THE MICROWAVE SPECTRUM AND UNEXPECTED STRUCTURE OF THE BIMOLECULAR COMPLEX FORMED BETWEEN ACETYLENE AND (Z)-1-CHLORO-2-FLUOROETHYLENE Nazir D. Khan, Helen.

Slides:



Advertisements
Similar presentations
CHIRPED-PULSE FOURIER-TRANSFORM MICROWAVE SPECTROSCOPY OF THE PROTOTYPICAL C-H…π INTERACTION: THE BENZENE…ACETYLENE WEAKLY BOUND DIMER Nathan W. Ulrich,
Advertisements

Spectra, Structures, and Dynamics of Weakly Bound Clusters from Dimers to Nonamers Wolfgang Jäger Department of Chemistry, University of Alberta.
Galen Sedo, Jamie L. Doran, Shenghai Wu, Kenneth R. Leopold Department of Chemistry, University of Minnesota A Microwave Determination of the Barrier to.
Rotational Spectra of Methylene Cyclobutane and Argon-Methylene Cyclobutane Wei Lin, Jovan Gayle Wallace Pringle, Stewart E. Novick Department of Chemistry.
Chirality of and gear motion in isopropyl methyl sulfide: Fourier transform microwave study Yoshiyuki Kawashima, Keisuke Sakieda, and Eizi Hirota* Kanagawa.
The inversion motion in the Ne – NH 3 van der Waals dimer studied via microwave spectroscopy Laura E. Downie, Julie M. Michaud and Wolfgang Jäger Department.
Observation of the weakly bound (HCl) 2 H 2 O cluster by chirped-pulse FTMW spectroscopy Zbigniew Kisiel, a Alberto Lesarri, b Justin Neill, c Matt Muckle,
FOURIER TRANSFORM MICROWAVE SPECTROSCOPY OF ALKALI METAL HYDROSULFIDES: DETECTION OF KSH P. M. SHERIDAN, M. K. L. BINNS, J. P. YOUNG Department of Chemistry.
Microwave Spectroscopic Investigations of the C—H…  Containing Complexes CH 2 F 2 …Propyne and CH 2 ClF…Propyne Rebecca A. Peebles, Sean A. Peebles, Cori.
Microwave Spectra and Structures of H 2 S-CuCl and H 2 O-CuCl Nicholas R. Walker, Felicity J. Roberts, Susanna L. Stephens, David Wheatley, Anthony C.
Rotational Spectra and Structure of Phenylacetylene-Water Complex and Phenylacetylene-H 2 S (preliminary) Mausumi Goswami, L. Narasimhan, S. T. Manju and.
Electronic Spectroscopy of DHPH Revisited: Potential Energy Surfaces along Different Low Frequency Coordinates Leonardo Alvarez-Valtierra and David W.
Microwave Spectrum and Molecular Structure of the Argon-(E )-1-Chloro-1,2-Difluoroethylene Complex Mark D. Marshall, Helen O. Leung, Hannah Tandon, Joseph.
†) Currently at Department of Chemistry, University of Manitoba A Microwave Study of the HNO 3 -N(CH 3 ) 3 Complex Galen Sedo, † Kenneth R. Leopold Department.
The Pure Rotational Spectrum of Pivaloyl Chloride, (CH 3 ) 3 CCOCl, between 800 and MHz. Garry S. Grubbs II, Christopher T. Dewberry, Kerry C. Etchison,
Rotationally-Resolved Spectroscopy of the Bending Modes of Deuterated Water Dimer JACOB T. STEWART AND BENJAMIN J. MCCALL DEPARTMENT OF CHEMISTRY, UNIVERSITY.
Fourier transform microwave spectra of CO–dimethyl sulfide and CO–ethylene sulfide Akinori Sato, Yoshiyuki Kawashima and Eizi Hirota * The Graduate University.
THE ANALYSIS OF HIGH RESOLUTION SPECTRA OF ASYMMETRICALLY DEUTERATED METHOXY RADICALS CH 2 DO AND CHD 2 O (RI09) MING-WEI CHEN 1, JINJUN LIU 2, DMITRY.
Ab Initio and Experimental Studies of the E Internal Rotor State of He-CH 3 F Kelly J. Higgins, Zhenhong Yu, and William Klemperer, Department of Chemistry.
THE MICROWAVE STUDIES OF GUAIACOL (2-METHOXYPHENOL), ITS ISOTOPOLOGUES & VAN DER WAALS COMPLEXES Ranil M. Gurusinghe, Ashley Fox and Michael J. Tubergen,
Effective C 2v Symmetry in the Dimethyl Ether–Acetylene Dimer Sean A. Peebles, Josh J. Newby, Michal M. Serafin, and Rebecca A. Peebles Department of Chemistry,
Rotational Spectra Of Cyclopropylmethyl Germane And Cyclopropylmethyl Silane: Dipole Moment And Barrier To Methyl Group Rotation Rebecca A. Peebles, Sean.
Intermolecular Interactions between Formaldehyde and Dimethyl Ether and between Formaldehyde and Dimethyl Sulfide in the Complex, Investigated by Fourier.
The rotational spectra of helium- pyridine and hydrogen molecule- pyridine clusters Chakree Tanjaroon and Wolfgang Jäger.
The rotational spectrum of acrylonitrile to 1.67 THz Zbigniew Kisiel, Lech Pszczółkowski Institute of Physics, Polish Academy of Sciences Brian J. Drouin,
CHIRPED PULSE AND CAVITY FOURIER TRANSFORM MICROWAVE (CP-FTMW AND FTMW) SPECTRUM OF BROMOPERFLUOROACETONE NICHOLAS FORCE, DAVID JOSEPH GILLCRIST, CASSANDRA.
S TRUCTURE D ETERMINATION AND CH···F I NTERACTIONS IN H 2 C=CHF···H 2 C=CF 2 B Y F OURIER - T RANSFORM M ICROWAVE S PECTROSCOPY Rachel E. Dorris, Rebecca.
Rotational Spectroscopic Investigations Of CH 4 ---H 2 S Complex Aiswarya Lakshmi P. and E. Arunan Inorganic and Physical Chemistry Indian Institute of.
Broadband Microwave Spectroscopy to Study the Structure of Odorant Molecules and of Complexes in the Gas Phase Sabrina Zinn, Chris Medcraft, Thomas Betz,
Helen O. Leung, Mark D. Marshall & Joseph P. Messenger Department of Chemistry Amherst College Supported by the National Science Foundation.
CHIRPED PULSE AND CAVITY FT MICROWAVE SPECTROSCOPY OF THE HCOOH – N(CH 3 ) 3 WEAKLY BOUND COMPLEX Rebecca B. Mackenzie, Christopher T. Dewberry, and Kenneth.
Chirped-Pulse Microwave Spectroscopy in the Undergraduate Chemistry Curriculum Sydney Gaster, Taylor Hall, Sean Arnold, Deondre Parks, Gordon Brown Department.
Microwave and Ab Initio Investigations of CHCl 2 F-OCS and Related Hydrochlorofluorocarbon Complexes Rebecca A. Peebles and Amanda L. Steber Department.
The Rotational Spectrum of the Water–Hydroperoxy Radical (H 2 O–HO 2 ) Complex Kohsuke Suma, Yoshihiro Sumiyoshi, and Yasuki Endo Department of Basic Science,
Microwave Spectroscopic Investigations of the Xe-H 2 O and Xe-(H 2 O) 2 van der Waals Complexes Qing Wen and Wolfgang Jäger Department of Chemistry, University.
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.
Rotational Spectra of N 2 O-H 2 Complexes University of Alberta Jen Nicole Landry and Wolfgang Jäger June 23, 2005.
Fourier-transform microwave spectroscopy of the CCCCl radical Takashi Yoshikawa, Yoshihiro Sumiyoshi, and Yasuki Endo Graduate School of Arts and Sciences,
Rotational spectra of C2D4-H2S, C2D4-D2S, C2D4-HDS and 13CH2CH2-H2S complexes: Molecular symmetry group analysis Mausumi Goswami and E. Arunan Inorganic.
Rebecca A. Peebles,a Prashansa B. Kannangara,a Brooks H
Rebecca A. Peebles,a Prashansa B. Kannangara,a Brooks H
Analysis of bands of the 405 nm electronic transition of C3Ar
Department of Chemistry
Mark D. Marshall, Helen O. Leung, Craig J. Nelson & Leonard H. Yoon
Microwave Spectra and Structures of H4C2CuCl and H4C2AgCl
Carlos Cabezas and Yasuki Endo
A.J. Barclay, S. Sheybani-Deloui, N. Moazzen-Ahmadi
V. Ilyushin1, I. Armieieva1, O. Zakharenko2, H. S. P. Müller2, F
G. S. Grubbs II*, S. A. Cooke⧧, and Stewart E. Novick*,
The CP-FTMW Spectrum of Bromoperfluoroacetone
Aimee Bell, Omar Mahassneh, James Singer,
M. Rezaei, J. George, L. Welbanks, and N. Moazzen-Ahmadi
3-Dimensional Intermolecular Potential Energy Surface of Ar-SH(2Pi)
Daniel Zaleski,a John Mullaney,a Nicholas Walkera and Anthony Legonb
Becca Mackenzie Chris Dewberry, Ken Leopold
The Effect of Protic Acid Identity on the Structures of Complexes with Vinyl Chloride: Fourier Transform Microwave Spectroscopy and Molecular Structure.
CHIRPED-PULSE FOURIER TRANSFORM MICROWAVE SPECTROSCOPY OF
Department of Chemistry
Analysis of the Rotationally Resolved Spectra to the Degenerate (
Mahdi Kamaee and Jennifer van Wijngaarden
Fourier transform microwave spectra of n-butanol and isobutanol
MICROWAVE SPECTRA FOR THE THREE 13C1 ISOTOPOLOGUES OF PROPENE AND NEW ROTATIONAL CONSTANTS FOR PROPENE AND ITS 13C1 ISOTOPOLOGUES NORMAN C. CRAIG, Department.
Ashley M. Anderton, Cori L. Christenholz, Rachel E. Dorris, Rebecca A
Fourier Transform Emission Spectroscopy of CoH and CoD
The rotational spectrum of the urea isocyanic acid complex
Fourier Transform Infrared Spectral
BROADBAND MICROWAVE SPECTROSCOPY AS A TOOL TO STUDY DISPERSION INTERACTIONS IN CAMPHOR-ALCOHOL SYSTEMS MARIYAM FATIMA, CRISTÓBAL PÉREZ, MELANIE SCHNELL,
Wei Lin, Anan Wu, Zin Lu, Daniel A. Obenchain, Stewart E. Novick
Michal M. Serafin, Sean A. Peebles
Daniel A. Obenchain, Derek S. Frank, Stewart E. Novick,
Presentation transcript:

THE MICROWAVE SPECTRUM AND UNEXPECTED STRUCTURE OF THE BIMOLECULAR COMPLEX FORMED BETWEEN ACETYLENE AND (Z)-1-CHLORO-2-FLUOROETHYLENE Nazir D. Khan, Helen O. Leung & Mark D. Marshall Department of Chemistry Amherst College Supported by the National Science Foundation

Leung, Marshall, Amberger, Fluoroethylene---HF Complexes 18.7(15)o 21.65o 29.99o 2.734 Å 1.892(14) Å 2.60952(14) Å 1.910297(68) Å 2.7825(3) Å 1.98833(44) Å Cole & Legon, CPL 400, 419 (2004) Leung, Marshall, Amberger, JCP 131, 204302 (2009) Leung & Marshall et. al, JCP 131, 204301 (2009) 2.7522(40) Å An increase in the number of F substituents has significant effects on the nature of intermolecular interactions. 41.6(51)o 2.020(41) Å Leung & Marshall, JCP 126, 114310 (2007)

1, 1-Difluoroethylene---HX Complexes 3.0762(3) Å 2.3309(4) Å 122.41o 34.22o Kisiel, Fowler, Legon, J. Chem. Soc., Faraday Trans. 88, 3385 (1992) 1.9883(4) Å 2.7825(3) Å 29.99o Leung, Marshall, Drake, Pudlik, Savji, McCune, J. Chem. Phys. 131, 204301 (2009) 2.65(1) Å 3.01(2) Å 122.4(8)o 53.3(2)o Leung, Marshall, J. Chem. Phys. 125, 154301 (2006) H C C F H H Cl H

A Different Structure for the 1, 1, 2-Trifluoroethylene---HF Complex 2.60952(14) Å 1.910297(68) Å 21.65o Leung, Marshall, Amberger, JCP 131, 204302 (2009) 41.6(51)o 2.7522(40) Å 2.020(41) Å Leung & Marshall, JCP 126, 114310 (2007) 122.41o 109.0o “Top binding” “Side binding” Top binding is sterically more favorable, and side binding is electrostatically more favorable.

1,1,2-Trifluoroethylene---HX Complexes 2.8694(9) Å 104.5(2)o 2.75(2) Å 69.2(7)o H C 2.02(4) Å 2.752(4) Å 109(1)o 42(5)o C F H H Leung, Marshall, J. Chem. Phys. 126, 114310 (2007) Leung, Marshall, Cashion, Chen, J. Chem. Phys. 128, 064315 (2008) 2.3416(7) Å 3.0796(5) Å 109.72(4)o 47.73(1)o Cl H Leung, Marshall, Ray, Kang, J. Phys. Chem. 114, 10975 (2010)

Effects of Chlorine Substitution: Chlorofluoroethylenes and chloroethylenes What is the effect of substituting chlorine atoms for fluorine atoms in various fluoroethylenes? Chlorine is less electronegative than fluorine Chlorine is more polarizable Acids were expected to preferentially bind to fluorine in chlorofluoroethylenes The primary interaction was expected to be weakened less by additional chlorine substitution than additional fluorine substitution

Chlorofluoroethylene---HF Complexes 1.9482(10) Å 124.371(70)o 2.7386(19) Å 29.14o 24.93(1)o F F H H 2.4535(2) Å 1.9445(2) Å HF preferentially binds to fluorine over chlorine in chlorofluoroethylenes 118.635o F F H H H H Cl Cl 2.7574(12) Å Leung, Marshall, Bozzi, Cohen, Lam, J. Mol. Spectrosc. 267, 43 (2010) F F Leung, Marshall, Lee, In preparation H 41.5(24)o 109.20(61)o F 2.020(18) Å H Cl Leung, Marshall, Bozzi, In preparation

Vinyl Chloride---HX Complexes 2.319(6) Å 2.59(1) Å 19.8(3)o 102.4(2)o 3.02(1) Å 88.6(2)o 58.5(6)o 2.93(1) Å F H Cl Cl H Cl C H C 2.409 Å 3.386 Å H Leung, Marshall, J. Phys. Chem. 118, 9783 (2014) Leung, Marshall, Bozzi, Cohen, Lam, J. Phys. Chem. 117, 13419 (2013) Cl Acid identity determines the structure of the vinyl chloride---HX complex Minimum energy structure predicted by ab initio calculations for the vinyl chloride---HCl dimer

(Z)-1-Chloro-2-fluoroethylene---HCCH Complex How does HCCH bind to (Z)-1-chloro-2-fluoroethylene? How do the geometric parameters compare to previous results? ?

Ab Initio Calculations 2.57958 Å 2.89827 Å 61.44o 104.33o Fluorine bound minimum 3.04148 Å 2.77504 Å 61.74o 85.67o Chlorine bound minimum θZE r θHCCH A = 11551.2790012 MHz B = 806.4824631 MHz C = 753.8504419 MHz 75 cm-1 A = 4768.7499746 MHz B = 1086.3100008 MHz C = 884.7630614 MHz 0 cm-1

Chirped-Pulse FTMW Spectroscopy Studied in the 5.5-18.1 GHz region 1% CHFCHCl, 1% HCCH in Ar at ~2 atm backing pressure Two isotopologues CHFCH35Cl---HCCH CHFCH37Cl---HCCH Nozzle is mounted perpendicular to microwave horns CHFCH35Cl---HCCH 313-202 Ar---CHFCH35Cl * CHFCH37Cl

Balle-Flygare FTMW Spectroscopy Studied in the 5.5-20.7 GHz region 1% CHFCHCl, 1% HCCH in Ar at ~2 atm backing pressure Six isotopologues CHFCH35Cl---HCCH, CHFCH37Cl---HCCH, CHFCH35Cl---H13C13CH, CHFCH37Cl---H13C13CH, CHFCH35Cl---H13CCH, 13CHFCH35Cl---HCCH Nozzle is mounted parallel to mirror axis, leading to Doppler doubling in each transition.

Representative Transition CHFCH35Cl---HCCH 313-202 F’ = 4.5 F” = 3.5 F’ = 1.5 F” = 1.5

(Z)-1-chloro-2-fluoroethylene---HCCH Transitions CHFCH35Cl---HCCH CHFCH37Cl---HCCH CHFCH35Cl---H13C13CH CHFCH37Cl---H13C13CH 13CHFCH35Cl---HCCH CHFCH35Cl---H13CCH Total # of transitions 101 104 88 76 6 7 # of a-type transitions 43 50 42 36 2 3 # of b-type transitions 58 54 46 40 4 Hyperfine components 587 533 476 372 16 21 J range 0-10 2-5 Ka range 0-4 0-3 0-1

Spectroscopic Constants (MHz) CHFCH35Cl---HCCH A 4885.649238(85) B 1057.174079(35) C 869.413173(32) ΔJ / 10-3 1.16322(23) ΔK / 10-3 0.0698551(82) ΔJK / 10-3 -0.8450(19) δJ / 10-3 0.25182(11) δK / 10-3 5.2715(12) χaa 39.83616(66) χbb -72.66307(83) χcc 32.82691(79) RMS 0.0018 Fluorine bound minimum A = 11551.2790012 MHz B = 806.4824631 MHz C = 753.8504419 MHz Chlorine bound minimum A = 4768.7499746 MHz B = 1086.3100008 MHz C = 884.7630614 MHz

Spectroscopic Constants (MHz) CHFCH37Cl---HCCH CHFCH35Cl---H13C13CH CHFCH37Cl---H13C13CH 13CHFCH35Cl---HCCH CHFCH35Cl---H13CCH A 4742.466963(66) 4844.133202(90) 4702.44029(10) 4822.9290(22) 4884.4318(18) B 1056.557011(24) 1009.347222(33) 1008.547251(52) 1052.27636(25) 1036.10835(23) C 864.330032(19) 835.57850(28) 830.692854(51) 864.10321(52) 855.08513(48) ΔJ / 10-3 1.15635(14) 1.07935(20) 1.07266(31) 1.1435(81) 1.1037(75) ΔK / 10-3 0.0656266(74) 0.068095(10) 0.063931(12) 0.0698551* ΔJK / 10-3 -0.5415(11) -0.8361(19) -0.5245(36) -0.8450* δJ / 10-3 0.254928(63) 0.22626(10) 0.22909(14) 0.25182* δK / 10-3 5.1913(60) 4.987(11) 4.920(21) 5.2715* χaa 31.40535(60) 39.85329(72) 31.41743(96) 39.819(20) 39.843(16) χbb -57.27402(70) -72.67854(85) -57.2854(10) -72.658(16) -72.6720(58) χcc 25.86868(62) 32.82525(75) 25.86795(96) 32.8387(71) 32.829(12) RMS 0.0014 0.0016 0.0017 0.0018 0.0015

Some Observations κ ranges from -0.92 – -0.90 Δ ranges from -0.21 – -0.18 amu·Å2 typical of a planar molecule in which out-of-plane vibrational contribution is dominant The rotational constants of 3 singly substituted isotopologues are used to locate the positions of 3 atoms.

Substitution Structure CHFCHCl--- HCCH |a|/Å 0.3758(40) 1.4935(10) 3.12697(48) |b|/Å 1.2627(12) 1.1668(13) 0.1631(92) + + - ± + - ± b Cl C C a C C C

Fit to Moments of Inertia Three geometric parameters are required to describe the structure of the complex Fit parameters to Ia and Ic of each of the six isotopologues, assuming the structures of CHFCHCl and HCCH remain unchanged upon complexation. a b 3.076(21) Å 2.8644(23) Å 87.54(34)o Cl C H F 62.4(12)o

Chlorine Quadrupolar Coupling Assuming no efg perturbation upon complexation, one of the principal efg axes should lie more or less along the C-Cl bond. Angle between C-Cl bond and a axis From χ tensor of CHFCH35Cl---HCCH 91.95o From fit to inertial data 89.61o

Chloroethylene---HCCH Complexes 3.076(21) Å 2.8644(23) Å 62.4(12)o 3.02(1) Å 88.6(2)o 58.5(6)o 2.93(1) Å Experimental structures 2.9854 Å 86.50o 57.84o 2.8339 Å 3.0415 Å 2.7750 Å 61.74o 85.67o Ab initio minimum energy structures

Chlorofluoroethylene---HCCH Complexes 3.076(21) Å 2.8644(23) Å 62.4(12)o 124.30(70)o 2.623(11) Å 52.82(28)o 2.977(17) Å HCCH binds to chlorine when only side binding is allowed HCCH binds to fluorine when only top binding is allowed

(Z)-1-Chloro-2-fluoroethylene---HX Complexes 3.076(21) Å 2.8644(23) Å 62.4(12)o 2.88560 Å 1.89650 Å 26.00o 109.99o Red: Most negative electric potential Blue: Most positive electric potential Minimum energy structure predicted by ab initio calculations for the dimer with HF Experimental structure of the dimer with HCCH

Summary The rotational spectra of six isotopologues of (Z)-1-chloro-2-fluoroethylene---HCCH have been observed and analyzed. HCCH interacts with the Cl and H atoms at one end of the double bond instead of the F and H atoms at the other end of the double bond. This bonding motif is different from that observed in all other chlorofluoroethylene---HX dimers. The different binding modes can be explained by different steric requirements for F and Cl in the chlorofluoroethylene dimers

Acknowledgements National Science Foundation for providing funding Thank you