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From the Bottom Up: Hydrogen Bonding in Ionic Liquids 6/19/2014 Olga Gorlova, Conrad Wolke, Joseph Fournier, Christopher Johnson and Mark Johnson
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Ionic Liquids Purely Ionic Salt Like Notably low vapor pressures + + + + + + + + + - - - - - - - - - o Large & Asymmetric Cation (EMIM + ) m (BF 4 ¯) n (EMIM + ) m (Cl¯) n (EMIM + ) m (Tf 2 N¯) n Liquids at Room Temperatures
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ESI Needle Temperature Controlled Ion Trap Mounted to He Cryostat Ion Optics 2m Flight Tube Wiley- McLaren TOF Reflectron DC-Turning Quad MCP Detector Differential Aperture Skimmers Heated Capillary RF-Ion Guides Experimental Setup hv = 600-4300 cm -1 Collisional cooling in 3D Paul Trap -Pulsed He and N 2 gas Pulsed Valve Ions inIons out Paul Trap 10 K RF Cryogenic Ion Trap
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ESI Needle Temperature Controlled Ion Trap Mounted to He Cryostat Ion Optics 2m Flight Tube Wiley- McLaren TOF Reflectron DC-Turning Quad MCP Detector Differential Aperture Skimmers Heated Capillary RF-Ion Guides Experimental Setup hv = 600-4300 cm -1 Room Temperature Ion Cold “Tagged” Ion Photofragment Absorption Evaporation
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1-Ethyl-3-methylimidazolium (EMIM + ) (BF 4 ¯) (EMIM + ) m (BF 4 ¯) n
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% Abs. 60080010001200140016002800300032003400 Photon Energy / cm -1 Bulk FT-IR (EMIM + ) (BF 4 ¯) Et/Me CH stretches Ring CH stretches
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% Abs. 60080010001200140016002800300032003400 Photon Energy / cm -1 Bulk FT-IR (EMIM + ) (BF 4 ¯) Et/Me stretches Ring CH ip bends Et/Me bends Ring CH stretches Ring stretches EMIM + (calc) Calc. Int. (EMIM + ) (BF 4 ¯) * 2 PEAKS? Red shift caused by H-bond?
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Pred. Yield % Abs. EMIM + 60080010001200140016002800300032003400 Photon Energy / cm -1 Bulk FT-IR Et/Me stretches Ring CH ip bends Et/Me bends Ring CH stretches Ring stretches EMIM + (calc) Calc. Int. * Isolated (EMIM + ) Spectrum Same Red Shifted Peak in Bare Ion * Anion Contribution ?
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Pred. Yield % Abs. ν3ν3 ν1ν1 11 BF 4 ‾ EMIM + 60080010001200140016002800300032003400 Photon Energy / cm -1 Bulk FT-IR Et/Me stretches Ring CH ip bends Et/Me bends Ring CH stretches Ring stretches EMIM + (calc) Calc. Int. * * Low Energy Band Broadened asymmetric B-F stretch C.J. Johnson, et. al, J. Chem. Phys. 139, 224305 (2013)
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Pred. Yield % Abs. ν3ν3 ν1ν1 11 BF 4 ‾ EMIM + 60080010001200140016002800300032003400 Photon Energy / cm -1 (2,1) Bulk FT-IR Et/Me stretches Ring CH ip bends Et/Me bends Ring CH stretches EMIM + (calc) Calc. Int. (EMIM + ) 2 (BF 4 ¯) Spectral response to assembly? C.J. Johnson, et. al, J. Chem. Phys. 139, 224305 (2013)
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Deuteration Isolate the C (2) H 8001000120014001600240026002800300032003400 Photon Energy / cm -1 C (2) D ip bend C (2) D Pred. Yield Ring CH ip bends Et/Me bends Ring stretches Et/Me stretches Ring CH stretches
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[d (2) -EMIM][BF 4 ] bulk Predissociation Yield Photon Energy / cm -1 d (2) -EMIM + d (2) -(2,1) EMIM + (2,1) Bare C (4,5) H stretches Bare C (4,5) H stretches C (2) D stretch 220024002800300032002300290031003300 (EMIM + ) 2 (BF 4 ¯) Deuterated Et/Me stretches Ring CH stretches -4 -10 C.J. Johnson, et. al, J. Chem. Phys. 139, 224305 (2013)
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Forcing the Hydrogen Bond Cl¯ Should strengthen the cation-anion interaction Still a spherical anion Will simplify the problem
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8001000120014001600280030003200 Predissociation Yield Photon Energy (cm -1 ) Hydrogen Bonding x5 (EMIM + ) (EMIM + ) 2 (BF 4 ¯) (EMIM + ) 2 (Cl¯) Ring CH ip bends Et/Me bends Ring stretches Et/Me stretches Ring CH stretches
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800120016002000240028003200 Photon Energy (cm -1 ) Predissociation Yield ν C(2)D ν C(2)H (2,1) (1,0) x5 (EMIM + ) 2 (Cl¯) Deuterated
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Ionic Liquids BF 4 ¯ Anion Effects Tf 2 N¯ Cl¯
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Ring CH ip bends 80010001200140016002800300032003400 N-shuttle C-F/C-S stretch S-O stretch Et/Me bends Ring Stretches Et/Me stretches Ring CH Stretches (1,0) (0,1) (1,2) (EMIM + ) 1 (Tf 2 N¯) 2 Predissociation Yield Photon Energy (cm -1 )
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Predissociation Yield 2000220024002600280030003200 Photon Energy (cm -1 ) H-Bonding 2360 - 223 (EMIM + ) (Cl¯) 2 (EMIM + ) (Tf 2 N¯) 2 ~0 Is it Hydrogen Bonding? Deuterated Spectra
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Conclusions A true hydrogen bond can be observed with the Cl¯, while Tf 2 N¯ and BF 4 ¯ have minimal hydrogen bonding character. Deuteration serves to isolate the acidic H- bonding position from other C-H stretches and Fermi resonances to better study the nature of the hydrogen bonding at the acidic position.
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Acknowledgements Conrad Wolke Joseph Fournier Chris Johnson Patrick Kelleher Steph Craig Gary Weddle Mark Johnson RG07 – Protonated Water Clusters
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Pred. Yield % Abs. ν3ν3 ν1ν1 11 BF 4 ‾ EMIM + (2,1) 60080010001200140016002800300032003400 Photon Energy / cm -1 (1,2) x10 x5 * 10 BF 4 ‾ Bulk FT-IR Et/Me stretches Ring CH ip bends Et/Me bends Ring CH stretches Ring stretches 2x Ring stretches (EMIM + ) m (BF 4 ¯) n
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8001000120014001600280030003200 Predissociation Yield Photon Energy (cm -1 ) (2,1) (1,2) (1,0) (EMIM + ) m (Cl¯) n
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800120016002000240028003200 Photon Energy (cm -1 ) Predissociation Yield δ C(2)D δ C(2)H ν C(2)D (2,1) (1,2) (1,0) x5 (EMIM + ) m (Cl¯) n Deuterated
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Predissociation Yield 2000220024002600280030003200 Photon Energy (cm -1 ) H-Bonding 2360 - 49 - 223 (EMIM) (EMIM + ) (BF 4 ¯) 2 (EMIM + ) (Cl¯) 2 (EMIM) (Tf 2 N¯) 2 2360 Hydrogen Bonding
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