82
ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS by NICHOLE M. JACKSON, B.S. A THESIS IN CHEMISTRY Submitted to the Graduate Faculty of Texas Tech University in Partial Fulfillment of the Requirements for the Degree of MASTER OF SCIENCE Approved Accepted December, 2001

ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

  • Upload
    others

  • View
    4

  • Download
    0

Embed Size (px)

Citation preview

Page 1: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

ANALYSIS OF THE PHYSICAL PROPERTIES

OF IONIC LIQUIDS

by

NICHOLE M. JACKSON, B.S.

A THESIS

IN

CHEMISTRY

Submitted to the Graduate Faculty of Texas Tech University in

Partial Fulfillment of the Requirements for

the Degree of

MASTER OF SCIENCE

Approved

Accepted

December, 2001

Page 2: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

ACKNOWLEDGEMENTS

I would like to thank Dr. Allan D. Headley for all his support and input on

my research project. The many emails that were sent back and forth with his

ideas and suggestions were a constant help. I would also like to thank Dr.

Richard A. Bartsch for his support and willingness to be on my committee. The

experience I received under his mentorship was invaluable. Dr. Jaewook Nam

was helpful in the theoretical analyses. For the NMR spectroscopic analysis, I

would like to thank Mr. David Purkiss. The financial support came from the

Welch Foundation without which none of this would have been feasible.

Page 3: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

TABLE OF CONTENTS

ACKNOWLEDGEMENTS ii

ABSTRACT v

LIST OF TABLES vi

LIST OF FIGURES vii

CHAPTER

I. INTRODUCTION 1

II. RESULTS AND DISCUSSION 12

Synthesis of 1-Alkyl-3-methylimidazollum Salts 13

NMR Studies of 1-Alkyl-3-methylimidazolium Salts 17

Nature of the Solvent Interactions 42

Use of SolvatochromIe Parameters to Analyze the Solvation Interactions of BMrBF4' 46

Analysis of the Solvent Interactions of BMrPFe' 49

Analysis with Gaussian 94 for Imidazollum Cations 51

Analysis of Solvation Properties of Ionic Liquids by Theoretical Descriptors 56

III. CONCLUSIONS 62

IV. EXPERIMENTAL 63

Preparation of 1-Methyl-3-propyllimidazolium Chloride ... 63

Preparation of 1-Butyl-3-methylimldazolium Chloride 63

Preparation of 1-Butyl-3-methylimldazolium Hexafluorophosphate 64

Page 4: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Preparation of 1-Butyl-3-methylimidazolium Tetrafluoroborate 64

Preparation of 1-Methyl-3-pentyllimidazolium Chloride.... 65

Preparation of 1-Oetyl-3-methylimidazolium Chloride 65

Preparation of 1-Hexadeeyl-3-methylimidazolium Bromide 66

Preparation of 1-Hexadecyl-3-methylimidazolium Tetrafluoroborate 66

Preparation of 1-Hexadecyl-3-methylimidazolium Hexafluorophosphate 66

Preparation of NMR Solvent Study Samples 67

Procedure for Calculating the Density 67

REFERENCES 69

IV

Page 5: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

ABSTRACT

The recognition of ionic liquids as possible green solvents has boosted the

interest in this field. Ionic liquids are simply, liquids that are comprised entirely of

ions. The aspect of ionic liquids as solvents and catalysts has gained notable

attention but little knowledge in the physical properties of these liquids has been

achieved. It is important to gain a quantitative understanding of how these new

class of solvents affect reaction rates and the outcome of reactions. As a result of

a better understanding, the ability to better predict the outcome of these reactions

performed in these solvents should enhance their usage. In this study, the

solute/solvent interactions of a group of ionic liquids, which have different alkyl

side chains and anions, were investigated. By changing the length of the side

chain or the anion, the physical properties of the ionic liquids vary. Ionic liquids

with hydrophobic side chains or bulky polarizable anions are not as good a

hydrogen bond donor as those with a less hydrophobic side chain or a smaller,

more basic anion.

Page 6: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

LIST OF TABLES

1 H NMR chemical shifts in ppm for the aromatic hydrogens of BMrBF4' in the deuterated solvents 18

2 H NMR chemical shifts in ppm for the aromatic hydrogens of BMrPFe' in the deuterated solvents 23

3 H NMR chemical shifts in ppm for the aromatic hydrogens of HDMrBF4'in deuterated solvents 30

4 H NMR chemical shifts in ppm for the aromatic hydrogens of HDMrPFe" in the deuterated solvents 35

5 SolvatochromIe Parameters 47

6 Coefficients and statistics using equation 14 without polarizability (71*) for BMrBF4" 49

7 Coefficients and statistics using equation 14 without polarizability (71*) for BMrPFe" 51

8 Z-Matrix for imidazolium cation of Figure 31 53

9 Charge distribution of atoms on the imidazolium cation 54

10 Charge distribution of atoms of 1-fluoroimidazolium cation 55

11 Theoretical descriptors for different ionic liquids and molecular solvents 59

VI

Page 7: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

LIST OF FIGURES

1 A, 1-ethyl-3-methylimidazolium, EMI""; B, 1-butyl-3-methylimidazolium, BMT; or C, A/-butylpyridinium cations, respectively 2

2 Organic cation with R side-arm groups and X" anion 3

3 A low-melting-point ionic liquid, 1-ethyl-3-methylimidazolium tetrachloroaluminate 3

4 Diels-Alder reaction in an ionic liquid system 5

5 Arene exchange of ferrocenes using a 1-butyl-3-methylimidazolium BMI*- based ionic liquid 6

6 Hydrogenation of 1-pentene to form pentane and 2-pentene 7

7 1-Butyl-3-methylimidazolium tetrafluoroborate (X" = BF4"), 1-butyl-3-methylimidazolium hexafluorophosphate (X' = PFe) 8

8 Reaction mechanism for synthesis of BMrci" 13

9 Reaction scheme for BMrBF4" and BMrPFe' 14

10 Reaction scheme for HDMrBF4' and HDMrPFe" 16

11 Aromatic hydrogen numbering for BMI* BF4" 17

12 Chemical shifts of the aromatic hydrogens Hi and H2 of BMrBF4' in the deuterated solvents 19

13 Chemical shifts of the aromatic hydrogens Hi and H3 of BMrBF4" in the deuterated solvents 20

14 Chemical shifts of the aromatic hydrogens H2 and H3 of BMrBF4' in the deuterated solvents 21

15 Chemical shifts of the aromatic hydrogens Hi and H2 of BMrPFe" in deuterated solvents 25

16 Chemical shifts of the aromatic hydrogens Hi and H3 of BMrPFe" in the deuterated solvents 26

VII

Page 8: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

17 Chemical shifts of the aromatic hydrogens H2 and H3

of BMrPFe" in the deuterated solvents 27

18 Slope comparison of BMrBF4' and BMrPFe' 29

19 Chemical shifts of the aromatic hydrogens Hi and H2 of HDMrBF4" in the deuterated solvents 31

20 Chemical shifts of the aromatic hydrogens Hi and H3 of HDMrBF4' in the deuterated solvents 32

21 Chemical shifts of the aromatic hydrogens H2 and H3 of HDMrBF4" in the deuterated solvents 33

22 Chemical shifts of the aromatic hydrogens Hi and H2 of HDMrPFe" in the deuterated solvents 36

23 Chemical shifts for the aromatic hydrogens Hi and H3 of HDMrPFe" in the deuterated solvents 37

24 Chemical shifts for the aromatic hydrogens H2 and H3 of HDMrPFe' in the deuterated solvents 38

25 Slope comparison of HDMrBF4" and HDMrPFe" 40

26 Slope comparison of BMrBF4", BMrPFg", HDMrBF4", andHDMrPFe" 41

27 Proposed interaction between the BMI* cation and the acidic solvent 42

28 Proposed interaction between the BMI* cation and the basic solvent 43

29 Proposed interaction between the HDMI* cation and the acidic solvent 44

30 Proposed interaction between the HDMI* cation and

the basic solvents 45

31 Aromatic hydrogen designation for BMrPFe" 50

32 Numbering system for imidazolium cation 52

VIII

Page 9: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

33 1-Fluoroimidazolium cation 55

34 Structure of 1,3-disubstituted imidazolium cation for which theoretical descriptors have been developed 57

iX

Page 10: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

CHAPTER I

INTRODUCTION

Organic reactions are mainly performed in nonaqueous media. Chemists

face a major challenge in the separation of the organic products, or catalysts,

from the reaction mixtures. Polar solvents, such as dimethyl sulfoxide (DMSO)

or dimethylformamide (DMF) are conventionally used to create the polar

environment for most organic reactions, present tremendous difficulty in the

separation of the products from the reaction mixtures. Added to this difficulty is

the cost to dispose of these solvents, which is estimated at approximately 5

billion dollars per year. Ionic liquids, a new field of chemistry, has extremely

interesting properties from a fundamental chemist's point of view and could have

a major impact on society. Industry is eagerly exploring ways in which ionic

liquids can deliver some benefits. The environmental impact of replacing

conventional solvents with ionic liquids could result in less waste formation,

reduction of cost, and the reduction in energy consumption.

Ionic liquids are liquids at room temperature that are comprised entirely of

ions. It is important to note that the term "ionic liquid" In this context represents a

whole class of liquids with a wide range of stabilities and properties, which

importantly can be readily tailored. It has been stated that there are in excess of

10^ readily accessible potential room temperature ionic liquid systems. Ionic

liquids have some unique properties that make them very important solvents for

Page 11: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

a large array of organic reactions. These ionic liquids may have a liquid range

from temperatures as low as -96 °C and as high as 300 C."

The organic cation is usually a heterocyclic cation such as 1-ethyl-3-

methylimidazolium, EMr, 1-butyl-3-methylimidazolium, BMr, or

A/-butylpyridinium shown in Figure 1. These large organic cations account for the

low melting points of the salts. The size of the cation is responsible for the

magnitude of the melting point, i.e., the bigger the cation, the lower the melting

point

H3C ^ ^ CH2CH3 N 1 CH2CH2CH2CH3

/r^ c .Nki>;N

|_| Q^ ^^"^ "CH2CH2CH2CH3 '3^

B

Figure 1. A, 1-ethyl-3-methylimidazolium, EMr; B, 1-butyl-3-methylimidazolium, BMI*; or C, A/-butylpyridinium cations, respectively.

By varying the organic cation, including its R group(s) and the identity of

the cation, as shown in Figure 2, ionic liquids can be fine-tuned to meet specific

properties. For example, the melting points differ as a function of the length of

the 1-alkyl group of 1-alkyl-3-methylimidazolium tetrafluoroborates^ and 1-alkyl-3-

methylimidazolium hexafluorophosphates.

Page 12: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

A general trend develops from hydrophilic to hydrophobic side chains, on

increasing the chain length due to increasing hydrocarbon character.

N3V ; N I

/ ^ \

Ro ^2 R,

Figure 2. Organic cation with R side-arm groups and X" anion.

The numbering system used in naming ionic liquids is also shown in

Figure 2. Anions, such as tetrachloroaluminate, [AICU]", on the other hand,

determine to a large extent the chemical properties of the system. Varying the

molar ratio of tetrachloroaluminate influences the Lewis acidity of Figure 3.

+ )\ AICI4"

Figure 3. A low-melting-point Ionic liquid, 1-ethyl-3-methylimidazolium tetrachloroaluminate.

As the molar ratio of aluminum trichloride to dialkylimidazolium chloride ranges

from <1 to >1, the ionic liquid transitions from a highly complexing mixture to

Page 13: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

what can be regarded as a Lewis acid-noncoordinating media. 1-Ethyl-3-

methylimidazolium chloride-aluminum chloride, EMrcrAICl3 is a liquid and

thermally stable from almost -100 °C to approximately 200 °C. For

chloroaluminate ionic liquid systems, such as EMrci'AICb, CI" is the main anion,

which is a Lewis base; the anion [AICU]" is neither acidic or basic and [AI2CI7]' is a

Lewis acid." The concentration of these anions and also the Lewis acidity of the

system vary depending on the ratio of AICI3 and EMrci" which determines the

acidity of the system and ultimately the chemical properties.

The role of the solvent in organic reactions can influence the course of

reactions in a variety of ways, such as higher reaction rates and better reaction

control. The Diels-Alder reaction is one of the most powerful carbon-carbon bond

forming reactions.' It has been shown that the polarity of the solvent has a

dramatic influence upon the endo-exo ratio in some Diels-Alder reactions. The

more polar (endo) transition state is stabilized by a more polar solvent.

Page 14: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

For the Diels-Alder reaction shown in Figure 4, the use of an acidic ionic liquid

increased the selectivity of the endo product in comparison to several other

solvents.""

w // * H3C CH2CH3

CH2=CHC02CH3 endo

CO2CH3 exo

Figure 4. Diels-Alder reaction in an ionic liquid system.

An observed endo selectivity enhancement of four fold from the 48% AICI3 basic

mixture to the 51% AICI3 acidic mixture was a direct result of the increase in

Lewls/Bronsted acidity of the medium, while the observed 5:1 endo/exo product

ratio is a reflection of the polarity of the medium.

"Probably the most Important advantage of using ionic liquids is that they

have no measurable vapor pressure," says chemistry professor Kenneth R.

Seddon, who leads a team at Queen's University of Belfast, Northern Ireland,**

making ionic liquids strong candidates for recyclable "green" solvents

Page 15: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

The use of ionic liquids as solvents has taken research into a direction of

dual functioning of the Ionic liquid wherein the ionic liquid is used as the solvent

and as the catalyst. Use of BMrCfAICb in an arene exchange reactions of

ferrocenes has been reported (Figure 5). ^

^

Arene

BMrcrAici3 Fe • Fe I +[BMI]HCl2 +arene I

Figure 5. Arene exchange of ferrocenes using a 1-butyl-3-methylimidazolium BMI*- based ionic liquid.

Ionic liquids that use the chloroaluminate ions are important because AICI3 Is

used industrially to catalyze a large number of reactions. For such biphasic

systems, the AICI3 is dissolved in the ionic liquid and, after the reaction Is

complete, the organic products separate into an organic layer and the catalyst

remains In the ionic liquid phase.

1-Butylpyridinium chloride-aluminum(lll) chloride, NbuPy' CfAICb, and 1-

ethyl-3-methylimidazolium chloride-aluminum(IH) chloride, EMrCPAICb, are Ionic

liquids used as solvents for different reactions and exhibit Bronsted, Lewis, and

Franklin acidity. ^ These properties make it possible to dissolve a wide range of

Page 16: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

organic molecules to an appreciable extent, meaning much lower volumes of

solvent are required for a given process. ^

By varying the anion, ionic liquids can be fine-tuned to provide desired

properties. Ionic liquids have been found to dissolve charged species so the

hydrogenation of 1-pentene using the Osborn [Rh(NBD)(PPh3)2]' PFe'complex

as the cationic catalyst precursor was tested (Figure 6). ^ With BMrSbFe" as the

solvent, hydrogenation rates of 1-pentene are nearly five times higher compared

to the homogeneous reaction in acetone, in spite of the expected limited

solubilities of reactants in the polar phase."* With BMrci" and CuCI (1:1.5), only

isomerization to 2-pentene with 100% selectivity was observed. This

demonstrates that selectivity can be strongly influenced by the nature of the

anion of an ionic liquid.

H3C [Rh(NBD)(PPh3)2]'^PF6"

H 2 C ^ ^ ^ ^CH3

"" H3C H2

Figure 6. Hydrogenation of 1-pentene to form pentane and 2-pentene.

In traditional solvent extraction, ^ the two immiscible phases employ an

organic solvent (diluent) and an aqueous solution. The diluents, which are

volatile, are a danger to the environment, expensive to purchase, and have a

Page 17: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

high cost to dispose of the waste. Studies of BMrPFe" as a medium for liquid-

liquid extraction prove that the distribution ratios of aromatic solutes in an ionic

liquid versus distribution ratios in 1-octanol-water system are similar in

relations. ^ This evidence proves that ionic liquids may be suitable media for the

design of novel liquid-liquid extraction systems.

1-Butyl-3-methylimidazolium tetrafluoroborate, BMrBF4" (Figure 7), has

been investigated as a solvent in two-phase catalytic hydrogenation reactions. 1-

Butyl-3-methylimidazollum hexafluorophosphate BMrPFe" has also been studied

in two-phase catalytic hydrogenation and in liquid-liquid extraction systems. ' '

HoC CH2CH2CH2CH3

Figure 7. 1-Butyl-3-methyllmidazolium tetrafluoroborate (X' = BF4'), 1-butyl-3-methylimidazolium hexafluorophosphate (X" = PFe").

Most of the research carried out thus far on these solvents has involved

their use in electrochemical systems and in organic syntheses. The ability to

predict property variations of molecules in different environments is important.

With the growing interest in ionic liquids, research on physlochemical properties

of these ionic liquids should be conducted. One way to probe specific properties

8

Page 18: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

of ionic liquids is to analyze their ability to be involved in the solute-solvent

interactions. The nature and extent of solute-solvent interactions are able to alter

various properties of solutes.'' Solvent effects on the electronic spectrum of a

molecule are referred as "solvatochromism". The SolvatochromIe shifts

associated with electronic transitions in solution result from different solvation

energies of the initial and final electronic states. Thus, study of SolvatochromIe

shifts gives relevant information concerning the kind of solute-medium

interactions and allows for the understanding of electronic distribution changes

between the states involved in the electronic transition. °

Various solvent parameters have been proposed to quantify the interactive

abilities of solvents with solutes. Over the years, a number of descriptors have

been developed, ^ but those developed by Taft and co-workers have been widely

used to analyze solvent effects on rates and equilibria of many organic reactions

and are used in this research project. ' ^

Kamlet, Taft, and co-workers have examined the nature and importance of

solute/solvent interactions and described them with Equation 1.^^

Property = bulk/cavity term + dipolarity/polarizability term(s)

+ hydrogen bonding term(s) + constant (1)

Page 19: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

The bulk/cavity term measures the energy that is needed to overcome the

cohesive solvent/solvent interactions to form a cavity for the solute molecule.

The dipolarity/polarizability terms measure the energies of solute/solvent dipole

and induced dipole interactions that contribute to solvation. The hydrogen

bonding term is a measure of specific interactions between the solvent and

solute. This reflects the ability of the solvent to accept hydrogen bonds from the

solute, which is designated as the hydrogen bond acceptor basicity (HBAB), and

the ability of the solvent to donate hydrogen bonds to the solute, which is

designated as the hydrogen bond donor acidity (HBDA). The first term in

Equation 1 is endoergic and the last two terms are exoergic. A linear statistical

fitting among the variables is used for Equation 1.

For an ionic liquid, the important medium contributions should be

dipolarity/polarizabiiity (owing to the charge separation), the hydrogen bond

donor abilities (owing to the presence of the acidic C-H), and the hydrogen bond

acceptor abilities (owing to the presence of an anion). The product of the

dipolarity/polarizability term TI* is a measure of the energies of the solvent dipole

and induced dipole interactions that contribute to solvation. "

Another way to evaluate the solvation properties of ionic liquids is the use

of theoretical descriptors. The relationships that exist between the chemical

properties of molecules and their molecular structural features have been used to

correlate the molecular structural properties of compounds with known biological,

chemical, and physical properties. ^ These relationships are often referred to as

10

Page 20: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

quantitative structure-activity relationships (QSAR). In cases where a specific

property is examined, the term that Is used is quantitative structure-property

relationships (QSPR). The success of QSAR and QSPR depends on the

assumption that quantitative relationships exist between microscopic features

and macroscopic properties of molecules. QSAR and QSPR have been used

successfully to predict different properties of compounds that have similar

molecular features to other compounds in a particular series. ® The ability of

QSAR and QSPR to make successful predictions of macroscopic properties

depends strongly on the accurate quantification of microscopic features of the

molecule, which are often refen-ed to as descriptors.

Molecular orbital calculations have been used for the development of

molecular descriptors. ^ The descriptors that are obtained by computational

methods are often reliable and may be obtained quickly. ® Statistically based

Interaction indices derived fi'om molecular surface electrostatic potentials have

been used also to predict the properties of molecules. ® A set of six theoretical

linear solvation energy relationship (TLSER) descriptors has been developed by

Famini and Wilson for a wide variety of compounds and used successfully to

correlate properties of the compounds,^ including five nonspecific toxins, the

activity of some local anesthetics and their molecular transform; opiate activity of

some fentanyl-like compounds; and the six physicochemical properties of

absorption on charcoal, HPLC retention index, octanol-water partition

coefficients, phosphononthiolate hydrolyslsrate constants, aqueous equilibrium

11

Page 21: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

constants and electronic absorption of some yields. TLSER descriptors have

been used successfully also to describe the effects of structural variations of

carboxylic acids, alcohols, silanols, anilines, hydrocarbons, and oximes on their

acid/base properties in the gas phase. ^ The TLSER descriptors were developed

to correlate with linear solvation energy relationships (LSER) descriptors. ^ The

descriptors give multi-linear regression (MLR) equations with correlation

coefficients, R, and standard deviations (SD) close to those for LSER and are

widely applicable to solute/solvent interactions as the LSER set. The TLSER

descriptors represent electronic properties of molecules in the gas phase. These

descriptors depict the interactions between the molecules - a solute and a

solvent.

Deciding on the most appropriate ionic liquid for a particular reaction

environment depends on a greater understanding of the solvents themselves. In

particular, the features of the ionic liquids which can be tailored, include: acid-

base characteristics, solubility, hydrophilicity, viscosity, and thermal range. ^

Changing the anion or the side chain will have an infiuence on the properties of

ionic liquids. With this in mind, my research focuses on the physical properties of

ionic liquids using NMR chemical shifts and theoretical calculations to study

solute/solvent interactions.

12

Page 22: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

CHAPTER II

RESULTS AND DISCUSSION

Svnthesis of 1-Alkvl-3-methvlimidazolium Salts

In the experimental section several ionic salts were synthesized but due to

time constraints only the BMI* and the HDMr cations were used to perform the

property studies. Figure 9 shows the reaction scheme for the synthesis of the

specific Ionic liquids, BMrBF4' and BMrPFe". The neat reaction of 1-

methylimidazole and 1-chlorobutane at refiux provided a high yield of the desired

salt.

The reaction of the 1-methylimldazole with the alkyl halide is likely an SN2

reaction as shown in Figure 8. The nucleophilic 1-methyllmidazole attacks the

V/" \ /" y V ^^ ^ CI CH2CH2CH2 CI • NAjy N / ^ \ / ^ ^

I \«^ _ - / CI "2 H H

Figure 8. Reaction mechanism for synthesis of BMrci".

primary alkyl halide to create the transition state which goes on to produce the

desired product. The yields for the reactions of BMrBF4' and BMfPFe" are

essentially the same, ranging from 94-98%.

13

Page 23: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

+ CH3CH2CH2CH2CI

Reflux 48 hours

' '

NaBF4

BF,

Figure 9. Reaction scheme for the synthesis of BMrBF4' and BMrPFe"

14

Page 24: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

As shown in Figure 9, equal moles of sodium tetrafluoroborate and 1-

butyl-3-methylimldazolium chloride, BMrci", are stired at room temperature in

acetone to produce BMrBF4" and equal moles of hexafluorophophoric acid and

BMrci" are stirred at room temperature In water to produce BMrPFe".

For the synthesis of 1-hexadecyl-3-methylimidazolium salts, the first

reaction of 1-methylimldazole and 1-bromohexadecane took place in essentially

quantitative yield. The reactions for producing the HDMrBF4" and HOMfPFe" are

the same as for BMrBF4" and BMrPFe' as seen In Figure 10. The alkyl bromide

was used on the saturated carbon chain because bromide is a better leaving

group.

Yields of 1-hexadecy-3-methyllmldazolium tetrafluoroborate and 1-

hexadecy-3-methylimidazolium hexafluorophophorate were essentially

quantitative.

15

Page 25: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

CH3(CH2)i5Br

heat 30 minutes

1 '

Br" (CH2)i5CH3

NaBF4

48 hours 48 hours

BF. (CH2)i5CH3

N \ >/N. pp - ^(CH2)i5CH3

Figure 10. Reaction scheme for the synthesis of HDMrBF4' and HDMrPFe"

16

Page 26: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

NMR Studies of 1-Alkvi-3-methvlimldazolium Salts

Figure 11 gives the numbering for the aromatic hydrogens of the ionic

liquid, 1-butyl-3-methylimidazolium tetrafluoroborate, BMI* BF4".

HoC CH2CH2CH2CH3

Figure 11. Aromatic hydrogen numbering for BMf BF4".

Solutions of the ionic liquid were prepared In the deuterated solvents

shown in Table 1 at a concentration of 0.45 M. Table 1 also shows the chemical

shift values in ppm for the aromatic hydrogens of BMI* BF4"in the different

deuterated solvents.

17

Page 27: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Table 1. H NMR chemical shifts in ppm for the aromatic hydrogens of BMrBF4' in the deuterated solvents.

Solvent

Acetone

Acetonitrile

Acetic Acid

DMF

DMSO

Ethand

Methanol

Trifluoroacetic Acid

Water

H i

8.89

8.46

8.67

9.15

9.07

8.77

8.78

8.59

8.54

H2

7.70

7.37

7.51

7.87

7.77

7.57

7.58

7.47

7.34

H3

7.65

7.34

7.47

7.80

7.69

7.50

7.51

7.45

7.30

As can be seen from Table 1, the different solvents have little influence on the

chemical shifts for H2 and H3compared to Hi. The chemical shifts of H2 and H3

show minor changes in the different solvents, while Hi has a larger chemical shift

range and appears be more sensitive to the change In solvent. Hi is shifted

farther downfield in a more polar solvent compared to H2 or H3. The chemical

shift for Hi in the polar DMF is 9.15 ppm whereas, H2 and H3 have chemical

shifts of 7.87 and 7.80, respectively.

Figures 12,13, and 14, are the plots of the chemical shift data for the

aromatic hydrogens of BMrBF4".

18

Page 28: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

^.£. -

9.1 -

9.0-

liftf

or H

ipp

m

00

CO

^ 8.8-co o "E (D

O 8.7-

8.6-

8.5-

8.4-

H20 •

• /

8HI R2 =

\t\

T •

= 1.306H2-1.06 = 0.984, SD = 0.04

y/ktOH

HOAc

r m

TFA

r — ., J

DMSO •

/ "Acetone

»

DMF

7.3 7.4 7.5 7.6 7.7 Chemical shift for H2 ppm

7.8 7.9

Figure 12. Chemical shifts of the aromatic hydrogens Hi and H2 of BMrBF4" in deuterated solvents. (DMF, dimethyl formamide; DMSO, dimethyl sulfoxide; acetone; MeOH, methanol; EtOH, ethanol; HOAc, acetic acid; TFA, trifluoroacetic acid; H2O, water; and AN, acetonitrile)

19

Page 29: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

9.2

9.1 -

9.0-

ppm

X

Shift

le

mic

al

8.9

8.8

8.7 o

8.6-

8.5-

8.4

DMSO

8HI = 1 . 4 0 5 H 3 - 1 . 7 3 R = 0.970, SD = 0.06

MeOH

HOAc

H20

Acetone

DMF

7.2 7.3 7.4 7.5 7.6 7.7

Chemical shift for H3 ppm 7.8 7.9

Figure 13. Chemical shifts of the aromatic hydrogens Hi and H3 of BMrBF4' in deuterated solvents.

20

Page 30: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

7.9

7.8-

7.7-

E Q.

x7 .6 a </)

o 17.5 0 O

7.4-

7.3

6H2 = 1 .096H3 -R = 0.996, SD

-

-

-

^ A N

yH20

1 T"

0.60 = 0.02

MeOH /

/Eton

y/noAc

\ F A

• ' 1 " " T

yoMso

A Acetone

I ' —

>DMF

i

1

7.2 7.3 7.4 7.5 7.6 7.7

Chemical shift for H3 ppm

7.8 7.9

Figure 14. Chemical shifts of aromatic hydrogens H2 and H3 of BMrBF4" in the deuterated solvents.

21

Page 31: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Since the concentrations of the solutions are the same, the chemical shift

variations are deemed to be solvent dependent. If the hydrogens of the ionic

liquid have different solvent dependencies, a plot of the chemical shifts of one

hydrogen versus another in different solvents should have a non-unity slope. If

these hydrogens are affected by solvation similarly, a plot of the chemical shifts

of the hydrogens should have a plot of unity.

Equation 2 shows the relationship that exists between the chemical shifts

of H2 and H3 in BMrBF4' from Figure 14. The goodness of the fit and the

> 2 _ 6H2 = 1 .098H3 - 0.60; R = 0.996, SD = 0.02 (2)

closeness of the slope to unity between these two hydrogens, reveals that the

aromatic hydrogens H2 and H3 are similarly affected by solvation. This

observation is reasonable because of the similar chemical environments for

these two hydrogens.

Similar relationships for the chemical shifts of Hi vs. H2 and Hi versus H3

give different slopes as shown in Equations 3 and 4 and Figures 12 and 13,

respectively. These results are not surprising since Hi is in a different

environment than that of H2 and H3. Hi is located between two electronegative

nitrogen atoms and the expectation is that Hi should be more acidic, and hence,

more sensitive to solvation effects than H2 and H3. The difference in slopes

22

Page 32: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

between Equations 3 and 4 reflects the slighfly different environments of H2 and

H3 owing to the different substltuents bonded to the nitrogen atoms.

8HI = 1 .306H2 - 1.06; R = 0.984, SD = 0.04 (3)

8HI = 1 .408H3 - 1.73; R = 0.970, SD = 0.06 (4)

Table 2 shows the chemical shift values in ppm of the NMR solvent study

conducted with BMrPFa' to evaluate the effect of changing the counterion.

Table 2. H NMR chemical shifts in ppm for the aromatic hydrogens of BMrPFe' in the deuterated solvents.

Solvent

Acetone

Acetonitrile

Acetic Acid

DMF

DMSO

Methanol

Trifluoroacetic Acid

H i

8.88

8.37

8.60

9.20

9.07

8.72

8.63

H2

7.69

7.35

7.48

7.88

7.73

7.54

7.56

H3

7.64

7.32

7.44

7.81

7.66

7.48

7.53

Ethanol and water were not used in these correlations because BMfPFe" is only

partially soluble In these solvents. Once again, diffierent solvents have little

influence on H2 and H3 compared to Hi. The chemical shifts of H2 and Hsshow

minor changes in the different solvents. Hi is more sensitive with a larger

23

Page 33: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

chemical shift range and shifts farther downfield in the more polar deuterated

solvents. The chemical shift of Hi in the polar DMF is 9.20 ppm; whereas H2 and

H3 are shifted to 7.88 and 7.81, respectively.

Figures 15,16, and 17, are plots of the chemical shift data for BMI* PFe".

Equation 5 shows the relationship between H2 and H3 for BMI* PFe".

)2^ 8H2 = 1 .088H3 - 0.56; R = 0.998, SD = 0.01 (5)

Since the slope is approximately unity, the indication is that the different solvents

affect H2 and H3 similarly. With the goodness of the fit and the closeness of the

slope to unity between the two hydrogens, reveals that the aromatic hydrogens,

H2 and H3 have similar solvation effects. Since the slope shown in Equation 5 is

similar to that for the BMrBF4" (Equation 3), these hydrogens for both salts

exhibit similar sensitivity to solvation effects.

24

Page 34: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

9.3 T

9.2 -

9.1 -

9 . 0 -

E Q.

^ 8.9 H

1 8.8-1 (/}

"TO o

I 8.7 o

8.6-

8.5-

8.4-

8.3 7.3

DMF

8HI = 1 . 6 1 8 H 2 - 3 . 4 4 R = 0.982, SD = 0.06 DMSO

MeOH

HOAc

• Acetone

7.4 7.5 7.6 7.7 Chemical shift for H2 ppm

7.8 7.9

Figure 15. Chemical shifts of the aromatic hydrogens Hi and H2 of BMrPFe" in deuterated solvents.

25

Page 35: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

9.25

9.15-

9.05-

8.95 E Q. Q.

^ 8.85 o

sz </)

S 8.75 E

JCZ

O

8HI = 1 . 7 2 8 H 3 - 4 . 2 0 R2 = 0.969, SD = 0.08

8.65-

8.55-

8.45-

8.35

DMSO

Acetone

MeOH

HOAc

7.3 7.4 7.5 7.6 7.7 Chemical shift for H3 ppm

DMF

7.8 7.9

Figure 16. Chemical shifts of the aromatic hydrogens Hi and H3 of BMrPFe' In the deuterated solvents.

26

Page 36: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

7.9 T

7.8-

8H2= 1.088H3-0.56 R2 = 0.998, SD = 0.01

DMF

7.7-1 E Q.

CN

X a I 7.6 15 o E 0)

O 7.5

7.4-

7.3 7.3

DMSO

Acetone

MeOH^/ TFA

HOAc

— I 1 1 1 —

7.4 7.5 7.6 7.7 Chemical shift for H3 ppm

— I —

7.8 7.9

Figure 17. Chemical shifts of the aromatic hydrogens H2 and H3 of BMfPFe' in the deuterated solvents.

27

Page 37: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

For BMr PFe", Equations 6 and 7 and Figures 16 and 17 show the

relationships for Hi vs. H2 and Hi vs. H3, respectively. Hi is in a different

environment than that of H2 and H3, being located between two electronegative

8HI = 1 .618H2-3 .44 ; R^ = 0.982, SD = 0.06 (6)

8HI = 1 .728H3 - 4.20; R = 0.969, SD = 0.08 (7)

nitrogen atoms in the ring. Based on the magnitude of the slopes, the implication

is that the chemical shift of Hi is approximately 1.6 times more sensitive to

changes in solvent properties, compared to H2 and 1.7 times more sensitive than

H3.

28

Page 38: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

18.

The comparison of slopes for BMrPFe" and BMrBF4" is shown in Figure

1.30

BF, PF,

Figure 18. Slope comparison of BMrBF4' and BMrPFe'.

The slopes of H2 vs. HI and H3 vs. HI for BMrBF4', are different from those for

BMrPFe", the anion is noted to play a role in the chemical shift variation of Hi for

both compounds. The slopes of BMrPFe" are larger than the slopes of BMrBF4".

The implication is that Hi of BMrPFe' is more sensitive to a change in the nature

of the solvent compared to BMrBF4'. Typically, the formation of hydrogen bonds

from basic solvents to acidic hydrogens,^such as Hi, Influences the chemical

shifts of the hydrogen; hydrogen bond to an acidic hydrogen from the solvent

shifts the hydrogen downfield.^ The size of the anion may play a role in the

sensitivity difference between BF4" and PFe". PFe" is larger than BF4". The larger

size makes the distance of interaction of PFe" with Hi greater, allowing for more

interaction with the solvent.

29

Page 39: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Table 3 shows the chemical shifts of the aromatic hydrogens of 1-

hexadecyl-3-methylimidazolium tetrafluoroborate, HDMrBF4". The data in Table

Table 3. H NMR chemical shifts in ppm for the aromatic hydrogens of HDMrBF4"in deuterated solvents.

Solvent Acetic acid Acetone Acetonitrile DMF DMSO Chloroform Methanol Trifluoroacetic Acid

Hi 9.02 9.07 8.39 9.29 9.07 8.52 8.76 8.42

H2 7.74 7.78 7.35 7.94 7.74 7.30 7.52 7.28

H3 7.72 7.72 7.32 7.86 7.68 7.27 7.45 7.26

3 show that the different solvents have little influence on H2 and H3 in comparison

to Hi. The chemical shifts of H2 and H3are smaller in the different solvents;

whereas, Hi is more sensitive. The more polar the deuterated solvent, the more

downfield Hi shifts. Hi shifts to 9.29 ppm in polar DMF solvent, while H2 and H3

are shifted to 7.94 and 7.86, respectively.

Figures 19, 20, and 21 are plots of the chemical shift data for the aromatic

hydrogens of HDMrBF4".

30

Page 40: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

9.4

9.2

9.0 ]

E QL Q.

X a ^ 8.8 sz <t) 15 o E 0) sz O 8.6 -

8.4

8.2

-

-

TFA ......J

-,...,_

6HI = 1 . 3 9 6 H 2 - 1 . 7 4 R2 = 0.98; SD = 0.04

/ M B O H

• / / C D C I 3

• AN

- 1 1 1

DMF A

DMSO / • y^ Acetone

/ HOAc

J i

I I • • • ! - • • i

7.2 7.3 7.4 7.5 7.6 7.7 7.8

Chemical shift for H2 ppm

7.9 8.0

Figure 19. Chemical shifts of the aromatic hydrogens Hi and H2 of HDMrBF4" in the deuterated solvents.

31

Page 41: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

9.4

9.3

9.2

9.1 -

E9.0 Q. Q.

^8.9

sz <n 158.8 o "E (D

08.7

8.6

8.5

8.4

8.3

DMF

6HI = 1 .436H3 ~ 1.97 R = 0.97; SD = 0.06

MeOH

CDC 13

DMSO

7.2 7.3 7.4 7.5 7.6 7.7

Chemical shift for H3 ppm

7.8 7.9

Figure 20. Chemical shifts of the aromatic hydrogens Hi and H3 of HDMrBF4" in the deuterated solvents.

32

Page 42: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

8.0

7.9

7.8

& 77 CM

X

1 7.6 </)

15 o

7.4

7.3

7.2

-

6H2= 1 . 0 6 6 H 3 - 0 . 4 1 R = 0.994; SD = 0.02

DMSO

MeOH /

y/AN

/CDCI3 •

TFA

1 1

• DMF

X Acetone

HOAc

1

7.2 7.4 7.6 7.8

Chemical shift for H3 ppm

8.0

Figure 21. Chemical shifts of the aromatic hydrogens H2 and H3 of HDMrBF4' in the deuterated solvents.

33

Page 43: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

HDMrBF4" was soluble in ethanol only at elevated temperatures;

therefore, ethanol was not used in the correlations. From the data in Figures 18,

19, and 20, H2 and H3 appear to be affected similarly by the different solvents,

while Hi seems to have a larger chemical shift variation.

Equation 8 shows the relationship that exists between the chemical shifts

of H2 and H3 for HDMrBF4" from Figure 20.

. 2 _ 8H2 = 1 .068H3 - 0.41; R = 0.994, SD = 0.02 (8)

The closeness to unity of the slope and the goodness of the fit between

the two hydrogens indicates that the aromatic hydrogens, H2 and H3 are similarly

affected by solvation as HDMrBF4"and HDMI PFe". This observation is

reasonable because of the chemical environments that these two hydrogens

occupy. Relationships for the chemical shifts of Hi versus H2 and Hi versus H3

give non-unity slopes as shown in Equations 9 and 10 and Figures 18 and 19.

8HI = 1 .398H2 - 1.74; R = 0.98, SD = 0.04 (9)

8HI = 1-438H3 - 1.97; R = 0.97, SD = 0.06 (10)

34

Page 44: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Chemical shift data for the aromatic hydrogens of HDMrPFe' in various

deuterated solvents are given in Table 4.

Table 4. H NMR chemical shifts in ppm for the aromatic hydrogens of HDMrPFe" in the deuterated solvents.

Solvent Acetic Acid Acetone Acetonitrile Chloroform DMSO DMF Methanol Trifluoroacetic Acid

Hi

8.81 9.00 8.43 8.55 9.07 9.28 8.76 8.14

H2

7,48 7.73 7.36 7.25 7.73 7.93 7.50 7.05

H3

7-46 7.67 7.33 7,24 7.67 7.86 7.44 7.02

HDMrPFe" was only soluble In ethanol at elevated temperatures so this solvent

was not used in the correlations. According to the data, the different solvents

have little influence on H2 and H3 in comparison to Hi. From Table 4, it is

obvious that the chemical shifts of the aromatic hydrogens of HDMrPFe' are

solvent dependent, with Hi showing to have greater dependency in comparison

to H2 and H3. The deuterated solvents that are more polar, such as DMF, shift H-

further downfield in comparison to a less polar solvent such as acetonitrile.

Figures 22, 23, and 24 are the plots of the chemical shift data for

HDMrPFe".

35

Page 45: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

9.4

9.2

9.0 -

E Q. CL

5 8.8

x : CO

15 .y 8.6 E x: O

8.4 -

8.2

8.0

-5HI = 1 .256H2 - 0.63 R = 0.96; SD = 0.06

HOAc / • /

y^MeOH

CDCI3 /

/ •AN

• TFA

1 1 1

DMF

DMSO / ^ /

/ • / Acetone

1

1

7.0 7.2 7.4 7.6

Chemical Shift for H2 ppm

7.8 8.0

Figure 22. Chemical shifts of the aromatic hydrogens Hi and H2 of HDMrPFe' in the deuterated solvents.

36

Page 46: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

9.4

9.2

9.0

E Q. Q.

^ 8.8 o

CO

"co 8.6 o "E <D

O 8.4

8.2

8.0

- 6HI = 1 .346H3 - 1.25 R = 0.97; SD = 0.04

"

HOAc • y

# /

DMSO X

/ Acetone

XMeOH

CDCI3 / • X X •

X AN

• TFA

1 1 1 I

DMF

1 1 1

7.0 7.2 7.4 7.6 7.8

Chemical Shift for H3 ppm

8.0

Figure 23. Chemical shifts for the aromatic hydrogens Hi and H3 of HDMrPFe" in the deuterated solvents.

37

Page 47: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

8.0

7.9

7.8 -

7.7

§: 7.6 H Csl

X a 7.5

CO

(Q

o E 0)

6

7.4 -

7.3

7.2

7.1

7.0

6.9 6.9

6H2 = 1 .066H3 - 0.43 R = 0.997; SD = 0.02

TFA

7.1

Acetone

DMSO

MeOH

DMF

HOAc

7.3 7.5 7.7

Chemical Shift for H3 ppm

7.9 8.1

Figure 24. Chemical shifts for the aromatic hydrogens H2 and H3 of HDMrPFe" in the deuterated solvents.

38

Page 48: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Equation 11 shows the unity that exists between H2 and H3. The similar

environments of H2 and H3 are influenced In the same way by the change in

solvent.

6H2 = 1 .066H3 - 0.43; R = 0.997; SD = 0.02 (11)

The relationship between Hi and H2 gives a different slope than the relationship

between Hi and H3, as seen in Equations 12 and 13.

6HI = 1 .256H2 - 0.63; R = 0.96; SD = 0.06 (12)

6HI = 1 .346H3 - 1.25; R = 0.97; SD = 0.04 (13)

Equations 12 and 13 show that Hi is affected slightly differently from H2 and H3.

Based on the magnitude of the slopes, the implication is that the chemical shift of

Hi is approximately 1.2 times more sensitive to changes in solvent properties,

compared to H2 and 1.3 times more sensitive than H3. The small difference in

slope can be a result of the large size of PFe" and the bent side arm decreasing

the solvent interactions.

39

Page 49: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

The comparison of the slopes of HDMrPFe" and HDMrBF4"is shown in

Figure 25. The smaller slopes of HDMrPFe" compared to HDMrBF4" happens

due to the large size of the PFe" and the orientation of the bulky side chain in

which both are hindering the interaction of the solvent with Hi.

1.39

Figure 25. Slope comparison of HDMrBF4" and HDMrPFe'

The use of the different anions and side arms plays a role in the

solute/solvent interaction of the ionic liquids. Figure 26 illustrates the difference

in slope for BMrBF4", BMrPFe", HDMrBF4', and HDMrPFe". The slopes of

BMrBF4", HDMrBF4", and HDMrPFe" range from 1.2 to 1.4, revealing that the

solute/solvent Interactions for these ionic liquids behave similariy in the same

environments. The slopes of 1.6 and 1.7 for BMrPFe" reveal that this ionic liquid

has the greatest solute/solvent interaction.

40

Page 50: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

BF, PF,

1.39

Figure 26. Slope comparison of BMrBF4", BMrPFe", HDMrBF4", and HDMrPFe".

41

Page 51: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Nature of the Solvent Interactions

The H NMR spectroscopic investigations give insight into possible

interactions of the anion with the cation and the solvent. The relationships

between two anions, PFe" and BF4" were studied along with altering the side

chain from a butyl to a hexadecyl. Figure 27 shows possible interaction of the

solvent with the anion and/or the cation. The proposed interaction between

CM 41^9

+ 'i">—Hl""'X""""H-sol

sol-H»»«'»>X"»«»»H3

H-C.H

/ 4^9

By-sol-H»»'»»»X"»»»"»H2

C4H9

N

CH-

Figure 27. Proposed interaction between the BMI* cation and the acidic solvent. X" = BF4" or PFe".

the anion and the solvent via hydrogen bond from the acidic solvents to the basic

anion could account for the slight chemical shift change of the protons as noted

for H2 and H3.

42

Page 52: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Figure 28 shows the possible solvent interacfions between the solvent and

the acidic hydrogens of the cation incorporated with the interaction of the anion.

C Hc

Figure 28. Proposed interaction between the BMr cation and the basic solvent. X" = BF4' or PFe".

The interaction between the solvent and the acidic hydrogens of the cation could

account for the difference in the slopes of the BF4" versus the PFe" anions. The

slope for PFe" is 0.30 greater than for BF4" of Hi indicating that the interaction of

PFe" with the cation may be a greater distance, thus allowing for more solvent

interaction with Hi. The smaller slope of Hi for BF4' indicates a closer interaction

of the anion with the cation giving less interaction for the solvent.

43

Page 53: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

The role of the side arm may be more significant with the HDMI* cation

with regard to the orientation of the side arm. Solvent interaction with the cation

and anion is shown in Figure 29.

P16H33

))—HV"'X'"""H-sol

CH

N u N sol-H"""X"i""»H2 \ • 2 V u CH.

^ CifiHo-a sol-H'»«'»X"»«»«»H3 / ^^ ' '

CH3

Figure 29. Proposed interaction between the HDMI* cation and the acidic solvent. X" = BF4" or PFe".

H2 and H3 have only slight chemical shifts in the different solvents and may be

attributed to the close interaction of the anion with the cation not allowing for

interaction with the solvent. The slope of unity for H2 and H3 Is consistent with

their similar solvent effects.

44

Page 54: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Interaction of the solvent with the cation is illustrated in Figure 30. The

interaction of Hi with the anion and the different solvents is influenced by the

H3 ..^'^"^\. H3 .P'^"''

Hf ^ ' °l CH3

\

sol:

'''u P 16 33

2 CH3

Figure 30. Proposed interaction between the HDMr cation and the basic solvents. X" = BF4" or PFe".

saturated alkyl chain. With the BF4" anion of HDMI*, the slopes are essentially

the same as with the BMrBF4" but HDMrPFe" is different from BMfPFe" based

on the slope being closer to unity. The long side chain of HDMrPFeis in a

dynamic equilibrium where the chain does not stay in one position, but flops back

and forth. From the results, the bulky alkyl side chain is oriented toward Hi more

than H3. The lower slope of HDMTPFe" gives evidence that the side chain is

blocking solvent interaction as the interaction of PFe" with Hi blocks the other

side preventing a greater solvent dependence.

45

Page 55: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Use of SolvatochromIe Parameters to Analvze the Solvation Interactions of BMrBFz"

Another way to consider how the properties of ionic liquids are affected by

a change of the anion or the side chain is the use of the Kamlet-Taft equation.

Equation 14 is used to analyze the solute-solvent Interactions that affect the

chemical shifts (8AH) of BMIC in different solvents. 6AH represents changes in

chemical shift and n*, a, and p are the solvent's dipolarity-polarizability, hydrogen

bond donor ability, and hydrogen bond acceptor ability, respectively, and 8AHois

the intercept.

8AH = 571* + aa + /)P + 8AHO (14)

The extent and importance of the different solute-solvent interactions are

obtained fi'om the sign and magnitude of the coefficients s, a, and b, wherein a

negative value implies a favorable interaction between the solute and solvent and

a positive value implies the opposite. For the solvation property, the magnitude

and sign of the coefficients reflect the relative importance of the solvent-solute

interaction.

DMF>DMSO>CH3C02H>CDCl3>MeOH>D20>CH3CN is the polarity trend

of the solvents used. Solvent acidity is a product of the coefficient a in Equation

14. Protic solvents interact with solutes that have basic sites. This interaction is

created by the formation of hydrogen bonds between a solvent molecule and a

46

Page 56: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

solute molecule. The effectiveness of such hydrogen bonds depends on the

ability of both solvent and solute molecules to approach close enough to allow

interaction of the hydrogen.

Table 5 presents the solvent parameters for the solvents used for the

regression equations.^ The contribution of TT* is typically much less than a

and p parameters because the polarizability effect is highly attenuated in the

solution phase. Therefore, a two-parameter equation was considered in this

research.

Table 5. SolvatochromIe Parameters.

Solvent rr 0 g DMSO

DMF

Acetonitrile

Acetone

Acetic Acid

Methanol

Ethanol

Water

1.00

0.88

0.75

0.72

0.62

0.60

0.54

1.09

0.00

0.00

0.15

0.07

1.09

0.98

0.86

1.13

0.76

0.69

0.37

0.48

0.00

0.62

0.77

0.18

Although the numbers look promising, the standard deviations show that

the regression equations are not reliable. To get reliable relationships, the rule of

thumb is, the number of solvents should be three times the number of

parameters being calculated. With this in mind, the equations are considered not

reliable due to an insufficient number of solvents analyzed. None the less, they

can give an indication of the nature of any solute/solvent interactions.

47

Page 57: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

The regression analysis was performed first with all three coefficients and

without a significant contribution from TT*, the regression analysis was performed

without the TT* resulting in Equations 15, 16, and 17.

Regression equations without the TT* variable for BMrBF4" are:

8HI = 8.63-0.17a+ 0.47P (15)

8H2 = 7.51-0.17a+ 0.32P (16)

8H3 = 7.48 - 0.17a + 0.26p. (17)

Solvent basicity is a product of the coefficient b in Equation 14. Basic solvents

form hydrogen bonds to acidic sites of solutes. From the equations, the

magnitude of the coefficient b for the basicity property of the salt is similar for H2

and H3, but different for Hi. Since Hi is bonded to a carbon, which is bonded to

two nitrogen atoms, it is expected that Hi should be more sensitive to solvent

effects. The similarity of the coefficients for H2 and H3 indicates a similar

interaction between the solvent and these hydrogens. The different

environments of H2 versus H3 result in the slightiy different coefficients.

48

Page 58: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Table 6 shows the standard deviations and n represents the number of

solvents used.

Table 6. Coefficients and statistics using equation 14 without polarizability (TT*) for BMrBF4".

Constant a b R n SD

8H1 8.63 + 0.12 -0.17 + 0.11 0.47 + 0.20 0.580 7 0.17

8H2 7.51+0.10 -0.17 + 0..08 0.32 + 0.15 0.590 7 0.13

8H3 7.48 + 0.09 -0.17 + 0.08 0.26 + 0.14 0.580 7 0.12

Analysis of the Solvent Interactions of BMrPFe"

To see the significance of the anion contribution on the properties,

BMrPFe". Figure 31 shows the aromatic hydrogens of BMrPFe" and shows the

interaction between the solvent and the acidic hydrogens of the cation, along with

the interaction with the anion.

49

Page 59: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Again the equations using all three coefficients resulted in polarizability effect not

being significant. Because the polarizability values showed no significant

dependability or statistical significance, these values were not retained.

Figure 31. Aromatic hydrogen designation for BMrPFe"

This observation is not surprising since BMrPFe" is a polar compound and

solvation by this mode should not play a major role in the solvation of these

compounds since the polar interaction between the anion and the cation of the

salt should be much stronger than the interaction with the solvent.

The regression analysis was performed without the TT* values resulting in

Equations 18, 19, and 20.

Regression equations computed for Figure 15 without n* values:

8HI=8 .48 -0 .06a+ 0.73P (18)

8H2=7.45 - 0.07a + 0.40p (19)

8H3=7.42 - 0.08a + 0.34p. (20)

50

Page 60: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Solvent basicity is a product of the coefficient b in Equation 14. Basic solvents

form hydrogen bonds to acidic sites of solutes. From the equations, the

magnitude of the coefficient b for the basicity property of the salt are similar for

H2 and H3, but different for Hi. Since Hi is bonded to a carbon that is between

two electronegative nitrogen atoms, it is expected that Hi should be more

sensitive to solvent effects. The similarity of the coefficients for H2 and H3

indicates similar Interactions between the solvent and these hydrogens. Hi has a

higher b coefficient than that of BMrBF4'. This is because of the larger size of

the PFe" anion creating a greater distance for the interaction with Hi, allowing for

a greater interaction witfi the solvent.

Table 7 shows the standard deviations and n represents the number of

solvents used for the calculations.

Table 7. Coefficients and statistics using equation 14 without polarizability (Tt*) for BMrPFe".

Constant a b R n SD

8H1 8.48 + 0.34 -0.06 + 0.28 0.73 + 0.51 0.541 6 0.27

8H2 7.45 + 0.22 -0.07 + 0.19 0.40 + 0.33 0.498 6 0.18

8H3 7.42 + 0.21 -0.08 + 0.17 0.34 + 0.32 0.477 6 0.17

51

Page 61: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Analysis with Gaussian 94 for Imidazolium Cations

Charge distribution on the atoms of the imidazolium cation contributes to

the physical properties of the ionic liquid. Varying the side arm is one way to

compare the charge distribution, by using the Gaussian 94 program. Gaussian

94 using standard basis sets with no modification^^ was executed to prepare the

ab initio calculations. Ail calculations were performed on a Silicon Graphics

Indigo computer. Conformations were optimized at each level of theory.

Convergence was to the limits imposed internally by Gaussian 94. Vibrational

frequencies were calculated at each level of theory and the results were used to

determine the nature of the conformations

Figure 32 shows the numbering system used for the imidazolium cation

calculations.

Ci C9

Hs 94 He

^10

Figure 32. Numbering system for imidazolium cation.

52

Page 62: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Table 8 shows the z-matrix placed in the Gaussian equations to produce

the charge distribution.

Table 8. Z-Matrix for imidazolium cation of Figure 31.

Atom Bond BondLenqth Anale C(1) C(2) C(1) N(3) C(2) C(4) N(3) N(5) C(1) H(6) C(1) H(7) C(2) H(9) N(3) H(10) C(4) H(8) N(5)

1.341 1.382 1.314 1.382 1.068 1.068 1.000 1.070 1.000

C(1) C(2) C(2) C(2) C(1) C(2) N(3) qi)

First Angle Third Atom Second Angle

106.478 109.552 106.477 131.288 131.286 125.754 126.029 125.751

C(1) N(3) N(3) N(5) C(1) 0(2) C{2)

0.000 0.000

179.684 -180.000 180.000 180.000 180.000

Angle T

Dihedral Dihedral Dihedral Dihedral Dihedral Dihedral Dihedral

Bond lengths, bond angles, and dihedral angles are the descriptions given for the

molecular geometry that is collectively known as the Z-matrix. The identity and

position of a general atom are specified by the Z-matrix.

53

Page 63: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Table 9 shows the relative charge distribution for the imidazolium cation.

Table 9. Charge distribution of atoms on the imidazolium cation.

t

1

2

3

4

5

6

7

8

9

10

Atom

C

C

N

C

N

H (H2)

H (H3)

H

H

H (Hi)

Sto-3g

0.067613

0.067604

-0.257026

0.260872

-0.257013

0.155994

0.156031

0.309131

0.309134

0.187660

RHF/3-21g

0.069705

0.068701

-0.884550

0.616498

-0.884552

0.360563

0.360563

0.450179

0.450179

0.391713

RHF/6-31g*

0.027307

0.027307

-0.684162

0.407426

-0.684163

0.315867

0.315867

0.470660

0.470660

0.333230

RHF/6-31+g*

0.074369

0.074369

-0.595444

0.279707

-0.595444

0.326072

0.326072

0.536161

0.536161

0.335453

The Gaussian numbering system for imidazolium cation is different from

the other calculations done previously In the research. H10, H6, and H7 are

equivalent to the representation of HI, H2 and H3, respectively and are the

atoms that are most important to this study. The level of theory increases as the

columns go fi-om Sto-3g to RHF/6-31+g*. According to tfie data, H6 and H7 have

the same charge throughout the levels of theory which contributes to the

argument that these two hydrogens are essentially the same. H10 has the

greatest postive charge compared to H6 and H7 showing that it Is more sensitive

to changes in the environment.

54

Page 64: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Figure 33 shows the numbering of 1-fluoroimidazolium cation.

H

/ \

H 10

Figure 33. 1-Fluoroimidazolium cation.

Table 10 shows the charge distribution for 1-fluoroimidazolium cation.

Table 10. Charge distribution of atoms of 1-fluoroimidazolium cation.

1 2 3 4 5 6 7 8 9 10

Atom C C N C N H H H F H

(H2) (H3)

(HI)

Sto-3g 0.07450 0.06310 -0.06642 0.25100 -0.25461 0.16270 0.16880 0.31503 0.08578

0.200134

RHF/3-21g 0.06857 0.09182 -0.42569 0.63681 -0.89223 0.37514 0.39110 0.46112 -0.12916 0.422514

RHF/6-31g 0.10171 0.14635 -0.30834 0.60051 -0.87987 0.34281 0.35898 0.47416 -0.21715 0.380857

RHF/6-31g* 0.03440 0.01618 -0.01635 0.38843 -0.70141 0.32852 0.34212 0.47832 -0.22783 0.357625

RHF/6-31+g* -0.11335 -0.01629 0.05691 0.22214 -0.56730 0.33671 0.34699 0.54834 -0.17003 0.355873

55

Page 65: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

The use of 1-fluoroimidazolium cation Is to determine the effect of

electi'onegative groups bonded to the nitrogen, to see how the positive charge of

HI versus H2 and H3 is affected. Similar to imidazolium cation, H10 has the

greater charge over H6 and H7. The charge of H10 for 1-fluorolmdazolium

cation is 0.355873 and H10 for imidazolium cation is 0.335453, which Illustrates

that the fluorine allows for a more positive charge on H10. The fluorine atom

also has an affect on H7 creating different charges for H6 and H7. Varying the

side arm on the cation can have an impact on the properties of the ionic liquid.

Analysis of Solvation Properties of Ionic Liquids bv Theoretical Descriptors

The generalized TLSER equation for solutes in a given medium is shown

in Equation 21:

SSP = aVmc +b7ti + csB +dq- +eeA + fq+ +SSPo. (21)

SSP represents the solute/solvent interactions that cause property variations.

Vmc describes the molecular van der Waals volume (in units of 100 cubic

angstroms, A" ). TIJ describes the dipolarity/polarizability contribution and is

obtained firom the division of the polarizability volume by the molecular volume to

produce a unitiess, size Independent quantity which indicates the ease with

which the electron cloud of a solute may be moved or polarized, SB is part of the

56

Page 66: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

hydrogen bond acceptor basicity (HBAB) contribution and is the energy

difference between the highest occupied molecular orbital (HOMO) of the solute

and the lowest unoccupied molecular orbital of (LUMO) water. Water was

chosen as the reference because it is the most common solvent. The

electrostatic term (q.) Is the largest negative formal charge on an atom of the

solute; the units are atomic charge units (acu). 8A describes the covalent acidity,

which reflects the ability of a solute to act as a Lewis acid. These descriptors are

obtained fi-om the difference between the energies of he LUMO of the solute and

the HOMO of water. q+ is the electrostatic acidity term and is the largest positive

formal charge on an atom of the solute; the units are in acu. SSPo is the

intercept. The coefficients of the MLR equations, a, b, c, d, e, and f, indicate the

significance of the different solute/solvent interactions to the property being

analyzed.

With only four salts examined in this research, a complete TLSER analysis

could not be carried out. These TLSER parameters are very useful in predicting

the abilities of these and other ionic liquids to act as solvents for reactions.

57

Page 67: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Figure 34 is the structure used to analyze different substituents of the

imidazolium cation.

Figure 34. Structure of 1,3-disubstituted imidazolium cation for which theoretical descriptors have been developed. X and Y are shown in Table 11

For many ionic liquids, the sti-ucture of the cations are different while the

anion remains the same. Thus characterization of the cation can be useful in

designing the proper ionic liquid. The TLSER descriptors computed^ for various

1,3-disubstituted imidazolium cations in Table 11 were accomplished using the

MNDO algorithm contained In MacSpartan. ®

58

Page 68: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Table 11. Theoretical descriptors for different ionic liquids and molecular solvents.

Substituted Cation

X=H; Y=H X=H; Y=F X=H; Y=CH3 X=H; Y = C F 3

X=F; Y=CF3 X=F; Y=CH3 X=F; X=F X=CH3; Y = C F 3

X=CH3; Y=CH3 X = C F 3 ; Y=CF3 X^CHs; Y=C4H7 X=CH3;Y=Ci6H3i X=H; Y = 0 C H 3

X=0CH3; Y=0CH3 X=H; Y=SiMe3 X=SiMe3; Y=SiMe3

Molecular solvents

Benzene CH2CI2 CHCI3 THF Acetone water MeOH EtOH EG DMSO AN

Vmc

70.417 76.317 88.432

104.228 110.126

94.341 82.210

122.255 106.434 138.085 158.926 368.808

97.845 125.276 152.686 234.837

Vmc

86.893 58.898 73.455 80.609 67.969 20.478 38.558 56.073 65.172 75.295 49.110

7Ci

0.1094 0.1045 0.1111 0.0948 0.0925 0.1071 0.1004 0.0985 0.1126 0.0879 0.1121 0.1101 0.1103 0.1190 0.1127 0.1142

TCi

0.1173 0.1106 0.1210 0.0999 0.0922 0.0549 0.0814 0.0893 0.0869 0.0980 0.1182

es

0.0959 0.0908 0.0981 0.0921 0.0874 0.0931 0.0784 0.0942 0.1000 0.0889 0.1013 0.1166 0.0962 0.0966 0.1021 0.1069

SB

0.1517 0.1344 0.1310 0.1378 0.1380 0.1237 0.1314 0.1324 0.1372 0.1540 0.1425

q-

0.1749 0.1688 0.2084 0.3124 0.3077 0.2027 0.0289 0.3145 0.2111 0.3039 0.2121 0.2116 0.1764 0.1461 0.3378 0.3474

q-

0.0593 0.1183 0.0723 0.3277 0.2839 0.3256 0.3292 0.3234 0.3276 0.7146 0.3422

EA

0.2305 0.2367 0.2285 0.2360 0.2415 0.2342 0.2427 0.2339 0.2267 0.2405 0.2254 0.2252 0.2312 0.2316 0.2242 0.2196

EA

0.1744 0.1702 0.1783 0.1471 0.1714 0.1237 0.1402 0.1442 0.1455 0.1615 0.1903

q+

0.2738 0.2826 0.2707 0.2800 0.2229 0.2075 0.2320 0.1989 0.1831 0.2133 0.1817 0.1817 0.2742 0.2043 0.2642 0.1686

q+

0.0593 0.0642 0.1030 0.0209 0.0233 0.1628 0.1803 0.1784 0.1875 0.0564 0.0951

59

Page 69: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

From the Table 11, it is obvious that as groups are added to the imidazolium

cation, the size of the cation increases. For effective solvation of some solutes,

especially dipolar molecules, solvents must gain access between the lines of

forces of these molecules and large solvents cannot effectively solvate such

solutes. Depending on the nature of the group added to the imidazolium cation,

the polarizability is affected differentiy. The addition of electronegative groups,

such as fluorine or the trifluoromethyl groups, decreases the polarizability,

relative to the imidazolium cation. Polarizbility effect is typically highly attenuate

in the condensed phase, compared to the gas phase and as a result, this factor

may not play a major role in solute/solvent interactions involving ionic liquids. By

changing the groups on the imidazolium cation, the ability to accept electrons

Increases slightiy only by adding electron donating groups. These numbers

indicate that the electron donating groups can only slightiy influence the

imidazolium cation's acceptability. An important solvation property for solvents in

the ability to donate electrons to the solute. It is obvious that the cation will not

be good at participating in this type of solute/solvent interaction. From Table 11,

EB only ranges as high as 0.1 and as low as 0.07 compared to molecular solvents

that range from 0.15 to 0.12. A similar observation is made for the most

negative atom on the imidazolium cation, and groups such as the trifluoromethyl

group, the negative charge is apparentiy pulled out to the fluorine. Of all the

solvent properties, the ability to accept a pair of electrons, changes of the groups

of the imidazolium cations have a tremendous effect. From Table 11, the

60

Page 70: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

substituted cations range from 0.24 to 0.21 and the molecular solvents range

from only 0.19 to 0.12. A solvent that comes close to this is nitrobenzene. On

the other hand, the most positive atom of the imidazolium cations is increased by

adding the electronegative groups to the imidazolium cations. Therefore, by

taking a look at the influence of the side arm on the cation is useful in predicting

the cation's properties.

61

Page 71: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

CHAPTER ill

CONCLUSIONS

The physical properties and solute/solvent interactions of ionic liquids can

be varied by changing the anion and/or the length of the side chain to fit specific

requirements. The solute/solvent interactions of BMrBF4" versus HDMrBF4" are

not affected significantiy by the different side chains. On the other hand, the

solute/solvent interactions of BMrPFe" versus HDMrPFe'are affected

significantiy by the difference in the side chain. By allowing the anion to remain

the same, theorectical properties of tiie cation can be predicted by varying the

character of the side chain. By studying the properties of the Ionic liquids, the

use of ionic liquids can be tuned to meet specific requirements as a solvent for

reactions.

62

Page 72: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

CHAPTER IV

EXPERIMENTAL SECTION

Preparation of 1-Methvl-3-propvllimidazolium Chloride

In an oven-dried round bottom flask, 1-chloropropane (2.50 g, 0.0318 mol)

was added to 1-methylimidazole (2.10 g, 0.0256 mol). The mixture was attached

to a reflux condenser and placed in a silicone oil bath heated to approximately

50 °C. The reaction was allowed to stir and heat at approximately 50 °C for 48

hours. The resulting light yellow solution was cooled to room temperature and

washed 3 times with 10 mL portions of ethyl acetate. The excess ethyl acetate

was removed under vacuum using the ft-eeze/thaw method; H NMR (CDCI3, 200

MHz) 6 10.42 (1H, s), 7.55 (1H, s), 7.43 (1H, s), 4.21 (2H, t), 4.03 (3H, s), 1.85

(2H, sex), 0.89 (3H, t);

Preparation of 1-Butvl-3-methvlimidazolium Chloride

In an oven-dried round bottom flask with a stirring bar, 1-chlorobutane

(5.00 g, 0.0540 mol) was added to 1-methylimidazole (4.00 g, 0.0487 mol). A

reflux condenser topped with a drying tube of calcium chloride was attached and

the assembled apparatus was placed in a silicone oil bath. The clear mixture

was stirred and heated at 70 °C for 48 hours. The resulting, tan color viscous

liquid was allowed to cool to room temperature and then was washed three times

with 20 mL portions of etfiyl acetate. After the last washing, the remaining ethyl

acetate was removed under vacuum at approximately 70 °C; IR (NaCI) v 3139-

63

Page 73: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

2872, 1570, 1171 cm-1; H NMR (CDCI3, 200 MHz) 6 10.04 (1H, s), 7.57 (1H, s),

7.42 (1H, s), 4.18 (2H, t). 3.95 (3H, s), 1.73 (2H, q), 1.19 (2H, sex), 0.78 (3H, t);

Preparation of 1-Butvl-3-methvlimidazolium Hexafluorophosphate

In an oven-dried round bottom flask with a stirring bar,

hexafluorophosphoric acid (2.00 g, 0.0164 mol) was added dropwise, to prevent

a significant temperature increase, to a mixture of 1-butyl-3-methylimidazolium

chloride (2.00 g, 0.0115 mol) in 10 mL of distilled water. The light tan mixture

was allowed to stir at room temperature for 48 hours. The upper acidic layer was

decanted and the lower ionic liquid was washed ten times with 20 mL of distilled

water or until the washings were no loner acidic. Acidity was tested with pH

paper. The resulting brown liquid was placed under vacuum at approximately

70°C to remove excess water. To ensure that the water was removed, a freeze-

thaw method was used. Under vacuum, the solution was quickly frozen with

liquid nitrogen and then thawed using a heat gun; H NMR (CDCI3, 200MHz) 6

8.35 (1H, s), 7.30 (2H, d). 4.08 (2H, t), 3.82 (3H, s), 1.82 (2H, q), 1.25 (2H, sex)

0.84 (3H,t); IR: 3169 and 3125 [vC—H) aromatic], 2966, 2939 and 2876 [v(C—

H) aliphatic]; 1573 and 1468 [v(C==C)l; 841 [v(PF)] cm"''. d= 1.36 g/cm^

Preparation of 1-Butvl-3-methvlimidazolium Tetrafluoroborate

In an oven-dried round bottom flask with a stirring bar, sodium

tetrafluoroborate (2.0o g, 0.0182 mol) was added to a mixture of 1-butyl-3-

methylimidazolium chloride (2.0o g, 0.0115 mol) in 10 mL of acetone. The light

64

Page 74: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

brown mixture was allowed to stir at room temperature for 48 hours. The

resulting gold color liquid was filtered through a plug of Celite. To remove the

excess acetone, the liquid under vacuum was heated to approximately 50 °C; H

NMR (CDCI3, 200 MHz) 6 8.65 (1H, s), 7.41 (2H, d), 4.13 (2H, t), 3.85 (3H, s),

1.79 (2H, q), 1.28 (2H, sex), 0.89 (3H, t); IR; 3166 and 3121 MC—H) aromatic];

2967, 2941, and 2883 [v(C—H) aliphatic]; 1575 and 1472 MC==C)]; 1061

MBF)]cm"V c/=1.21 g/cm^

Preparation of 1-Methvl-3-pentvllimidazolium Chloride

In an oven-dried round bottom flask, 1-chloropentane (2.90 g, 0.0272 mol)

was added to 1-methylimidazole (2.20 g, 0.0268 mol). The mixture was attached

to a reflux condenser and placed in a silicone oil bath. The reaction was allowed

to stir and heat at approximately 70 °C for 48 hours. The resulting light green

solution was allowed to cool to room temperature and then washed with 10 mL

portions of ethyl acetate three times. After the last washing, the excess ethyl

acetate was removed under vacuum by heating to approximately 70 °C.

Preparation of 1-Octvl-3-methvlimidazolium Chloride

In an oven-dried round bottom flask, 1-chlorooctane (4.00 g, 0.0269 mol)

was added to 1-methylimidazole (2.00 g, 0.0244 mol). The mixture was

assembled to a reflux condenser and placed in a silicone oil bath. The reaction

was allowed to stir and heat to approximately 70 °C for 48 hours. The resulting

light gold solution was allowed to cool and then washed three times with 10 mL

65

Page 75: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

portions of ethyl acetate. After the final wash, the excess ethyl acetate was

removed under vacuum by heating to approximately 70 °C. H NMR (CDCI3, 200

MHz) 6 10.16 (1H, s), 7.56 (1H, s), 7.35 (1H, s), 4.19 (2H, t), 3.99 (3H, s), 1.77

(2H, m), 1.12 (10H,m), 0.70 (3H,t);

Preparation of 1-Hexadecvl-3-methvlimidazolium Bromide

In an oven-dried round bottom flask, 1-bromohexadecane (22.40 g,

0.0734 mol) was added to 1-methylimidazole (6.00 g, 0.0731 mol). The mixture

was attached to a reflux condenser, placed in a silicone oil bath and heated to

140°C during a period of 10 minutes. An exothermic reaction in the latter stages

of heating produces an emulsion that disappears after a few minutes resulting in

a brown viscous liquid. Upon cooling the reaction a brown solid formed.

Preparation of 1-Hexadecvl-3-methvlimidazolium Tetrafluoroborate

In an oven-dried round bottom flask, sodium tetrafluoroborate (2.00 g,

0.0182 mol) was added to 1-hexadecyl-3-methylimldazolium bromide (4.00 g,

0.0103 mol) dissolved in 20 mL of acetone and allowed to stir for 48 hours. The

resulting mixture was filtered through a plug of celite. To remove the excess

acetone, the liquid under vacuum was heated to approximately 50 °C. The

resulting yellowish solid was dried under vacuum overnight. H NMR (CDCI3, 200

MHz) 5 8.81 (1H, s), 7.34 (1H, s), 7.27 (1H. s), 4.14 (2H, t), 3.89 (3H, s), 1.84

(2H, m), 1.22 (26H, m), 0.85 (3H, t); m. p. 155 °C

66

Page 76: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

Preparation of 1-Hexadecvl-3-methvlimidazolium Hexafluorophosphate

In an oven-dried round bottom flask, hexafluorphosphoric acid (2.40 g,

0.0164 mol) was added to 1-hexadecyl-3-methylimidazolium bromide (4.00 g,

0.0103 mol) dissolved in 20 mL of acetone and allowed to stir for 48 hours. The

resulting mixture was filtered through a plug of celite. To remove the excess

acetone, the mixture under vacuum was heated to approximately 50 °C. The

resulting yellowish solid was dried under vacuum overnight. H NMR (CDCI3, 200

MHz) 6 8.56 (1H, s), 7.25 (1H, s), 7.24 (1H, s), 4.02 (2H, t), 3.79 (3H, s), 1.73

(2H, m), 1.12 (26H, m), 0.74 (3H, t); m. p. 163°C

Preparation of NMR Solvent Studv Samples

Each NMR sample was prepared in a glove box that was flushed out with

nitrogen gas. The ionic liquid was measured out and the appropriate solvent was

added to make consistent concentration of 0.45 mol/L. The samples were

analyzed on either the IBM/Bruker AF 200 MHz, IBM/Bruker AF 300 MHz, or the

Varian UnitylNOVA 500 MHz NMR machine.

Procedure for Calculating the Density

The Paar DMA 602 external measuring cell, the Paar 60 processing unit,

and the Neslab EX-210/FTC-350A Cooler/Circulator are the components that

make up the density measuring system. The measurement of densities with the

Paar instrument is based on the change of the natural frequency of a hollow

oscillator when filled with a liquid in the DMA 602 unit.

67

Page 77: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

The instrument was calibrated by performing measurements on air and

delonized water. The accuracy of the calibration was checked by measuring the

density of acetone and comparing to the literature values of CRC Handbook.

Each Ionic liquid was measured three times.

68

Page 78: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

REFERENCES

1. Seddon, K. R. J. Chem. Technol. Biotechnol. 1997, 68,351.

2. Seddon, K. R. Molten Salt Forum: Proceedings of the 5^ International Conference on Molten Salt Chemistry and Technology. 1998, 5-6, 53.

3. Welton, T. Chem. Rev. 1999,112,3926; (b) Wasserscheid, P., Keim, W. Agnew. Chem., Int. Ed. 2000, 39, 3772.

4. Freemantle, M. C&E News, 1998, March 30, 32.

5. Holbrey, J. D., Seddon, K. R. J. Chem. Soc, Dalton Trans. 1999, 2133.

6. Gordon, C. M., Holbrey, J. D., Kennedy, A. R., Seddon, K. R. J. Mater. Chem. 1998, 8, 2627.

7. Chauvin, Y., Olivier-Bourbigou, H. Chemtech. 1995, 25, 26.

8. Fischer, T., Sethi, A., Welton, T., Woolf, J. Tetrahedron Lett. 1999, 40, 793.

9. Carey, F. A., Sundberg, R. J. Advanced Organic Chemistry. Part B: Reactions and Synthesis. Plenum Press: New York and London; 3 ^ ed.; 1990, 1000.

10. Lee, C. W. Tetrahedron Lett. 1999,40, 2461.

11. Carmichael, H. Chemistry in Britian. 2000, 36.

12. Smith, G. P., Dworkin, A. S., Pagni, R. M., Zingg, S. P., J. Am. Chem. Soc. 1989,111,5075.

13. Seddon, K. R. www.ch.qub.ac.uk/resources/ionic/review/review.html

14. Olivier, H., Chauvin, Y. Chem. 2nd. 1996, 249.

15. Olivier, H., Chauvin, Y. Electrochem. Soc. Proceedings. 1998, 96 7,70.

16. Rydberg, J., Musikas, C, Choppin, G. R. Principles and Practices of Solvent Extraction. 1992, Marcel Dekker: New York.

69

Page 79: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

17. Huddleston, J. G., Willauer, H. D., Swatioski, R. P., Visser, A. E., Rogers, R. D. Chem. Commun. 1998,1765.

18. Saurez, P. A. Z., Dullius, J. E. L., Einloft, S., DeSouza, R. F., Dupont, J. Polyhedron, 1996,15, 1217.

19. Carmichael, A. J., Hardacre, C, Holbrey, J. D., Seddon, K. R., Nieuwenhuyzen, M. Electrochem. Soc. Proceedings. 2000, vol. 99-41.

20. Headley, A. D., Starnes, S. D., Cheung, E. T., Malone, P.L, J. Phys. Org. Chem. 1995,8,26.

21. Chastanheira, E. M. S., Martinho, J. M. G., Chem. Phys. Lett. 1991,185, 319.

22. (a) Hausch, C. Ace. Chem. Res. 1962, B2, 232; (b) Koppel, I. A., Palm, V A. In Advances in Linear Free Energy Relationships, Chapman, N. B., Shorter, J. Eds., Plenum Press: London, 1972; (c) Charton, M. Prog. Phys. Org. Chem. 1981, 13, 119; (d) Reynolds, W. F. Prog. Phys. Org. Chem. 1983, 14, 165.

23. (a) Abboud, J. L. M., Kamlet, M.J., Taft, R. W. J. Am. Chem. Soc. 1977, 92, 8325; (b) Taft, R. W. In Steric Effects in Organic Chemistry, Newman, M. S. Ed.; Wiley and Sons: New York, 1956; (c) Fujita, T., Takayama, C, Nakajima, M. J. Org. Chem. 1973, 38, 1623; (d) Taft, R. W., Abboud, J. L. M., Anvia, F., Berthelot, M., Fujio, M., Gal, J. F., Headley, A. D., Henderson, W. G., Koppel, I., Qian, J. H., Mishima, M., Taagepera, M., Uiji, S. J. Am. Chem. Soc. 1988,110, 1979.

24. (a) Kamlet, M. J., Doherty, R. M., Abraham, M. H., Taft, R. W. Quant, Struct.-Act. Relat. 1988, 7, 71; (b) Mishima, M., Mclver, R. T., Jr., Taft, R. W., Bordwell, F. G., Olstead, W. N. J. Am. Chem. Soc. 1984, 106, 2717.

25. Headley, A. D., McMurray, M. E. J. Phys. Org. Chem. 1994, 7, 63.

26. Olson, E. C , Christoffersen, R. E. Computer-Assisted Drug Design. ACS Symposium Series 112, American Chemical Society: Washington, D. C, 1979.

27. Gupta, S. P. Chem. Rev. 1987, 87, 1183-1253.

70

Page 80: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

28. (a) Loew, G. H., Poulsen, M., Kirkjian, E., Ferreil, J., Sudhindra, B. S., Rebagliati, M. EHP, Environ. Health Perspect. 1985, 61, 69-96; (b) Pedersen, L., EHP, Environ. Health Perspect. 1985, 61, 185-190; (c) Chastrette, M.; Rajzmann, M., Chanon, M. J. Am. Chem. Soc. 1985, 107, 1-11; (d) Kier, L. B., Hall, L., Molecular Connectivity in Structure-Activity Analysis, Research Studies Press Ltd.: Letchworth, England. 1986.

29. Ford, M. G., Livingstone, D. J. L. Quant. Struct.-Act. Relat. 1990, 9. 107 114.

30. (a) Politzer, P., Daiker, K. C; In The Force Concept in Chemistry. Deb, B. M. (ed). Van Nostrand Reinhold Co.: New York, 1981, Chap. 6; (b) Sjoberg, P., Murray, J. S., Brinck, T., Politzer, P. Can. J. Chem. 1990, 68, 1440-1443; (c) Politzer, P., Murray, J. S. In Reviews in Computational Chemistry, vol. 2, Lipkowitz, K. B., Boyd, D. B. (eds), VCH Publishers: New York, 1991, Chap. 7; (d) Brinck, T., Murray, J. S., Politzer, P. J. Org. Chem. 1991,56,5012-5015.

31. (a) Famini, G. R. Using Theoretical Descriptors in Quantitative Structure Activity Relationships. V. CRDEC-TR-085, US Army Chemical Research, Development and Engineering Center, Aberdeen Proving Ground, MD, 1989; (b) Wilson, L Y., Famini, G. R. J. Med. Chem. 1991, 34, 1668-1674; (c) Famini, G. R., Kassel, R. J., King, J. W., Wilson, L. Y. Quant. Stmct. Act. Relat. 1991,10, 344-349; (d) Famini, G. R., Ashman, W. P., Mickiewicz, A. P., Wilson, L. Y. Quant. Struct.-Act. Relat. 1992, 11, 162 170; (e) Famini, G. R., Penski, C. A., Wilson, L. Y. J. Phys. Org. Chem. 1992, 5, 395-408.

32. Famini, G. R., Marquez, B. C, Wilson, L. Y. J. Chem. Soc, Perkin Trans. 2, 1993,773-782.

33. (a) Kamlet, M. J., Doherty, R. M., Abraham, M. H., Taft, R. W. Quant. Struct.-Act. Relat. 1988, 7, 71-78; (b) Mashima, M., Mclver Jr., R. T., Taft, R. W., Bordwell, F. G., Olmstead, W. N. J. Am. Chem. Soc. 1984, 106, 2717-2718.

34 (a)Kamlet, M.J., Doherty, R.M., Abraham, M.H., and Taft, R.W. Quant, Struct.-Act. Relat. 1988, 7, 71. (b) Mishima, M. Jr., Mclver, R. T., Taft, R. W., Bordwell, F.G., and Olstead, W. N. J. Am. Chem. Soc. 1984,106, 2717.

35 Williams, D. H. and Fleming, I. Spectroscopic Methods in Organic Chemistry, 5*^ed. McGraw-Hill: London, 1996.

71

Page 81: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

36. Kamlet, M. J., Abboud, J. L. M., Taft, R. W. Prog. Phys. Org. Chem. 1981, 13,485.

37. Frisch, M. J., Trucks, G. W., Schlegel, H. B., Gill, P. M. W., Johnson, B. G., Robb, M. A., Cheeseman, J. R., Keith, T., Peterson, G. A., Montgomery, J. A., Raghavachari, K., Al-Laham, M. A., Zakrzeski, V. G., Ortiz, J. v., Forseman, J. B., Wong, M. W., Cioslowski, J., Stefanov, B. B., Nanayakkara, A., Challacombe, M., Peng, C. Y., Ayala, P. Y., Chen, W., Andres, J. L., Replogle, E. S., Gomperts, R., Martin, R. L., Fox, D. J., Binkley, J. S., Defrees, D. J., Baker, J., Stewart, J. P., Head-Gordon, M., Gonzales, C, Pople, J. A. Gaussian Inc.: Pittsburgh, PA, 1995.

38. (a) Famini, G. R., Benjamin, D., Kim, C, Veerawat, R., Wilson, L. Y. Czech. Chem Commun. 1999, 64, 1727; (b) Mishima, M. Jr., Mclver, R. T., Taft, R. W., Bordwell, F. G., Olstead, W. N. J. Am. Chem. Soc. 1984, 106,2717.

39. Marketed by Wavefunotion. Inc. Irvine, CA

72

Page 82: ANALYSIS OF THE PHYSICAL PROPERTIES OF IONIC LIQUIDS A

PERMISSION TO COPY

In presenting this thesis in partial fulfillment of the requirements for a master's

degree at Texas Tech University or Texas Tech University Health Sciences Center, I

agree that the Library and my major department shall make it freely available for

research purposes. Permission to copy this thesis for scholarly purposes may be

granted by the Director of the Library or my major professor. It is understood that

any copying or publication of this thesis for financial gain shall not be allowed

without my further written permission and that any user may be liable for copyright

infringement.

Agree (Permission is granted.)

Student Signatui'e Date

Disagree (Permission is not granted.)

Student Signature Date