Halogen Bonding Darin J. Ulness Department of Chemistry Concordia College, Moorhead, MN.

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Halogen Bonding

Darin J. UlnessDepartment of Chemistry

Concordia College, Moorhead, MN

Outline

• Hydrogen bonding

• History

• The hole and hole bonding

• I(2)CARS Spectroscopy

• Data

• Discussion

Hydrogen Bonding•Hydrogen on a N, O, F•Interact with a N, O, F•Bond distance shorter than sum of Van der Waals Radii

•Angle approximately 180o

Halogen Bonding

•I > Br > Cl, no F•Interact with a N, O•Bond distance shorter than sum of Van der Waals Radii

•Angle approximately 180o

Halogen Bonding: History

•F. Guthrie, J. Chem. Soc. 16, 239 (1863)

•Complexation of I2 and NH3

•I. Remsen, J.F. Norris, Am. Chem. J. 18, 90, (1896)

•Complexation of X2 and methyl amines

•O. Hassel, Proc. Chem. Soc. 7, 250 (1957) [Nobel Prize 1969]•Donor/acceptor complexes: Halogens and Lone Pair

•T. Di Paolo, C. Sandorfy, Can. J. Chem. 52, 3612 (1974)•Spectroscopic studies aromatic amines and halo-alkanes

Halogen Bonding: Today

Halogen Bonding

Biochemistry• Biomolecular engineering• Drug Design

Materials Science• Crystal engineering• Molecular recognition

ComputationalChemistry

• hole bondingVoth A. R. et.al. PNAS 2007;104:6188-6193 Resnati et.al. J. Fluroine Chem.

2004;104: 271

The hole

I

Test ChargeFree Iodine

Atom

Test Charge “feels” an electroneutral field

Test charge far from an iodine atom

The hole

I

Test charge close to an iodine atom

Test Charge “feels” an electropositive field

An arbitrary spherical surface carries an eletropositive potential !

The hole

Test Charge

In molecules the electron density is directed into the bond

The hole

Electropositve-hole

Test Charge

Electroneutral“ring”

Electronegative“belt”

The hole

Electropositve-hole

Test Charge

Electroneutral“ring”

Electronegative“belt”

Perfluoroinate: Stronger hole

hole bonding with pyridine

Pyridine as a probe of Halogen bonding

The ring stretches of pyridine act as a probe of its environment

C

N

C

C C

C

C

N

C

C C

C

“ring-breathing” mode “triangle” mode

Pyridine as a probe of Halogen bonding

Hydrogen bonding to a water modulates the stretching frequency

C

N

C

C C

C

free pyridine

C

N

C

C C

C

O

HH

H-bonded pyridine

Experiment

•Coherent Raman Scattering: e.g., CARS•Frequency resolved signals•Spectrograms•Molecular liquids

Light

frequency

Spectrum

time

One frequency (or color)

Electromagnetic radiation•Focus on electric field part

Noisy Light: Definition•Broadband•Phase incoherent•Quasi continuous wave

Ele

tric

Fie

ld S

tren

gth

Time

No

isy

Lig

ht

Sp

ect

rum

Frequency

Time resolution onthe order of the correlation time, c

P= E

Nonlinear Optics

Signal

Material

Light field

Perturbation series approximation

P(t) = P(1) + P(2) + P(3) …

P(1) = (1)E, P(2) = (2)EE, P(3) = (3)EEE

CARSCoherent Anti-Stokes Raman Scattering

R

1

12

CARS

1-2= R

CARS= 1 +R

CARS with Noisy Light•I(2)CARS

•We need twin noisy beams B and B’.•We also need a narrowband beam, M.•The frequency of B (B’) and M differ by roughly the Raman frequency of the sample.•The I(2)CARS signal has a frequency that is anti-Stokes shifted from that of the noisy beams.

B

B’M

I(2)CARS

I(2)CARS: Experiment

Monochromator

NarrowbandSource

BroadbandSource(noisy light)

Lens

Sample

Interferometer

B

B’

MI(2)CARS

ComputerCCD

I(2)CARS: Spectrogram

Monochromator

NarrowbandSource

BroadbandSource

Lens

Sample

Interferometer

B

B’

MI(2)CARS

ComputerCCD

•Signal is dispersed onto the CCD

•Entire Spectrum is taken at each delay

•2D data set: the Spectrogram

•Vibration information

I(2)CARS: Data Processing

18000 18100 18200 18300 18400

-2

-1

0

1

2

BenzeneT22

0 200 400 600 800 1000 1200

0

25

50

75

100

125

150

BenzeneT22

100 200 300 400

0.2

0.4

0.6

0.8

Fourier

Transformation

X-Marginal

Pyridine as a probe of Halogen bonding

980 1000 1020 1040

0.0

0.2

0.4

0.6

0.8

1.0

No

rma

lize

d X

-ma

rgin

al

Wavenumber / cm-1

Pyridine as a probe of Halogen bonding

980 1000 1020 1040

0.0

0.2

0.4

0.6

0.8

1.0 100% pyr 85% pyr 70% pyr 55% pyr 25% pyr

No

rma

lize

d X

-ma

rgin

al

Wavenumber / cm-1

freepyridine

H-bondedpyridine

ring-breathing

Pyridine as a probe of Halogen bonding

C4F9I

C6F13IC3F7I

2-iodo-perfluoropropane

1-iodo-perfluoroalkanes

1-iodo-perfluoroalkanes

0

0.5

1

1.5

2

2.5

3

3.5

4

900 920 940 960 980 1000 1020 1040 1060 1080 1100

Neat

0.1

0.2

0.3

0.4

0.5

0.6

0.7

.8

0.9

C6F13I and Pyridine

0

0.5

1

1.5

2

2.5

3

3.5

4

900 920 940 960 980 1000 1020 1040 1060 1080 1100Frequency (cm-1)

Norma

lized In

tesity

Neat

0.1

0.2

0.3

0.4

0.5

0.6

0.7

.8

0.9

C4F9I C6F13I

2-iodo-perfluoropropane

C6F13I and Pyridine

0

0.5

1

1.5

2

2.5

3

3.5

4

900 920 940 960 980 1000 1020 1040 1060 1080 1100Frequency (cm-1)

Norma

lized In

tesity

Neat

0.1

0.2

0.3

0.4

0.5

0.6

0.7

.8

0.9

C3F7I C6F13I

Pyridine and C3F7I

0

0.5

1

1.5

2

2.5

3

3.5

4

900 920 940 960 980 1000 1020 1040 1060 1080 1100

Frequency (cm-1)

Norma

lized In

tensity

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

Neat

Temperature StudiesC3F7I C6F13I

C3F7I Temp Study

0

0.5

1

1.5

2

2.5

3

3.5

4

4.5

900 920 940 960 980 1000 1020 1040 1060 1080 1100

Frequency (cm-1)

Norma

lized In

tensity

c3f7ipy65Cc3f7ipy50Cc3f7ipy35Cc3f7ipy25Cc3f7ipy15Cc3f7ipy0Cc3f7ipy -15Cc3f7ipy -30C0.9

Neat Py25C

Name

0

0.5

1

1.5

2

2.5

3

3.5

4

4.5

900 920 940 960 980 1000 1020 1040 1060 1080 1100

Frequency (cm-1)

Norma

lized In

tensity

c6f13ipy60Cc6f13ipy40Cc6f13ipy25Cc6f13ipy15Cc6f13ipy0Cc6f13ipy-15Cc6f13ipy-25C0.8

0.9

Neat

Thermodynamic Conclusions

•The equilibrium constant for the 2-iodo-perflouropropane is greater than for the 1-iodo-perfluoroalkanes.

•Mole fraction studies•The energy of interaction (strength of the halogen bond) is comparable across the iodo-perfluoroalkanes.

•Equal blue-shifts•The enthalpy for complexation is smaller for the 2-iodo-perfluoropropane than for the 1-iodo-perfluoroalkanes.

•Temperature studies

Thermodynamic Conclusions

H

S

py

py py

pyipa

ipa ipa

ipa

vH

vS

sH

sS

hbH

hbS

Thermodynamic Conclusions

H

S

py

py py

pyipa

ipa ipa

ipa

vH

vS

sH

sS

hbH

hbS

Thermodynamic Conclusions

H

S

py

py py

pyipa

ipa ipa

ipa

vH

vS

sH

sS

hbH

hbS

I’m Special !

2-iodo-perfluoropropane 1-iodo-perfluoroalkanes

Conjecture

•Stronger and more F directed self-halogen bonding leads to more local solvent structure order.

•Increased positive entropy contribution•Increased positive enthalpy contribution

One is better than two ?

One is better than two ?

Importance of the Fluorine

Pyridine and H2H

0

0.5

1

1.5

2

2.5

900 920 940 960 980 1000 1020 1040 1060 1080 1100

Frequency (cm-1)

Norma

lized In

tensity

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

Neat

Acknowledgements

•Dr. Haiyan Fan

•Dr. Mark Gealy

•Jeff Eliason

•Scott Flancher

•Diane Moliva

•Danny Green

•NSF CAREER: CHE-0341087

•Dreyfus Foundation

•Concordia Chemistry Research Fund

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