cynthia j. jameson - stem womenstemwomen.org/talks/rppt29.pdf · cynthia j. jameson university of...
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The temperature dependence of chemical shifts: mechanisms and contributions
Cynthia J. Jameson University of Illinois at Chicago
19F NMR
T→
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outline• the intramolecular shielding surface• temperature dependence of the average chemical
shift in an “isolated” diatomic molecule• in an “isolated” polyatomic molecule• temperature dependence of intermolecular chemical
shifts in a constant volume homogeneous system• temperature dependence of intermolecular chemical
shifts in a constant pressure homogeneous system; the major contribution from expansion of the solvent
• temperature dependence in heterogeneous systems: one Xe in a cage; n Xe in a cage
• Xe in a channel; the major contribution from temperature dependence of the adsorption isotherm
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I. the intramolecular shielding surface
for H2+ molecule
the shielding functionis known all the way from the value 8.875 ppm at infiniteseparation through the 11.4296 ppm at the equilibriumgeometry, and 35.5009ppm for the united one-electron atom, He+. R. A. Hegstrom, Phys. Rev. A 19, 17-30 (1979)
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H2+ vibrational wavefunctions
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vibrational averaging occurs around the equilibrium bond distance
• For a given v,J state, the averaging weights the extended bond values of shielding more than the compressed bond values of shielding because of
(a) anharmonicity of the vibration(b) centrifugal stretching
That is, the average bond length is longer than the equilibrium bond length, becoming more pronounced at higher v levels.
• Going to higher temperatures weights the higher vibrational levels more, thus shifting further away from the shielding value at the equilibrium bond length.
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the temperature coefficient of the chemical shift
• sign will depend on the sign of the derivative of the shielding function at the equilibrium geometry
• magnitude will depend on the magnitude of the derivative of the shielding function at the equilibrium geometry and the anharmonicity of the vibration
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in the vicinity of the equilibrium geometry
proton becomes less shieldedwith increasing bond length 23Na becomes more shielded
with increasing bond length
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shielding changes in the vicinity of the equilibrium geometry
HF, HCl, LiH, NaH, F2, ClFscaling permits direct comparison of F with Cl, Li with Na,
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compare shielding derivatives across the Periodic Table
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scaling places first and second row on same graphgreater shieldingwith bond stretchleads to decreasingchemical shift withincreasing T
less shieldingwith bond stretchleads to increasingchemical shift withincreasing T
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sign of chemical shift with lighter atomsubstitution is same as with increasing temperature, both correspond to greater average bond lengths
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II. T dependence of chemical shift in an isolated diatomic molecule
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13C in isolated CO molecule
increasing chemical shift with increasing T
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15N in isolated N2 molecule
increasing chemical shift with increasing T
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diatomic molecule rovibl averaging
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III. an isolated polyatomic molecule• experimental observations in samples of
various known densities, followed by extrapolation to zero density finds a temperature dependence that is intrinsic to an isolated molecule
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15N in isolated NNO molecule
increasing chemical shift with increasing T
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15N in NH3, 31P in PH3 and PF3isolated molecules
increasing chemical shift with increasing T
decreasing chemical shift with increasing T
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31P in isolated moleculesdecreasing chemical shift with increasing T
increasing chemical shift with increasing T
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Temperature dependence of 19F
increasing chemical shift with increasing T
fluoroalkanes
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19F in isolated molecules
increasing chemical shift with increasing T
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Temperature dependence of 19F
increasing chemical shift with increasing T
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various nuclei in isolated molecules
increasing chemical shift with increasing T
but not for31P in PH3
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quantum mechanical calculations of shielding surfaces in polyatomic molecules• NH3, PH3
• CH4, OH2
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15N shielding surface in NH3molecule
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15N and 31P shielding function of the inversion coordinate in NH3 and PH3
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shielding surfaces for 13C in CH4, 17O in H2O compared with 15N in NH3 and 31P in PH3
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dynamic averages in polyatomic molecules
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the inversion potential and its wavefunctions for NH3
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calculated T dependence of 15N shielding in NH3
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calculated T dependence of 15N shielding in NH3 and ND3
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calculated temperature dependence for 15N, 13C, 31P, 17O
decreasing chemical shift with increasing T
for “central” atoms the Tdependenceis not simpleto calculate
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approximate analysis of 19F temperature dependence
for nuclei of any terminal atom in a molecule,there is one dominant bond stretch term and the angle deformation terms are less important
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can estimate ⟨Δr⟩vibfrom position of two atoms in the Periodic Table usingHerschbach and Laurieparameters
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calculated temperature dependence of 19F using one parameter fit to isolated molecule data
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When system is not an isolated molecule, temperature dependence of intermolecular interactions come into play.
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IV. intermolecular shifts in a constant volume homogeneous system • In a sealed sample of fluid above the
critical point or at T,p above the liquid-vapor equilibrium curve: the temperature dependence of the chemical shift comes entirely from that in the isolated molecule plus that due to the virial expansion of the shielding.
σ(T,ρ)=σ0(T) + σ1 (T)ρ + σ2 (T)ρ2 +…(see ‘Intermolecular Chemical Shifts’ for details)
(usually) increasing chemical shift with increasing density
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density coefficient of the 129Xe chemical shift, the secondvirial coefficient of shielding, σ1(T)
Jameson et al. J. Chem. Phys. 59, 4540-4546 (1973).
the magnitude of the density coefficient decreases with increasing temperature.
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density coefficient of the 129Xe chemical shift in various gases
Jameson et al. J. Chem. Phys. 65, 3401-3406 (1976);J. Chem. Phys. 66, 5226-5230 (1977).
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V. intermolecular shifts in a constant pressure homogeneous system
the major contribution from expansion of the liquidδ(T,ρ) ≈ δ0(T) + δ1eff(T) ρLIQ(T) + …where ρLIQ is the number density of molecules in the liquid and δ1eff(T) is the density coefficient of the chemical shift in cases where a linear dependence on density is observed.
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19F σ(T,ρ)-σ0(T) ≈ σ1eff(T) ρLIQ(T) +…
critical point
increasing chemical shift with increasing density
nearly linear dependence on density of liquid, butsmaller slope
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from gas to liquid shifts: σ(T,ρ)- σ0(T) ≈ σ1eff(T) ρLIQ(T) +…
incr
easi
ng c
hem
ical
shi
ft
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n-pentane : n-hexane :
Xe chemical shift temperature dependence in solution
Molecular Dynamics simulations resultsJ. Phys. Chem. C, 111, 15771-15783 (2007).
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T dependence of the solvent densityis responsiblefor most of the observed steep T dependence of Xe chemical shifts in solution.The remainder is from T dependent Xe Interactions with alkane, δ1(T)
divide out the densityto get δ1effjust as in
pure liquids
Contributions to the temperature dependence of Xe chemical shifts in solution
pentane
hexane
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VI. intermolecular shifts in heterogeneous systems: one in a cage, n in a cage• one Xe in a cage: governed by probability
distribution functions changing with temperature• compare with one Xe in a flexible cage governed
by (a) probability distribution functions changing with temperature, and (b) dynamics of cage atoms changing with temperature
• n Xe in a cage governed by (a) one-body probability distribution functions changing with temperature, and (b) two-body distribution functions changing with temperature
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first consider one Xe in a cage, no Xe-Xe interactions
• What is the expected temperature dependence of the chemical shift?
• This depends on the size of the cage relative to the diameter of the Xe atom
• in a small cage, the potential energy surface for the Xe is lowest in the center
• in a larger cage, there are potential energy minima for the Xe at points ~ 4 Å to the wall, less favorable at the center
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smaller probability near center of cagewhere chemical shift is lower
With increase in temperature, probability density spreads out, including more of central regionwhere chemical shift is lower
Let us take a look atpoints on this plane
on this plane, where isXe is likely to be found?
Xe in a rigid cage NaA
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Xe-cage contribution only. This intermolecular chemical shift decreases with increasing temperature
at higher T, Xe can explore regions of higher potential energy and smaller chemical shift
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GCMC simulationsJameson and Kostikin, 2001
Xe in zeolite NaY
EXPERIMENT
Temperature dependence of 129Xe chemical shift at near-zero loading
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At low temperatures, Xe spends most of its time in the low potential energy regions next to the walls of the large cages, which correspond to higher chemical shifts. As temperature increases, the Xeprobability density spreads out over more regions farther away from the walls, whichcorrespond to lower chemical shifts.This is the same trend as for one Xe in NaA cage
Xe at near zero loading in NaY
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Xe in a small flexible cage
two contributions: • Xe probability distribution within the cage
changes with T• cage deformation (away from nearly spherical)
is more pronounced at higher T, leads tocloser Xe interactions with wall atoms
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One-body distribution function for Xe@cryptoAfrom Monte Carlo simulations
Unlike Xe in the larger NaA cage, for Xe in this smaller cage, the probability is highest in the center, and lower near the walls.
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Temperature dependence of Xe@cryptoAnot including cage deformation
68.94243
70.73260
69.62253
73.04273
75.31283
Our Monte Carlo SIMULATIONS
76.35293
78.77300
δ , ppmT, K
EXPERIMENTS from Bartik et al. 1998
Monte Carlo SIMULATIONSD. N. Sears and C. J. Jameson, 2003
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Xe-Xe chemical shift contributions
• with increasing number of Xe atoms in the same cage, Xe-Xe contributions increase, leading to higher chemical shifts
• for a fixed number of Xe atoms in the cage, temperature dependence is a combination of Xe-Xe contributions changing with T and Xe- wall contributions changing with T
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n Xe atoms in a rigid cageXe-Xe contributions dominate overXe-cagecontributionsat n large enough.
Xe-Xe interactionsexplore regionshigher up on repulsive Xe-Xepotential wall at higher T, these correspond to larger chemical shifts.
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VII. heterogeneous systems: changing occupancy in a channel
dominated by changes in adsorption isotherm with increasing temperature, that is, Xe occupancy changes markedly with temperature
J.A. Ripmeester, C. I. RatcliffeAnal. chim. Acta283, 1103 (1993)
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maximum Xeoccupancyis reached
increasing Xe occupancy as T decreases
For a sealed sample of Xe in NaY, steep increase in Xechemical shift from increasing Xe-Xe contributions
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single crystal experimentsA. Comotti, S. Bracco,L. Ferretti, M. Mauri, R. Simonutti and P. Sozzani Chem Commun 2007, 350-352
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A. Comotti, S. Bracco, L. Ferretti, M. Mauri, R. Simonutti and P. SozzaniChem. Commun.2007, 350-352
δ⊥ increasesXe-Xecontributionsincrease with increasing Xeoccupancyas T decreases
continuous flow
HP 129XeNMR
δ || not dependent on Xe loading
increases with increasing T.This has to dowith theconstrictionsin the channel
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observe temperature dependence at fixed Xe occupancy
• Xe in NaY at full occupancy• Xe in silicalite at full occupancy
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maximum Xeoccupancyis reached
increasing Xe occupancy as T decreases
Xe in NaY at full occupancy12 Xe per unit cell
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The anisotropic environment of silicalitegives rise to 3 unique tensor componentsprimarily arising from Xe-Xe contributions. Two of the components change dramatically with temperature, while the smallest component hardly changes. The changes in the Xe-Xe pair distribution function with temperature predicted by the Monte Carlo calculations reproduce the observed changes in line shape.
Xe at full loading(16 Xe per unit cell)in silicalite
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Temperature dependence with no change in ⟨N⟩Xe
EXPERIMENTS
150 K
300 K
J. A. Ripmeester et al.J. Am. Chem. Soc. 2001, 123, 10399
Jameson et al.J. Phys. Chem. B 1997, 101, 8418
CALCULATIONS
δ / ppm
160180200220240
150 K300 K
Jameson 2003
Xe line shapes at full occupancyare well reproduced by GCMC simulations
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ACKNOWLEDGMENTSGas phase shifts:Patricia M. BurrellSheila M. CohenAngel C. de DiosJila HonarbakhshA. Keith JamesonChun Luan LeeJames MoyerDaulat OppusungguHarriet ParkerKarla SchuettSteven Wille
Shielding surfaces:
Angel C. de DiosHyung-Mi LimDevin N. SearsLela Vukovic
Rovibrationalaveraging
Angel C. de DiosHans-Jörg Osten
Cages & channelsBernoli I. BaelloAngel C. de DiosRex E. Gerald IIA. Keith JamesonPavel KostikinHyung-Mi LimDevin N. SearsLela Vukovic
Solutions::Sohail MuradDevin N. SearsHuajun Yuan