ab initio calculation 4 ΔE/cm -1 0293 ΔE BSSE /cm -1 0128 A, B, C /MHz13898, 1766, 158410168, 1307, 1176 |μ a |, |μ b |, |μ c |/D2.5, 0.4, 0.04.9, 0.0, 0.0 D J /kHz1.861.97 D JK /kHz13.421445.40 M cc /uǺ 2 1.743.31
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Internal Rotation The 0 + and 0 component lines of the 4 04 3 03 μ a transition of normal CH 2 F 2 – H 2 CO Relative intensity 1:3 5 Rotational spectra
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CH 2 F 2 -HCOH ( 0 + ) CH 2 F 2 -HCOH ( 0 - ) 13 CH 2 F 2 -HCOH ( 0 - ) CH 2 F 2 -H 13 COH ( 0 - ) A/MHz 13725.398(3)13719.351(3)13675(2)13671(2) B/MHz 1737.258(1)1736.720(1)1731.0654(8)1698.7766(8) C/MHz 1559.247(1)1559.218(1)1554.1606(8)1528.0736(8) D J /kHz2.33(1) 2.29(2)2.22(2) D JK /kHz21.25(5)20.78(5)[20.78] d 1 /kHz-0.24(1)-0.23(1)[-0.23] d 2 kHz0.029(6)0.022(6)[0.022] /kHz 2.592.134.942.98 N23 99 Spectroscopic parameters for complex of CH 2 F 2 – H 2 CO including 13 C isotopologues Rotational spectra 6 It’s not possible to determine the vibrational energy spacing (∆E) between the two tunneling states
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Molecular Structure C–H … F–C Bifurcated C–H 2 … O=C Weak hydrogen bonds(WHB) a/Åa/Åb/Åc/Å C CH2F2 Exp.±0.965(3)±0.370(8)0 Cal.-0.982-0.3240 C H2CO Exp.±2.551(1)±0.389(8)0 Cal.2.5720.3200 Substitution coordinates of the two carbon atoms M cc = 1.69 uÅ 2 M cc = 1.65 uÅ 2 7
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Molecular Structure The parameters fitted r H8F2 /Å ∠ C7H8 … F2/° ∠ H8 … F2C1/° Exp.(r 0 )2.658(1)113.56(1)113.41(5) Cal. 2.583114.27114.61 The parameters derived r/År/Åα/°β/° Exp.(r 0 )3.132(1)73.58(5)84.99(5) Cal. 3.09674.1283.65 8
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Internal Rotation Experimental and calculated data Exp.Cal. ∆M aa /uǺ 2 0.0400.039 ∆M bb /uǺ 2 -0.034-0.030 ∆M cc /uǺ 2 0.050 ∆E/MHz-3411 Potential barrier and structural relaxations V 2 =180(10) cm -1 ∆r =0.027Å∆α =-1.4°∆β = 2.6(5)° J. Mol. Spectrosc. 1979, 76, 266 Potential energy pathway Flexible Model Structural relaxations
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10 Internal Rotation Flexible model ERHAM ΔE/GHz /° ΔE/GHz CH 2 F 2 -H 2 O8.20.661.40 CH 2 ClF-H 2 O1.70.821.20 CHClF 2 -H 2 O23.20.6616.01 CH 2 F 2 -CH 2 O2.63.413.78 Tunnelling splittings calculated for some complexes of freons with C 2v symmetric molecules J. Mol. Struct., 2005, 742, 87. Angew. Chem. Int. Ed., 2006, 45, 2438. J. Mol. Spectrpsc.., 2011, 268, 7.
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Dissociation Energy Stretching force constant: Dissociation energy by assuming a Lennard-Jones potential function: a b R CM =3.65 Å 9.3 Nm -1 10.4 kJmol -1 11 J. Chem. Phys. 1983, 78, 3501. Can. J. Phys. 1975, 53, 2007. J. Am. Chem. Soc. 1963, 85, 1715.
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Dissociation Energy ComplexesE D /kJ mol -1 CH 2 F 2 … OCS2.1 (CH 2 F 2 ) 2 6.6 CH 2 F 2 … H 2 O7.5 CH 2 F 2 … C 2 H 4 O9.6 CH 2 F 2 … H 2 CO10.4 J. Phys. Chem. A, 2008, 112, 12616. Angew. Chem. Int. Ed. 1999, 38, 2924. J. Am. Chem. Soc. 1999, 121, 10098. ChemPhysChem 2004, 5, 1779. 12
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13 II. Chlorofluoromethane − Formaldehyde CH 2 FCl − H 2 CO
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14 Ab initio calculation ΔE/cm -1 068130 ΔE BSSE /cm -1 1007 A, B, C /MHz 4976, 1995, 16356014, 1625, 1290 13388, 1196, 1106 |μ a |, |μ b |, |μ c |/D 0.3, 0.0, 0.43.2, 0.8, 0.0 2.3, 0.4, 0.,0 χ aa /MHz 28.2130.11 -67.35 ( χ bb - χ cc )/MHz -59.08-102.32 -6.48 M cc /uǺ 2 27.851.64 1.63 MP2/6-311++G** calculated spectroscopic parameters of the plausible conformers of CH 2 FCl – H 2 CO
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15 Rotational spectra I ( 35 Cl)=3/2 I ( 37 Cl)=3/2 Recorded 3 13 ←2 12 transition of the observed conformer of CH 2 FCl-H 2 CO showing the 35 Cl hyperfine structure and tunnelling splitting due to the internal motion of formaldehyde. Relative intensity 1:3
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16 Rotational spectra 35 Cl 37 Cl 0+0+ 0-0- 0+0+ 0-0- A/MHz5984.591(2)5982.678(2)5818.926(4)5817.196(4) B/MHz1598.0839(4)1597.4318(4)1593.4878(3)1592.8376(3) C/MHz1272.0274(4)1271.9895(4)1261.4602(2)1261.4242(2) χ aa /MHz31.13(1)31.11(2)24.59(4)24.54(5) (χ bb - χ cc )/MHz-105.82(2)-105.84(3)-83.53(4)-83.56(5) Δ c /uÅ 2 -3.38-3.53-3.37-3.52 D J /kHz1.595(2)[1.595] D JK /kHz17.77(4)[17.77] d 1 /kHz0.329(3)[0.329] d 2 /kHz0.086(2)[0.086] /kHz 3.04.2 N15070 Spectroscopic parameters for complex of CH 2 FCl – H 2 CO 6014 1625 1290 30.11 -102.32
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17 Molecular Structure Bond length/ÅValence angle/°Dihedral angel/° Cl2C11.770 F3C11.370F3C1Cl2109.7 H4C11.086H4C1F3109.0H4C1F3Cl2118.7 H5C11.086H5C1F3109.0H5C1F3H4122.6 O6Cl23.554(8)O6Cl2C161.9(2)O6Cl2C1F3180.0 C7O61.215C7O6Cl282.8(10)C7O6Cl2C1180.0 H8C71.104H8C7O6121.6H8C7O6C10.0 H9C71.104H9C7O6121.6H9C7O6H8180.0 Derived structural parameters r 1 /Å2.918α/°120.8 r 2 /Å2.821β/°96.6 R CM /Å3.700γ/°96.7 r 0 and r e (MP2/6-311++G (d, p)) geometries of the CH 2 FCl-H 2 CO C–H … Cl–C Bifurcated C–H 2 … O=C Weak hydrogen bonds(WHB)
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Internal Rotation Experimental and calculated data Exp.Cal. ∆M aa /uǺ 2 0.0570.055 ∆M bb /uǺ 2 -0.045-0.041 ∆M cc /uǺ 2 0.0720.076 ∆E/MHz-5389 Potential barrier and structural relaxations V 2 =125(10) cm -1 ∆R=-0.098Å∆θ=-2.3°∆φ= 12.2(5)° J. Mol. Spectrosc. 1979, 76, 266 Potential energy pathway Flexible Model Structural relaxations R(τ) = R 0 + 1/2 ΔR [1 – cos (2τ)] θ(τ) = θ 0 + 1/2 Δθ [1 – cos (2τ)] ϕ (τ) = ϕ 0 + 1/2 Δ ϕ [1 – cos (2τ)
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Dissociation Energy Stretching force constant: Dissociation energy by assuming a Lennard-Jones potential function: complexk s /Nm -1 E B /kJmol -1 CH 2 FCl … H 2 O8.68.5 CH 2 FCl … H 2 CO8.69.8 J. Chem. Phys. 1983, 78, 3501. Can. J. Phys. 1975, 53, 2007. J. Am. Chem. Soc. 1963, 85, 1715.
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20 III. Chlorotrifluoromethane − Formaldehyde CF 3 Cl − H 2 CO
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MP2/6-311++G** calculated spectroscopic parameters of the plausible conformers of CF 3 Cl – H 2 CO Ab initio calculation 21 ΔE/cm -1 0251385415 ΔE BSSE /cm -1 0364438464 A, B, C /MHz 4821, 787, 7685590, 872, 869 3493, 848, 7753182, 894, 795 |μ a |, |μ b |, |μ c |/D 1.7,2.0,0.02.1, 0.0, 0.0 0.1, 1.7, 0.10.3, 2.8, 0.0 χ aa /MHz -67.4572.49 -1.6124.27 ( χ bb - χ cc )/MHz -6.880.08 -72.00-97.52
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22 Rotational spectra Recorded 6 1 ←5 1 transition of the observed conformer of CF 3 Cl- H 2 CO showing the 35 Cl hyperfine structure and the internal motion of formaldehyde. Feature of symmetric top
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23 Rotational spectra m = 0m = ±1 CF 3 35 Cl-H 2 COCF 3 37 Cl-H 2 COCF 3 35 Cl-H 2 COCF 3 37 Cl-H 2 CO B/MHz776.1356(2)775.7614(3)775.9321(3)775.5624(4) 1.5χ aa /MHz-110.86(2)-87.0(2)-110.3(2)-87.4(4) D J /kHz1.642(1)1.639(3)1.660(3)1.676(5) D JK /MHz1.7050(3)1.7116(2)1.6914(2)[1.6914] H JK /kHz0.670(3)[0.670] σ/kHz4.35.33.72.2 N4832 16 An effective symmetric top
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24 Molecular Structure a/Åa/Å rere -0.342 rsrs ±0.294(5) Assuming that the formation of the complex does not affect the electric field gradient at chlorine nucleus: χ aa = 0.5χ z (3cos 2 θ za - 1) θ = 10.6° r e and r s coordinates of substituted chlorine atom Halogen Bond C −Cl···O=C
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Dissociation Energy Stretching force constant: Dissociation energy by assuming a Lennard-Jones potential function: k s = 128π 4 (μR CM ) 2 B 4 /hD J E B = 1/72k s R 2 CM complexk s /Nm -1 E B /kJmol -1 CF 3 Cl … H 2 O5.07.7 CF 3 Cl … H 2 CO6.311.0 J. Chem. Phys. 1983, 78, 3501. Can. J. Phys. 1975, 53, 2007. J. Am. Chem. Soc. 1963, 85, 1715.
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26 Conclusions E D = 7.5 kJ mol -1 V 2 = 340 cm -1 ∆E = 0.66 GHz E D = 10.4 kJ mol -1 V 2 = 180 cm -1 ∆E = 3.41 GHz E D = 8.5 kJ mol -1 V 2 = 336 cm -1 ∆E = 0.82 GHz E D = 9.8 kJ mol -1 V 2 = 125 cm -1 ∆E = 5.39 GHz E D = 7.7 kJ mol -1 E D = 11.0 kJ mol -1
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27 Acknowledgement Prof. W. Caminati Dr. L. B. FaveroDr. A. MarisDr. L. Evangelisti Ms. C. Calabrese Dr. F. Gang Prof. S. Melandri Thanks for attention ! attention ! Mr. L. Spada
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