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Supporting InformationOxidative Ionization Under Certain Negative-Ion Mass Spectrometric Conditions
Isra Hassan, Julius Pavlov, Ramu Errabelli and Athula B. Attygalle*
Table of Contents
Page no.List of Chemical Sources 5Supplementary Figure S1. a) Sample placement in an open HePI source on a Quattro
Ultima mass spectrometer; b) Sample placement and introduction of SF6 to a
closed HePI source on the same instrument. The original ESI source has the
same configuration, excepting that a methanolic solution of the sample is
sprayed through the capillary held at high voltage (instead of passing helium to
generate HePI plasma).
6
Supplementary Figure S2. Negative-ion HePI mass spectra acquired on a Waters
Micromass ZQ single-quadrupole mass spectrometer from background ambient
air at capillary voltage settings of (a) 4.0 kV , (b) 3.0 kV, (c) 2.5 kV, and (d)
1.8 kV. The peak intensities are normalized to the absolute intensity (in
arbitrary units) of the m/z 32 peak recorded at capillary voltage 4.0 kV.
7
Supplementary Figure S3. CID mass spectra acquired under ESI-MS conditions from
mass-isolated m/z 108 (a, b, c, and d), and m/z 109 (e, f, g, and h) ions,
generated from a methanolic solution of 1,4-hydroquinone, on a Waters
Micromass Quattro ultima triple quadrupole mass spectrometer. The CID
spectra of the m/z 108 ion were acquired at a capillary voltage 4.0 kV and at
laboratory-frame collision energies of (a) 10 eV, (b) 20 eV, (c) 30 eV, and (d)
8
1
40 eV, and those of the m/z 109 ion were acquired at a capillary voltage of 1.5
kV and at laboratory-frame collision energies of (e) 10 eV, (f) 20 eV, (g) 30
eV, and (h) 40 eV.
Supplementary Figure S4. Absolute intensity of m/z 108 (blue trace) and 109 (red
trace) ions, generated from a methanolic solution of 1,4-hydroquinone by ESI
at a capillary voltage of 3.20 kV, monitored against time by a selective ion
recording (SIR) experiment on a Waters Micromass Quattro Ultima triple
quadrupole mass spectrometer. After two minutes of signal acquisition, the
source was engulfed with sulfur hexafluoride, and at 7.5 min, the flow of SF6
was switched off. Insets show mass spectra corresponding to each region.
9
Supplementary Figure S5. Negative-ion nanospray ESI mass spectra recorded on a
Waters SYNAPT G2 Q-TOF mass spectrometer at different cone voltage
settings (10-80 V) from methanolic solutions of (a) catechol, (b) resorcinol,
and (c) hydroquinone. Other experimental conditions: flow rate 1 mL/min,
capillary voltage 4.0 kV, extraction cone voltage 3 V. Row 9 depicts typical
spectra recorded at a cone voltage setting of 20 V, from the same solutions and
under the same conditions after positioning the capillary tip closer to the
entrance cone to effect a plasma discharge.
10
Supplementary Figure S6. Negative-ion ESI mass spectra recorded on a Waters
SYNAPT G2 Q-TOF mass spectrometer of a) catechol , b) resorcinol and c)
hydroquinone (nanospray) under the following instrumental conditions:
extraction-cone voltage 1.5 V, sampling-cone voltage 20 V, Vernier probe
adjustment screw 5.92 mm, source temperature 100 oC, desolvation gas flow
rate 450 L/hr. The capillary voltage was varied between 1.4 and 4.0 kV.
11
Supplementary Figure S7. Negative-ion HePI mass spectra recorded on a Waters
Micromass Quattro Ultima triple quadrupole mass spectrometer from samples
12
2
of a) 2,3-dimethylbenzene-1,4-diol, b) 2,3,5-trimethylbenzene-1,4-diol, c) 2,5-
dihydroxybenzonitrile, d) 2,5-dihydroxybenzaldehyde, and e) 2,5-
dihydroxycyclohexa-2,5-diene-1,4-dione.
Supplementary Figure S8. Negative-ion HePI mass spectra recorded on a Waters
Micromass Quattro Ultima triple quadrupole mass spectrometer from samples
of a) 2,3-dihydroxybenzaldehyde, b) 3,4-dihydroxybenzaldehyde and c) 2,3-
dihydroxybenzonitrile.
13
Supplementary Figure S9. Negative-ion HePI mass spectra recorded on a Waters
Micromass Quattro Ultima triple quadrupole mass spectrometer from samples
of a) 2-methylbenzene-1,3-diol; b) 2,5-dimethylbenzene-1,3-diol; c) 2,6-
dihydroxybenzonitrile; d) 1-(2,6-dihydroxyphenyl)ethanone at a cone voltage
of 10 V, hexapole transfer 1 lens voltage of 20 V, source temperature of 150
oC, desolvation temperature of 300 oC and a capillary voltage of 3.2 kV.
14
Supplementary Figure S10. Negative-ion HePI mass spectra recorded on a Waters
Micromass Quattro Ultima triple quadrupole mass spectrometer from samples
of a) 5-methylbenzene-1,3-diol; b) 1-(2,4-dihydroxyphenyl)ethanone; c) (2,4-
dihydroxyphenyl)(phenyl)methanone; d) 1-(2,4,6-trihydroxyphenyl)ethanone;
e) 2,3,4-trihydroxybenzonitrile at a cone voltage of 10 V, hexapole transfer 1
lens voltage of 20 V, source temperature of 150 oC, desolvation temperature of
300 oC and a capillary voltage of 3.2 kV.
15
Supplementary Figure S11. Full-scan HePI mass spectra (left) and product-ion mass
spectrum of the O2-• adduct (right) from samples of a) 2-methoxyphenol; b) 3-
methoxyphenol; c) 4-methoxyphenol at a cone voltage of 10 V, hexapole
transfer 1 lens voltage of 20 V, source temperature of 150 oC, desolvation
temperature of 300 oC and a capillary voltage of 3.2 kV recorded on a Waters
16
3
Micromass Quattro Ultima triple quadrupole mass spectrometer.
Table T1. Calculation of the energy released or absorbed as hydroquinone, catechol,
and resorcinol lose hydrogen gas to produce their respective quinones. The
Gaussian 09 program, using the unrestricted HF method and 6-31G + (d,p)
basis set for all atoms, was used to calculate the sum of electronic and zero-
point energies for each molecule.
17
Table T2. Atom coordinates, select bond lengths, and absolute energies of energy-
optimized product ions and transition states of the superoxide radical-anion
adduct of hydroquinone
18 - 27
Table T3. Bond dissociation energies of H-O-O-H at 298 K 28
4
Chemical Sources:
The following chemicals were purchased from Paragos e. K. (Herdecke, Germany) and used as
obtained: 2,3,4-trihydroxybenzonitrile, 2,6-dihydroxybenzonitrile, 2,3-dihydroxybenzonitrile,
2,4-dihydroxybenzonitrile, 2,5-dihydroxybenzonitrile, 2,5-dihydroxybenzoquinone. 2,4,6-
Trihydroxyacetophenone was purchased from Indofine Chemical Company (Hillsborough, NJ)
and used as obtained.
1,4-Benzoquinone-d4 was purchased from Cambridge Isotope Laboratories (Cambridge, MA).
The following chemicals were purchased from Aldrich (St. Louis, MO): 1,4-benzoquinone, 1,2-
dihydroxybenzene (catechol), 1,3-dihydroxybenzene (resorcinol), 1,4-dihydroxybenzene (1,4-
hydroquinone), 2-aminophenol, 3-aminophenol, 4-aminophenol, 2-methoxyphenol (guaiacol), 3-
methoxyphenol, 4-methoxyphenol (mequinol), 2-hydroxybenzaldehyde, 3-
hydroxybenzaldehyde, 4-hydroxybenzaldehyde, 2,3-dimethyl-1,4-hydroquinone, trimethyl-1,4-
hydroquinone, 5-methylresorcinol, 2,5-dimethylresorcinol, 2,3-dihydroxybenzaldehyde, 3,4-
dihydroxybenzaldehyde, 2,5-dihydroxybenzaldehyde, 2,4-dihydroxyacetophenone, 2,6-
dihydroxyacetophenone, 2’,4’-dihydroxybenzophenone.
Sulfur hexafluoride was provided by Concorde Specialty Gases (Eatontown, NJ).
5
a)
b)
Supplementary Figure S1. a) Sample placement in an open HePI source on a Quattro Ultima
mass spectrometer; b) sample placement and introduction of SF6 to a closed HePI source on the
same instrument. The original ESI source has the same configuration, excepting that a
methanolic solution of the sample is sprayed through the capillary held at high voltage (instead
of passing helium to generate HePI plasma).
6
Supplementary Figure S2. Negative-ion HePI mass spectra acquired on a Waters Micromass ZQ single-
quadrupole mass spectrometer from background ambient air at capillary voltage settings of (a) 4.0 kV,
(b) 3.0 kV, (c) 2.5 kV, and (d) 1.8 kV. The peak intensities are normalized to the absolute intensity (in
arbitrary units) of the m/z 32 peak recorded at capillary voltage 4.0 kV.
7
Supplementary Figure S3. CID mass spectra acquired under ESI-MS conditions from mass-isolated m/z
108 (a, b, c, and d), and m/z 109 (e, f, g, and h) ions, generated from a methanolic solution of 1,4-
hydroquinone, on a Waters Micromass Quattro ultima triple quadrupole mass spectrometer. The CID
spectra of the m/z 108 ion were acquired at a capillary voltage 4.0 kV and at laboratory-frame collision
energies of (a) 10 eV, (b) 20 eV, (c) 30 eV, and (d) 40 eV, and those of the m/z 109 ion were acquired at a
capillary voltage of 1.5 kV and at laboratory-frame collision energies of (e) 10 eV, (f) 20 eV, (g) 30 eV,
and (h) 40 eV.
8
Supplementary Figure S4. Absolute intensity of m/z 108 (blue trace) and 109 (red trace) ions, generated
from a methanolic solution of 1,4-hydroquinone by ESI at a capillary voltage of 3.20 kV, monitored
against time by a selective ion recording (SIR) experiment on a Waters Micromass Quattro Ultima triple
quadrupole mass spectrometer. After two minutes of signal acquisition, the source was engulfed with
sulfur hexafluoride, and at 7.5 min, the flow of SF6 was switched off. Insets show mass spectra
corresponding to each region.
9
Supplementary Figure S5. Negative-ion nanospray ESI mass spectra recorded on a Waters SYNAPT G2
Q-TOF mass spectrometer at different cone voltage settings (10-80 V) from methanolic solutions of (a)
catechol, (b) resorcinol, and (c) hydroquinone. Other experimental conditions: flow rate 1 L/min,
capillary voltage 4.0 kV, extraction cone voltage 3 V. Row 9 depicts typical spectra recorded at a cone
voltage setting of 20 V, from the same solutions and under the same conditions after positioning the
capillary tip closer to the entrance cone to effect a plasma discharge.
10
Supplementary Figure S6. Negative-ion ESI mass spectra recorded on a Waters SYNAPT G2 Q-TOF
mass spectrometer of a) catechol , b) resorcinol, and c) hydroquinone (nanospray) under the following
instrumental conditions: extraction-cone voltage 1.5 V, sampling-cone voltage 20 V, Vernier probe
adjustment screw 5.92 mm, source temperature 100 oC, desolvation gas flow rate 450 L/hr. The capillary
voltage was varied between 1.4 and 4.0 kV.
11
Supplementary Figure S7. Negative-ion HePI mass spectra recorded on a Waters Micromass Quattro
Ultima triple quadrupole mass spectrometer from samples of a) 2,3-dimethylbenzene-1,4-diol, b) 2,3,5-
trimethylbenzene-1,4-diol, c) 2,5-dihydroxybenzonitrile, d) 2,5-dihydroxybenzaldehyde, and e) 2,5-
dihydroxycyclohexa-2,5-diene-1,4-dione, at a cone voltage of 10 V, hexapole transfer 1 lens voltage of 20
V, source temperature of 150 oC, desolvation temperature of 300 oC and a capillary voltage of 3.2 kV.
12
.
Supplementary Figure S8. Negative-ion HePI mass spectra recorded on a Waters Micromass Quattro
Ultima triple quadrupole mass spectrometer from samples of a) 2,3-dihydroxybenzaldehyde, b) 3,4-
dihydroxybenzaldehyde and c) 2,3-dihydroxybenzonitrile, at a cone voltage of 10 V, hexapole transfer 1
lens voltage of 20 V, source temperature of 150 oC, desolvation temperature of 300 oC and a capillary
voltage of 3.2 kV.
13
Supplementary Figure S9. Negative-ion HePI mass spectra recorded on a Waters Micromass Quattro
Ultima triple quadrupole mass spectrometer from samples of a) 2-methylbenzene-1,3-diol; b) 2,5-
dimethylbenzene-1,3-diol; c) 2,6-dihydroxybenzonitrile; d) 1-(2,6-dihydroxyphenyl)ethanone at a cone
voltage of 10 V, hexapole transfer 1 lens voltage of 20 V, source temperature of 150 oC, desolvation
temperature of 300 oC and a capillary voltage of 3.2 kV.
14
Supplementary Figure S10. Negative-ion HePI mass spectra recorded on a Waters Micromass Quattro
Ultima triple quadrupole mass spectrometer from samples of a) 5-methylbenzene-1,3-diol; b) 1-(2,4-
dihydroxyphenyl)ethanone; c) (2,4-dihydroxyphenyl)(phenyl)methanone; d) 1-(2,4,6-
trihydroxyphenyl)ethanone; e) 2,3,4-trihydroxybenzonitrile at a cone voltage of 10 V, hexapole transfer 1
lens voltage of 20 V, source temperature of 150 oC, desolvation temperature of 300 oC and a capillary
voltage of 3.2 kV.
15
Supplementary Figure S11. Full-scan HePI mass spectra (left) and product-ion mass spectrum of the
O2-• adduct (right) from samples of a) 2-methoxyphenol; b) 3-methoxyphenol; c) 4-methoxyphenol at a
cone voltage of 10 V, hexapole transfer 1 lens voltage of 20 V, source temperature of 150 oC, desolvation
temperature of 300 oC and a capillary voltage of 3.2 kV recorded on a Waters Micromass Quattro Ultima
triple quadrupole mass spectrometer.
16
Table T1. Calculation of the energy released or absorbed as hydroquinone, catechol, and resorcinol lose
hydrogen gas to produce their respective quinones. The Gaussian 09 program, using the unrestricted HF
method and 6-31G + (d,p) basis set for all atoms, was used to calculate the sum of electronic and zero-
point energies for each molecule.
Sum of electronic and zero-point energies(Hartree/Particle)
M(Dihydroxybenzene)
M - H2
(Quinone)H2 Energy of
reaction (Hartree/Particle)
Energy of reaction (kcal/mol)
Hydroquinone -380.323052 -379.206402 -1.120774 -0.004124 -2.60Catechol -380.330234 -379.195371 -1.120774 0.014089 8.88Resorcinol -380.331414 -379.19964 -1.120774 0.011 6.93
17
Table T2. Atom coordinates, bond lengths, absolute energies and charge distributions of energy-
optimized product ions and transition states of the superoxide radical-anion adduct of hydroquinone
Number Structure Page Number
1 20
2 Front view: 21 - 25
18
Side view:
3 Front view:
Side view:
26 - 24
19
#1
14 to 15 bond length: 1.60793 ÅAnnihilation of the first spin contaminant: S**2 before annihilation 0.7782, after 0.7505Zero-point vibrational energy 317056.2 (Joules/mol) 75.77825 (Kcal/mol)Standard orientation:
--------------------------------------------------------------------- Center Atomic Atomic Coordinates (Angstroms) Number Number Type X Y Z --------------------------------------------------------------------- 1 6 0 2.194214 -0.368082 -0.019290 2 6 0 2.083611 1.002731 -0.083693 3 6 0 0.834434 1.593733 -0.048174 4 6 0 -0.313879 0.822209 0.059173 5 6 0 -0.190896 -0.560030 0.125853 6 6 0 1.060471 -1.147086 0.088864 7 1 0 2.970226 1.595879 -0.164257 8 1 0 0.732411 2.656890 -0.098022 9 1 0 -1.084179 -1.148186 0.223218 10 1 0 1.141128 -2.216497 0.133854 11 8 0 3.492825 -0.927827 -0.075127 12 1 0 3.531153 -1.848833 0.206371 13 8 0 -1.529138 1.427336 0.115596 14 1 0 -2.335495 0.772654 0.046730 15 8 0 -3.572383 -0.057317 -0.073112 16 8 0 -3.261676 -1.426286 -0.102893 ---------------------------------------------------------------------Zero-point correction= 0.120760 (Hartree/Particle) Thermal correction to Energy= 0.130502 Thermal correction to Enthalpy= 0.131446 Thermal correction to Gibbs Free Energy= 0.083133 Sum of electronic and zero-point Energies= -529.940889 Sum of electronic and thermal Energies= -529.930458 Sum of electronic and thermal Enthalpies= -529.929514 Sum of electronic and thermal Free Energies= -529.980692
20
#2 Front view:
#2 Side view:
#2
Distance between atoms 13 and 14: 3.30723 Å
Annihilation of the first spin contaminant: S**2 before annihilation 0.7776, after 0.7507Standard orientation: ---------------------------------------------------------------------
21
Center Atomic Atomic Coordinates (Angstroms) Number Number Type X Y Z --------------------------------------------------------------------- 1 6 0 -0.127007 1.154785 -0.008966 2 6 0 1.188076 1.585005 0.054027 3 6 0 2.242653 0.693111 0.053583 4 6 0 2.065215 -0.725753 -0.024027 5 6 0 0.693122 -1.116536 -0.072490 6 6 0 -0.364606 -0.210754 -0.069068 7 1 0 1.383885 2.643499 0.106516 8 1 0 3.251389 1.065082 0.107479 9 1 0 0.475789 -2.172135 -0.129328 10 1 0 -1.380427 -0.615979 -0.103206 11 8 0 -1.125515 2.123263 0.001716 12 1 0 -1.964038 1.710208 -0.060191 13 8 0 3.019375 -1.542936 -0.003902 14 1 0 -2.198688 -1.775494 0.368288 15 8 0 -3.078666 -1.497951 0.135823 16 8 0 -3.034273 -0.224167 -0.119626 ---------------------------------------------------------------------Zero-point correction= 0.119366 (Hartree/Particle) Thermal correction to Energy= 0.129598 Thermal correction to Enthalpy= 0.130543 Thermal correction to Gibbs Free Energy= 0.080658 Sum of electronic and zero-point Energies= -530.080701 Sum of electronic and thermal Energies= -530.070469 Sum of electronic and thermal Enthalpies= -530.069525 Sum of electronic and thermal Free Energies= -530.119410
22
Charge Distribution (Mulliken) #2
23
Mulliken atomic spin densities #2:
1 C 0.170003 2 C -0.136490
24
3 C 0.141609 4 C -0.089712 5 C 0.118288 6 C -0.182213 7 H 0.008019 8 H -0.008572 9 H -0.006196 10 H 0.008970 11 O -0.002795 12 H -0.002892 13 O -0.020092 14 H -0.011087 15 O 0.106716 16 O 0.906445 Sum of Mulliken atomic spin densities = 1.00000
Diagram of atom numbering for #2:
Interatomic distances (Angstroms):1 and 16: 4.612142 and 16: 5.166503 and 16: 5.105474 and 16: 4.472635 and 16: 3.736346 and 16: 3.847851 and 14: 3.381022 and 14: 3.610593 and 14: 3.327184 and 14: 2.723645 and 14: 2.317226 and 14: 2.73360
25
#3 Front view:
#3 Side view:
#3
Annihilation of the first spin contaminant: S**2 before annihilation 0.9982, after 0.7986 Standard orientation: --------------------------------------------------------------------- Center Atomic Atomic Coordinates (Angstroms) Number Number Type X Y Z --------------------------------------------------------------------- 1 6 0 0.038970 -0.699564 -0.154033 2 6 0 1.291603 -1.243914 -0.139532 3 6 0 2.468569 -0.428255 0.001556 4 6 0 2.251298 0.988739 0.124957 5 6 0 0.993195 1.519055 0.108701 6 6 0 -0.179900 0.710742 -0.029828 7 1 0 -0.828535 -1.326182 -0.255417 8 1 0 1.438327 -2.306303 -0.233310 9 1 0 3.121762 1.613610 0.230173 10 1 0 0.843811 2.580197 0.201020 11 8 0 3.613916 -0.921029 0.016675 12 8 0 -1.340084 1.231708 -0.039494 13 1 0 -2.720148 0.480274 -0.277112 14 8 0 -3.634233 0.111977 -0.378547 15 8 0 -3.551964 -1.088985 0.355482
26
16 1 0 -3.738709 -0.791789 1.230793 ---------------------------------------------------------------------Zero-point correction= 0.120154 (Hartree/Particle) Thermal correction to Energy= 0.130180 Thermal correction to Enthalpy= 0.131124 Thermal correction to Gibbs Free Energy= 0.080943 Sum of electronic and zero-point Energies= -530.122654 Sum of electronic and thermal Energies= -530.112627 Sum of electronic and thermal Enthalpies= -530.111683 Sum of electronic and thermal Free Energies= -530.161865
27
Table T3. Bond dissociation energies of H-O-O-H at 298 K
Dissociation energy (kJ/mol) Dissociation energy (kcal/mol)O-O bond 213.8 ± 2.1a 50.7H-O bond 374.5 ± 8.4b 89.1aT. L. Cottrell, The Strengths of Chemical Bonds, 2d ed., Butterworth, London, 1958; B. deB. Darwent, National Standard Reference Data Series, National Bureau of Standards, no. 31, Washington, 1970; S. W. Benson, J. Chem. Educ. 42:502 (1965); and J. A. Kerr, Chem. Rev. 66:465 (1966).bWagman, D. D., Evans, W. H., Parker, V. B., Halow, L., Bailey, S. M., and Schumm, R. H., Selected values of chemical thermodynamic properties. Part 3. Tables for the first thirty-four elements in the standard order of arrangement, Nat. Bur. Stand. (U.S.), Tech. Note 270-3 (1967) and Part 4, Tables for Elements 35 through 53 in the standard order of arrangement, Nat. Bur. Stand. (U. S.), Tech. Note 270-4 1969).
28