SUPPLEMENTARY MATERIAL< Energetic effects of alkyl groups (methyl and ethyl) on the nitrogen of
morpholine molecule >
Vera L. S. Freitas*, Carlos A. O. Silva, Mónica A. T. Paiva, Maria D. M. C. Ribeiro da Silva
Centro de Investigação em Química, Department of Chemistry and Biochemistry, Faculty of Science, University of Porto, Rua do Campo Alegre, 687, P-4169-007 Porto, Portugal
TABLE OF CONTENTSPage
S1. Purification ..................................................................................................................................................
S3
S2. Combustion calorimetry …………..…………………………………………………..…………………..
S4
S3. Vacuum drop microcalorimetric technique ……..………………………………………………………...
S8
S4. Computational studies – G3(MP2)//B3LYP method ………………………………………….………….
S11
TABLE INDEXPage
Table S1. Source details of the materials used and purification information and analysis of N-methylmorpholine and N-ethylmorpholine.........................................................................................
S3
Table S2. Typical combustion results and standard (p = 0.1 MPa) massic energy of combustion, at T = 298.15 K, for N-methylmorpholine....................................................................................................
S6
Table S3. Typical combustion results and standard (p = 0.1 MPa) massic energy of combustion, at T = 298.15 K, for N-ethylmorpholine.......................................................................................................
S7
Table S4. Calvet microcalorimetry results for the process of vaporization of N-methylmorpholine.................
S9
Table S5. Calvet microcalorimetry results for the process of vaporization of N-ethylmorpholine....................
S10
Table S6. Absolute standard enthalpies, H 298.15 K° , and entropies, S298.15 K
° , obtained by G3(MP2)//B3LYP composite method for the two most stable conformers of N-methylmorpholine, and the corresponding derived gas-phase standard molar enthalpies, ∆ f Hm
° (g), entropies, ∆ f Sm° (g),
and Gibbs energy of formation, ∆ f Gm° (g), at T = 298.15 K, and the conformational
composition, i...... S12Table S7. Absolute standard enthalpies, H 298.15 K
° , and entropies, S298.15 K° , obtained by G3(MP2)//B3LYP
composite method for the two most stable conformers of N-ethylmorpholine, and the corresponding derived gas-phase standard molar enthalpies, ∆ f Hm
° (g), entropies, ∆ f Sm° (g),
and Gibbs energy of formation, ∆ f Gm° (g), at T = 298.15 K, and the conformational
composition, i...... S13Table S8. G3(MP2)//B3LYP enthalpies, H 298.15 K
° , with corresponding conformer composition (in
S1
parentheses and boldface), and experimental gas-phase standard (pº = 0.1 MPa) molar enthalpies of formation, ∆ f Hm
o (g ), at T = 298.15 K, for N-methylmorpholine and N-ethylmorpholine conformers and for the auxiliary species………………………………………………………...
S14
Table S9. Standard (pº = 0.1 MPa) molar heat capacities in the gaseous phase for N-methylmorpholine and N-ethylmorpholine, derived from statistical thermodynamics using the vibrational frequencies calculated at the B3LYP/6-31G(d) level of theory (scaled by a factor of 0.960 0.022).....................................................................................................................................
S16
S2
Throughout this paper, the standard state (and thus any standard thermodynamic property) of a pure
liquid refers to the pure substance in the liquid phase under the pressure of p = 0.1 MPa. When the substance
is a pure gas, its standard state is that of an ideal gas at p of 0.1 MPa (or, which is equivalent, that of a real
gas at p = 0). Standard states will be denoted by a superscript “o”.
The relative atomic masses used throughout this paper were those suggested by the IUPAC
Commission in 2013 [1].
S3
S1. Purification
The purity control of the samples was carried out by gas-liquid chromatography, using an Agilent 4890 apparatus equipped with an HP-5 column, cross-
linked, 5% diphenyl and 95% dimethylpolysiloxane (15 m 0.530 mm i. d. 1.5 μm film thickness), and by the ratio of carbon dioxide recovered during the
combustion experiments (gravimetric analysis results are given in tables S2 and S3).
Table S1 Source details of the materials used and purification information and analysis of N-methylmorpholine and N-ethylmorpholine.
Chemical Name CAS Registry No. Source Initial purity Purification method Final mass fraction purity
N-methylmorpholine 109-02-4 Sigma-Aldrich 0.9991 a Vacuum distillation 0.9995b
1.0001 0.0002c
N-ethylmorpholine 100-74-3 TCI 0.969 a Vacuum distillation 0.9990b
Benzoic acid 65-85-0 NIST 0.999996 a
Decane 124-18-5 Sigma-Aldrich 0.990 a a Values stated in the certificate of analysis of the supplier;b Mass fraction purities obtained from gas-liquid chromatography;c Results obtained from combustion calorimetry, based on mass fraction of carbon dioxide recovery (mean and standard deviation of the mean for six experiments).
S4
S2. Combustion calorimetry
The combustion experiments of the organic nitrogen compounds were performed with an isoperibol
calorimeter [2-4]. This calorimeter has a twin valve bomb, with an internal volume of 0.290 dm 3 made of
stainless steel (with a wall thickness of 1 cm). The calorimetric system was calibrated using benzoic acid
Standard Reference Material (SRM) 39j supplied by National Institute of Standards & Technology [5],
having a massic energy of combustion of (26434 ± 3) J·g-1, when burned under certificate conditions. For
each calibration experiment, 1.00 cm3 of desionized water was added to the bomb, and the bomb was flushed
and charged to 3.04 MPa with pure oxygen (xO2≥ 0.99995). The calibration results were corrected to give the
energy equivalent, ε (calor), corresponding to the average mass of water added to the calorimeter of 2900.0
g. One set of six calibration experiments was performed leading to the value of the energy equivalent of the
calorimeter, ε (cal) = (15551.2 ± 1.6) J·K-1, where the standard uncertainty quoted is the estimated standard
deviation of the mean.
The liquid samples were enclosed in polyester bags made of Melinex® (0.025 mm thickness), using
the technique described by Skinner and Snelson [6]. In each experiment, the sample and the auxiliary were
introduced in a platinum crucible inside the bomb and in contact with a cotton thread fuse attached to the
platinum ignition wire (Goodfellows, = 0.05 mm). All weighs were performed in a Mettler AE240, with a
precision ± (110-5) g. The combustion bomb was flushed and filled with pure oxygen (xO2≥ 0.99995) until
reaching a pressure of 3.04 MPa and, approximately, 2900.0 g of water were introduced inside the
calorimeter. The calorimeter temperature was measured to ± (110-4) K, at intervals of ten seconds using a
S10 four wire calibrated ultra-stable thermistor probe (Thermometrics, standard serial No. 1030) and
recorded by a high sensitivity nanovolt/microohm meter (Agilent 34420 A) interfaced to a computer
programmed to compute the adiabatic temperature change, Tad. The samples were ignited at T = (298.150 ±
0.001) K, by the discharge of a 1400 F capacitor through the platinum ignition wire.
The combustion reactions for N-methylmorpholine (C5H11NO) and N-ethylmorpholine (C6H13NO) are
represented by the following equations, respectively:
C5 H11 NO (l) + 7.25 O2 (g) → 5 CO2 (g ) + 5.5 H2 O (l) + 0.5 N2 (g) (S1)
C6 H13NO (l) + 8.75 O2 (g) → 6 CO2 (g ) + 6.5 H2 O (l) + 0.5 N2(g) (S2)
The temperature profiles for each experiment were divided into three periods, fore-, main- and after-
periods, each one with one hundred points at least. The energy of reaction was always referred to the initial
temperature of 298.15 K. The accurate numerical calculation of the corrected temperature rise in the
isoperibol calorimetry was carried out by means of the LABTERMO program [7] based in the method of
S5
calculation described by Coops et al. [8]. The electrical energy for the ignition U(ign) was determined from
the change in potential difference across a 1400 μF capacitor through the platinum ignition wire.
The internal energy associated to the isothermal bomb process, ∆ U (IBP), was calculated through eq.
S3, in which ∆ T ad is the calorimeter temperature change corrected for the heat exchange and the work of
stirring, ∆ m (H2 O ) represents the difference between the mass of water added to the calorimeter and the
mass of 2900.0 g assigned to ε (cal ), ε f is the energy equivalent of the content in the final state, ∆ U (ign) is
the electric energy for the ignition, and cp (H2 O, l ) is the massic heat capacity, at constant pressure, for liquid
water.
∆ U (IBP ) /J=−{ε (cal )+∆ m (H2O ) ∙ c p (H2O, l )+εf }∆ T ad+∆ U (ign ) (S3)
After the calorimetric measurements the combustion products were analyzed: the caobon dioxide
(CO2) formed was collected in absorption tubes [9] and calculated from the increase in weight of the tubes by
multiplying it by the factor 1.0045, previously derived by Rossini [10]; the nitric acid formed was determined
by titration and the respective correction was based on 59.7 kJ·mol-1 (the molar energy of formation for 0.1
mol·dm-3 HNO3 (aq) from N2 (g), O2 (g) and H2O (l) [11]). The cotton thread used has an empirical formula
CH1.686O0.843 and a massic energy of combustion 16240 J·g-1 [8], a value previously confirmed in our
laboratory. In the case of Melinex, it was considered the standard massic energy of combustion of dry
Melinex ∆ c uo = (22902 ± 5) J·g-1 [6]. This value was confirmed by combustion of Melinex samples in
our laboratory. The mass of Melinex used in each experiment was corrected for the mass fraction of water
(0.0032).
For the experiments with a small carbon soot residue formed during the combustion, the necessary
energetic correction for its formation was based on standard molar energy of combustion of 33 kJmol-1
[11].
The value for the pressure coefficient of specific energy (∂u /∂ p)T , was assumed to be
0.2 J·g-1·MPa-1, at T = 298.15 K, a typical value for most organic compounds [12]. The mass of compound,
m(cpd) used in each experiment was determined from the total mass of CO2 produced after allowance for
that formed from the Melinex.
The reduction of weight in air to mass in vacuum was made using specific densities: 0.92 gcm-3 for
N-methylmorpholine [13] and 0.91 gcm-3 for N-ethylmorpholine [14]. The standard massic energies of
combustion of the compounds, ∆ c uo, were calculated according to the procedure given by Hubbard et al. [15].
The results for typical combustion experiments and the individual values of ∆c uo(l), together with the
mean and the estimated standard deviation of the mean, for N-methylmorpholine and
N-ethylmorpholine are given in Tables S2 and S3, respectively.
S6
S7
Table S2 Typical combustion results and standard (p = 0.1 MPa) massic energy of combustion, at T = 298.15 K, for N-methylmorpholine.a
Experiment 1 2 3 4 5 6
m (CO2, total) / g 1.74688 1.84867 1.47548 1.68892 1.45580 1.47456m (cpd) / g 0.68390 0.73197 0.57709 0.58663 0.56842 0.57982m (fuse) / g 0.00299 0.00213 0.00253 0.00263 0.00229 0.00287m (Melinex) / g 0.11099 0.11038 0.09427 0.17858 0.09409 0.09104m (carbon) / g 0 0 0 0.00015 0 0Tad / K 1.61767 1.71966 1.36733 1.51144 1.34849 1.36761ef / (J·K-1) 15.70 15.85 15.25 15.45 15.23 15.26m (H2O) / g 2.0 0.2 1.4 1.0 0.5 0U (IBP) / J 25194.96 26770.73 21275.73 23520.95 20993.26 24241.69U (carbon) / J 0 0 0 4.95 0 0U (Melinex) / J 2541.93 2528.00 2159.06 4089.89 2154.94 2085.04U (fuse) / J 48.56 34.59 41.09 42.71 37.19 46.61U (HNO3) / J 44.12 49.69 40.48 42.15 39.04 40.54U (ign) / J 0.68 0.74 0.73 0.78 0.74 0.65US / J 11.64 12.37 9.59 11.55 9.46 9.57
∆ c uo / (J·g-1) 32970.78 32987.80 32968.02 32967.29 32990.79 32952.36
% CO2100.083 99.958 100.029 100.007 99.987 100.005
−∆c uo = (32972.8 ± 5.8) J·g-1, b
%C O2= (100.012 ± 0.017) b
aThe symbols presented in this table have the following meaning: m(CO2, total), mass of carbon dioxide; m(cpd), mass of compound; m(fuse), mass of fuse (cotton); m(Melinex), mass of Melinex; m(carbon), mass of carbon residue formed; Tad, corrected temperature rise; ef, energy equivalent of the contents in the final state; m(H2O), deviation of mass of water added to the calorimeter from 2900.0 g; U(IBP), internal energy associated to the isothermal combustion reaction under actual bomb conditions (eq. S3); U(carbon), energy of combustion of carbon residue; U(Melinex), energy of combustion of Melinex; U(fuse), energy of combustion of the fuse (cotton); U(HNO3), energy correction for the nitric acid formation; U(ign), electric energy for the
S8
ignition; US, standard state correction; ∆ c uo, standard (p = 0.1 MPa) massic energy of combustion for the compound; % CO2, percentage of carbon dioxide recovered;b The standard uncertainty corresponds to the estimated standard deviation of the mean for six experiments.
S9
Table S3 Typical combustion results and standard (p = 0.1 MPa) massic energy of combustion, at T = 298.15 K, for N-ethylmorpholine.a
Experiment 1 2 3 4 5 6
m (CO2, total) / g 1.17972 0.95338 1.20530 1.21422 1.09061 1.18227m (cpd) / g 0.41191 0.31583 0.42219 0.42626 0.38297 0.42222m (fuse) / g 0.00268 0.00221 0.00200 0.00237 0.00219 0.00233m (Melinex) / g 0.10087 0.10015 0.10222 0.10178 0.09127 0.09191m (carbon) / g 0 0.00100 0 0 0 0Tad / K 1.06997 0.85399 1.09519 1.10430 0.99248 1.08065ef / (J·K-1) 14.69 14.32 14.72 14.71 14.50 14.72m (H2O) / g 1.3 1.8 0.7 1.0 0.7 0U (IBP) / J 16659.66 13285.17 17049.65 17192.85 15450.36 16820.12U (carbon) / J 0 33.00 0 0 0 0U (Melinex) / J 2310.06 2293.61 2341.13 2331.08 2090.29 2104.91U (fuse) / J 43.52 35.89 32.48 38.49 35.57 37.84U (HNO3) / J 32.90 26.73 34.29 38.77 37.68 32.90U (ign) / J 1.20 1.20 1.20 1.20 1.19 1.19US / J 7.26 5.88 7.42 7.48 6.60 7.23 cuº (cpd) / (J·g-1) 34633.57 34689.73 34662.89 34666.72 34676.93 34667.33
% CO299.784 99.866 99.770 99.212 99.697 99.670
−∆c uo = (34666.2 ± 7.6) J·g-1, b
aThe symbols presented in this table have the same meaning of the symbols of the above table;bThe standard uncertainty corresponds to the estimated standard deviation of the mean for six experiments.
S10
S3. Vacuum drop-microcalorimetric technique
The standard (pº = 0.1 MPa) molar enthalpies of vaporization, ∆ lg H m
º , of the two
N-alkylmorpholine derivatives were determined by the vacuum drop-microcalorimetry technique.
This technique was described by Skinner et al for the study of solids [16], for the determination of
enthalpies of sublimation, which was adapted and tested for liquid vaporizations in our Laboratory
[17]. The measurements were carried out with a high temperature Calvet microcalorimeter (Setaram
HT1000, Lyon, France) with the vacuum promoted by a rotary vacuum pump and a vapour
diffusion pump. Both apparatus and technique have been already described in the literature [18].
The temperature, T, of the hot reaction vessel of the calorimeter was predefined for the
vaporization study of each compound: 334 K for N-methylmorpholine and 376 K for N-
ethylmorpholine. During the vaporization experiments of N-ethylmorpholine the cells of the
calorimeter where filled with nitrogen, once the compound is hygroscopic. The samples (ranging
from 4-6 mg) contained in thin glass capillary tubes sealed at one end, were dropped simultaneously
with the corresponding blank tube at T = 298.15K into the hot reaction vessel in the Calvet
microcalorimeter, held at the hot-zone temperature; after reached the thermostability, the sample is
removed from the hot-zone by vacuum. The samples of the compound and the glass capillary tubes
were weighed with a precision ± (110-6) g on a Mettler-Toledo UMT2 microbalance.
The blank heat capacity corrections for the glass capillary tubes and for the different
sensibilities of the two measuring cells were determined in separate experiments. Individual blank
correction experiments were performed by dropping tubes of nearly equal mass, between 20 and 25
mg to within (110-4) g, into each of the twin calorimetric cells. A blank heat capacity correction,
as a function of the hot reaction vessel, T, and of the masses of the blank and of the experimental
capillary tube, was obtained.
The microcalorimeter was calibrated in situ for the two predefined temperatures through the
determination of the enthalpy of vaporization of decane, a recommended reference material,
following a procedure identical to that described above for the compounds, using its values of the
standard molar enthalpy of vaporization, at T = 298.15 K, ∆ lg Hm
º = (51.4 0.2) kJmol-1 [19]. The
calibration constants determined for the experimental conditions of each of the compounds were:
kcal(N-methylmorpholine) = (1.042 0.018) and kcal(N-ethylmorpholine) = (1.013 0.010); these
constants were obtained as the average of five and six independent experiments, respectively, with
the quoted standard uncertainty being the combined standard uncertainty which include the
estimated standard deviation of the mean and the standard uncertainty associated with the reference
value of the decane.
S11
The Calvet microcalorimetry results obtained for the process of vaporization of the two
compounds studied are given in tables S4 and S5.
Table S4 Calvet microcalorimetry results for the process of vaporization of N-methylmorpholine.a
Ensaio 1 2 3 4 5 6
TCalvet / Kb 334.58 334.58 334.70 334.33 334.28 334.41
m(sct) / mg 23.3665 22.2779 24.6631 22.2750 23.3794 21.5401
m(rct) / mg 23.3723 22.3034 24.7906 22.3037 23.3809 21.5486
m(cpd) / mg 5.825 5.698 5.488 4.820 6.450 5.738
H(blank) / mJ 9.060 5.186 7.770 5.788 9.256 4.022
H(total) / J 2.471 2.420 2.383 1.975 2.801 2.428
H(corr) / J 2.462 2.415 2.375 1.970 2.792 2.424
∆ l, 298.15Kg, T Calvet Hm
° (exp)/ kJmol-1 44.54 44.67 45.61 43.07 45.63 44.51
∆298.15 KTCalvet H m
° (g)/ kJ·mol-1 4.65 4.65 4.66 4.61 4.61 4.62
∆ lg H m
° (298.15 K) / kJ·mol-1 39.9 40.0 40.9 38.5 41.0 39.9
∆ lg H m
° (298.15 K) = 40.0 3.1 kJ·mol-1, c
aThe symbols presented in this table have the following meaning: TCalvet, temperature of the hot reaction vessel; m(sct) mass of the sample capillary tube; m(rct) mass of the reference capillary tube; m(cpd), mass of the compound; H(blank), blank heat capacity corrections for the glass capillary tubes; H(total), total enthalpy calculated from the area of the enthalpic peak obtained in the experiment; H(corr), enthalpy change corrected taking into account the blank experiments, calculated from H(corr) = H(total) + H(blank); ∆ l, 298.15K
g, T Calvet Hm° (exp), enthalpy of vaporization from 298.15 K to temperature of the hot reaction
vessel calculated from ∆ l, 298.15Kg, T Calvet Hm
° ( exp )=¿¿, where k cal is the calibration constant of the calorimeter for
the experimental conditions and M the molar mass of the compound; ∆298.15 KTCalvet H m
° (g), enthalpy change in the
gas-phase phase from 298.15 K to the temperature of the hot reaction vessel; ∆ lg H m
° (298.15 K), enthalpy of vaporization at 298.15 K of the compound calculated from
∆ lg Hm
° ( 298.15 K ) = ∆ l ,298.15 Kg , TCalvet Hm
° (exp) ∆298.15KTCalvet H m
° (g).bThe standard uncertainty of the temperature measurements is u(T/K) = 0.01.cThe standard uncertainty corresponds to the expanded uncertainty determined from the combined standard uncertainty (which include the contribution of calibration with decane) and the coverage factor k = 2.57 (for an effective degrees of freedom of 6, calculated from Welch-Satterthwaite formula, and a 0.95 level of confidence) [20].
S12
Table S5 Calvet microcalorimetry results for the process of vaporization of N-ethylmorpholine.a
Ensaio 1 2 3 4 5 6
TCalvet / Kb 375.72 375.96 375.85 375.85 375.85 375.72
m(sct) / mg 21.4623 24.7950 25.1841 20.2711 20.6168 19.5893
m(rct) / mg 21.5412 24.8160 25.2411 20.3145 20.7141 19.6417
m(cpd) / mg 5.0690 5.0481 4.4696 5.6581 5.6960 4.9751
H(blank) / mJ 38.652 31.862 33.357 37.981 40.579 39.223
H(total) / J 2.302 2.370 2.060 2.619 2.693 2.282
H(corr) / J 2.341 2.402 2.094 2.657 2.734 2.321
∆ l, 298.15Kg, T Calvet Hm
° (exp)/ kJmol-1 53.87 55.51 54.65 54.79 55.99 54.43
∆298.15 KTCalvet H m
° (g)/ kJ·mol-1 12.41 12.45 12.43 12.43 12.43 12.41
∆ lg H m
° (298.15 K) / kJ·mol-1 41.5 43.1 42.2 42.4 43.6 42.0
∆ lg H m
° (298.15 K) = 42.4 2.6 kJ·mol-1, c
aThe symbols presented in this table have the same meaning of the symbols of the above table.bThe standard uncertainty of the temperature measurements is u(T/K) = 0.01.cThe standard uncertainty corresponds to the expanded uncertainty determined from the combined standard uncertainty (which include the contribution of calibration with decane) and the coverage factor k = 2.36 (for an effective degrees of freedom of 8, calculated from Welch-Satterthwaite formula, and a 0.95 level of confidence) [20].
S13
S4. Computational studies – G3(MP2)//B3LYP method
Molecular calculations concerned with this work were performed with the Gaussian-03
software package [21] using the composite method G3(MP2)//B3LYP [22], a variation of the
Gaussian-3 (G3) theory [23].
Estimated gas-phase enthalpy of formation
A systematic conformation search was made for N-methylmorpholine and N-ethylmorpholine
to determine the low energy conformers. The fractional population of each conformer at T = 298.15
K was calculated assuming a Boltzmann distribution.
In tables S6 and S7 are the absolute standard enthalpies, H 298.15 K° , and entropies, S298.15 K
° ,
obtained by G3(MP2)//B3LYP composite method [22] for the most stable conformers of each N-
alkylmorpholine, and the corresponding derived gas-phase standard molar enthalpies, ∆ f Hm° (g),
entropies, ∆ f Sm° (g), and Gibbs energy of formation, ∆ f Gm
° (g), at T = 298.15 K, and the
conformational composition, i.
The gas-phase standard molar enthalpy of each working reaction was calculated taking into
account eqs. S4 and S5. The enthalpy of reaction, ∆R H m° , at T = 298.15 K, was obtained
computationally from the absolute standard enthalpies, H 298.15 K° , of each species. The rearrangement
of eq. S5 and the knowledge of the experimental standard molar gas-phase enthalpies of formation
of all the auxiliary species used reported in table S8 enabled the calculation of the species under
study.
The G3(MP2)//B3LYP absolute enthalpies, H 298.15 K° , and the experimental enthalpies of
formation in the gas phase, ∆ f Hm° (g), of the molecular species used are given in Table S8.
∆R H m° =∑ H298.15 K
° (products )−∑ H298.15K° ( reagents ) (S4)
∆R H m° =∑∆ f Hm
° (products )−∑∆ f Hm° (reagents ) (S5)
S14
Table S6. Absolute standard enthalpies, H 298.15 K° , and entropies, S298.15 K
° , obtained by G3(MP2)//B3LYP composite method for the two most stable conformers of N-methylmorpholine, and the corresponding derived gas-phase standard molar enthalpies, ∆ f Hm
° (g), entropies, ∆ f Sm° (g),
and Gibbs energy of formation, ∆ f Gm° (g), at T = 298.15 K, and the conformational composition, i. 1 a. u. (Hartree) corresponds to 2625.50
kJmol-1.
Conformationa H 298.15 K° b /
a.u.
∆ f Hm° (g) c /
kJmol-1
S298.15 K° d /
JK-1mol-1
∆ f Sm° (g) e /
JK-1mol-1
∆ f Gm° (g) f /
kJmol-1χ i
g
I 326.565719 155.1 2.3 332.44 612.4 45.1 0.9991
II 326.559012 137.5 2.3 333.40 604.8 59.6 0.0009
aAtom color code: grey, C; red, O; blue, N; white, H.bObtained from G3(MP2)//B3LYP method [22].cEstimated from nine working reactions;dObtained from B3LYP/6-31G(d) method for a frequency factor scale of 1.0029 [24] ;eCalculated from, ∆ f Sm
° ( g )=S298.15 K° (conformer i )−∑ S298.15K
° (elements) considering the standard absolute entropy elements values, at 298.15 K,
S298.15 K° (H2 , g ) = 130.680 JK-1mol-1, S298.15 K
° (C, graphite ) = 5.740 JK-1mol-1, S298.15 K° (N2 , g ) = 191.609 JK-1mol-1, and S298.15 K
° (O2 , g ) = 205.147 JK-
1mol-1 taken from ref. [25];fCalculated from ∆ f Gm
° ( g )=∆f H m° ( g )−T ∆ f Sm
° ( g );
g Calculated from χ i=e
−[ Δf Gmo (g)/ RT ]
/∑i
n
e−[ Δf Gm
o ( g)/RT ]
.
S15
Table S7. Absolute standard enthalpies, H 298.15 K° , and entropies, S298.15 K
° , obtained by G3(MP2)//B3LYP composite method for the two most stable conformers of N-ethylmorpholine, and the corresponding derived gas-phase standard molar enthalpies, ∆ f Hm
° (g), entropies, ∆ f Sm° (g), and
Gibbs energy of formation, ∆ f Gm° (g), at T = 298.15 K, and the conformational composition, i. 1 a. u. (Hartree) corresponds to 2625.50 kJmol-1.
Conformationa H 298.15 K° b /
a.u.
∆ f Hm° (g) c /
kJmol-1
S298.15 K° d /
JK-1mol-1
∆ f Sm° (g) e /
JK-1mol-1
∆ f Gm° (g) f /
kJmol-1χ i
g
I 365.802204 180.7 2.6 364.35 622.1 4.8 0.9231
II 365.799930 174.8 2.6 363.38 623.1 11.0 0.0760
III 365.795538 163.2 2.6 365.04 621.4 22.1 0.0009
aAtom color code: grey, C; red, O; blue, N; white, H.bObtained from G3(MP2)//B3LYP method [22].cEstimated from six working reactions;dObtained from B3LYP/6-31G(d) method for a frequency factor scale of 1.0029 [24] ;eCalculated from, ∆ f Sm
° ( g )=S298.15 K° (conformer i )−∑ S298.15K
° (elements) considering the standard absolute entropy elements values, at 298.15 K,
S298.15 K° (H2 , g ) = 130.680 JK-1mol-1, S298.15 K
° (C, graphite ) = 5.740 JK-1mol-1, S298.15 K° (N2 , g ) = 191.609 JK-1mol-1, and S298.15 K
° (O2 , g) = 205.147 JK-
1mol-1 taken from ref. [25];fCalculated from ∆ f Gm
° ( g )=∆f H m° ( g )−T ∆ f Sm
° ( g );
S16
g Calculated from χ i=e
−[ Δf Gmo (g)/ RT ]
/∑i
n
e−[ Δf Gm
o ( g)/RT ]
.
S17
Table S8. G3(MP2)//B3LYP enthalpies, H 298.15 K° , with corresponding conformer composition (in
parentheses and boldface), and experimental gas-phase standard (pº = 0.1 MPa) molar enthalpies of
formation, ∆ f Hmo (g ), at T = 298.15 K, for N-methylmorpholine and N-ethylmorpholine conformers
and for the auxiliary species. 1 a. u. (Hartree) corresponds to 2625.50 kJmol-1.
Atom/Compound Atom/ Molecular Structure H 298.15 K° / a. u. ∆ f Hm
o (g ) /
kJmol-1
Hydrogen H 0.499780 218.0 [25]
Carbon C 37.788425 716.7 [25]
Oxygen O 74.989704 249.17 [25]
Nitrogen N 54.524582 472.68 [25]
carbazole 516.611310 (1.0) 205.0 3.0 [26]
cyclohexane 235.407852 (1.0) 123.3 ± 0.8 [26]
9,10-dihydroanthracene 539.796179 (1.0) 159.7 2.6 [26]
N-ethylmorpholine365.802204 (0.9231)365.799930 (0.0760)365.795538 (0.0009)
This work
N-ethylpiperidine 329.906796 (0.9)329.904880 (0.1) 82.1 2.0 [27]
1-ethylpyrazole 304.326951 (1.0) 132.6 3.3 [28]
imidazole 225.873397 (1.0) 132.9 0.6 [26]
indole 363.214962 (1.0) 164.3 1.3 [29]
N-methylcarbazole 555.842444 (1.0) 199.1 0.5 [30]
(continued overleaf)
S18
Table S8 (continued) G3(MP2)//B3LYP enthalpies, H 298.15 K° , with corresponding conformer
composition (in parentheses and boldface), and experimental gas-phase standard (pº = 0.1 MPa) molar enthalpies of formation, ∆ f Hm
o (g ), at T = 298.15 K, for N-methylmorpholine and N-ethylmorpholine conformers and for the auxiliary species. 1 a. u. (Hartree) corresponds to 2625.50 kJmol-1.
Atom/Compound Atom/ Molecular Structure H 298.15 K° / a. u. ∆ f Hm
o (g ) /
kJmol-1
1-methylimidazole 265.103076 (1.0) 126.5 1.1 [31]
1-methylindole 402.445506 (1.0) 155.8 2.8 [32]
N-methylmorpholine 326.565719 (0.9991)326.559012 (0.0009) This work
N-methylphenothiazine 953.586193 (1.0) 271.3 4.1 [33]
N-methylphenoxazine 630.963683 (1.0) 97.5 1.6 [33]
N-methylpiperidine 290.670724 (1.0) 59.1 1.7 [34]
1-methylpyrazole 265.088374 (1.0) 156.5 2.1 [35]
N-methylpyrrole 249.051704 (1.0) 103.1 0.5 [26]
morpholine 287.334005 (0.78)287.332743 (0.22) 141.7 1.5 [36]
piperidine 251.439307 (0.76)251.438108 (0.24) 47.2 0.6 [26]
1H-pyrazole 225.855898 (1.0) 179.4 0.8 [37]
pyrrole 209.822541 (1.0) 108.4 0.6 [26]
tetrahydropyran 271.303681 (1.0) 223.4 1.0 [26]
thioxanthene 898.319446 (1.0) 218.7 4.2 [38]
S19
Standard molar heat capacities in the gaseous phase
Table S9 Standard (pº = 0.1 MPa) molar heat capacities in the gaseous phase for
N-methylmorpholine and N-ethylmorpholine, derived from statistical thermodynamics using the
vibrational frequencies calculated at the B3LYP/6-31G(d) level of theory (scaled by a factor of
0.960 0.022) [39].
T / KC p
o (g) / JK-1mol-1
N-methylmorpholine N-ethylmorpholine
200.00 83.87 99.49
250.00 101.48 119.98
298.15 120.05 141.70
300.00 120.78 142.56
350.00 140.96 166.16
400.00 160.96 189.52
450.00 180.05 211.80
500.00 197.85 232.56
550.00 214.27 251.70
600.00 229.32 269.24
650.00 243.11 285.31
700.00 255.75 300.05
S20
REFERENCES
S21
1. Meija J, Coplen TB, Berglund M, Brand WA, De Bièvre P, Gröning M, Holden NE, Irrgeher
J, Loss RD, Walczyk T, Prohaska T. Atomic weights of the elements 2013 (IUPAC Technical
Report). Pure Appl Chem. 2016;88:265-91.
2. Gundry HA, Harrop D, Head AJ, Lewis GB. Thermodynamic properties of organic oxygen
compounds 21. Enthalpies of combustion of benzoic acid, pentan-1-ol, octan-1-ol, and hexadecan-
1-ol. J Chem Thermodyn. 1969;1:321-32.
5. Certificate of Analysis, Standard Reference Material 39j, Benzoic Acid Calorimetric
Standard, N. B. S., Washington, 1995.
6. Skinner HA, Snelson A. The heats of combustion of the four isomeric butyl alcohols. Trans
Faraday Soc. 1960;56:1776-83.
7. Santos LMNBF, Silva MT, Schröder B, Gomes L. LABTERMO: Methodologies for the
calculation of the corrected temperature rise in isoperibol calorimetry. J Therm Anal Calorim.
2007;89:175-80.
8. Coops J, Jessup RS, van Nes K. Calibration of calorimeters for reactions in a bomb at
constant volume. In: Rossini FD, editor. Experimental Thermochemistry, vol. 1. New York:
Interscience; 1956. pp. 27-58.
9. Ribeiro da Silva MAV, Ribeiro da Silva MDMC, Pilcher G. The constrution, calibration and
use of a new high-precision static-bomb calorimeter. Rev Port Quím. 1984;26:163-72.
10. Rossini FD. The heat of formation of water. J Res Nat Bur Stand. 1931;6:1-35.
11 Wagman DD, Evans WH, Parker VB, Schumm RH, Halow I, Bailey SM, Churney KL, Nuttal
RL. The NBS tables of chemical thermodynamics properties. J Phys Chem Ref Data. 1982; II,
Suppl. 2.
12. Washburn EN. Standard states for bomb calorimetry. J Res Nat Bur Stand (US). 1933;10:525-
58.
13. ChemSpider, Search and Share Chemistry. http://www.chemspider.com/Chemical-
Structure.7684.html?rid=7a8a2828-07b8-4ad3-8e16-c4ba782d05a9 of subordinate document.
Accessed 8 Dec 2016.
14. ChemSpider, Search and Share Chemistry. http://www.chemspider.com/Chemical-
Structure.7244.html?rid=33375fbb-d5fa-4636-8681-dcb356b098e9&page_num=0 of subordinate
document. Accessed 8 Dec 2016.
15. Hubbard WN, Scott DW, Waddington G. Standard states and corrections for combustions in a
bomb at constant volume. In: Rossini FD, editor. Experimental Thermochemistry, vol. 1. New
York: Interscience; 1956. pp. 75-128.
16. Adedeji FA, Brown DLS, Connor JA, Leung WL, Paz-Andrade IM, Skinner HA.
Thermochemistry of arene chromium tricarbonyls and the strenghts of arene-chromium bonds. J
Organomet Chem. 1975;97:221-8.
17. Ribeiro da Silva MAV, Matos MAR, Amaral LMPF. Thermochemical study of 2-, 4-, 6-, and
8-methylquinoline. J Chem Thermodyn. 1995;27:565-74.
18. Santos LMNBF, Schröder B, Fernandes OOP, Ribeiro da Silva MAV. Measurement of
enthalpies of sublimation by drop method in a Calvet type calorimeter: design and test of a new
system. Thermochim Acta. 2014;415:15-20.
19. Sabbah R, Xu-wu A, Chickos JS, Planas Leitão ML, Roux MV, Torres LA. Reference
materials for calorimetry and differential thermal analysis. Thermochim Acta. 1999;331:93-204.
20. Taylor BN, Kuyatt CE. Guidelines for evaluating and expressing the uncertainty of NIST
measurement results, NIST Technical Note 1297, 1994 Edition.
21. Gaussian 03, Revision C.012. Frisch MJ, Trucks GW, Schlegel HB, Scuseria GE, Robb MA,
Cheeseman JR, Montgomery Jr. JA, Vreven T, Kudin KN, Burant JC, Millam JM, Iyengar SS,
Tomasi J, Barone V, Mennucci B, Cossi M, Scalmani G, Rega N, Petersson GA, Nakatsuji H, Hada
M, Ehara M, Toyota K, Fukuda R, Hasegawa J, Ishida M, Nakajima T, Honda Y, Kitao O, Nakai H,
Klene M, Li X, Knox JE, Hratchian HP, Cross JB, Bakken V, Adamo C, Jaramillo J, Gomperts R,
Stratmann RE, Yazyev O, Austin AJ, Cammi R, Pomelli C, Ochterski JW, Ayala PY, Morokuma K,
Voth GA, Salvador P, Dannenberg JJ, Zakrzewski VG, Dapprich S, Daniels AD, Strain MC, Farkas
O, Malick DK, Rabuck AD, Raghavachari K, Foresman JB, Ortiz JV, Cui Q, Baboul AG, Clifford
S, Cioslowski J, Stefanov BB, Liu G, Liashenko A, Piskorz P, Komaromi I, Martin RL, Fox DJ,
Keith T, Al-Laham MA, Peng CY, Nanayakkara A, Challacombe M, Gill PMW, Johnson B, Chen
W, Wong MW, Gonzalez C, Pople JA. Gaussian, Inc., Wallingford CT, 2004.
22. Baboul AG, Curtiss LA, Redfern PC, Raghavachari K. Gaussian-3 theory using density
functional geometries and zero-point energies. J Chem Phys. 1999;110:7650-7.
23. Curtiss LA, Raghavachari K, Redfern PC, Rassolov V, Pople JA. Gaussian-3 (G3) theory for
molecules containing first and second-row atoms. J Chem Phys. 1998;109:7764-76.
24. Merrick JP, Moran D, Radom L. An evaluation of harmonic vibrational frequency scale
factors. J Phys Chem A. 2007;111:11683-700.
25. Chase Jr. MW. NIST JANAF Thermochemical tables, Fourth Edition, J Phys Chem Ref Data,
Monograph 9. 1998;1-1951.
26. Pedley JB. Thermochemical data and structures of organic compounds thermodynamics.
Texas: Research Centre, College Station; 1994.
27. Ribeiro da Silva MAV, Cabral JITA, Gomes JRB. Experimental and computational study on
the thermochemistry of ethylpiperidines. J Chem Thermodyn. 2006;38:1072-8.
28. Ribeiro da Silva MAV, Ribeiro da Silva MDMC, Matos MAR, Jimenez P, Roux MV,
Elguero J, Claramunt R, Cabildo P, Sanchez-Migallón A. Enthalpies of combustion, heat capacities,
and enthalpies of vaporization of 1-ethylimidazole and 1-ethylpyrazole. J Chem Thermodyn.
1999;31:129-38.
29. Ribeiro da Silva MAV, Cabral JITA, Gomes JRB. Experimental and computational study on
the molecular energetics of indoline and índole. J Phys Chem A. 2008;112:12263-9.
30. Steele WV, Knipmeyer SE, Nguyen A, Chirico RD. Thermodynamic properties of 9-
methylcarbazole and 1,2,3,4-tetrahydro-9-methylcarbazole. Rept. NIPER-520. 1991;1-45.
31. Vitorino J, Bernardes CES, Minas da Piedade ME. A general strategy for the experimental
study of the thermochemistry of protic ionic liquids: enthalpy of formation and vaporisation of 1-
methylimidazolium ethanoate. Phys Chem Chem Phys. 2012;14:4440-6.
32. Ribeiro da Silva MAV, Cabral JITA, Gomes JRB. Combined experimental and computational
study of the energetics of methylindoles. J Chem thermodyn. 2009;41:1193-8.
33. Oliveira TSM, Freitas VLS, Ribeiro da Silva MDMC. Energetic insights on two dye key
molecules: N-methylphenothiazine and N-methylphenoxazine. J Chem Thermodyn. 2016;94:7-15.
JCT 94 (2016) 7-15.
34. Ribeiro da Silva MAV, Cabral JITA, Gomes P, Gomes JRB. Combined experimental and
computational study of the thermochemistry of methylpiperidines. J Org Chem.2006;71:3677-85.
35. Mó O, Yáñez M, Roux MV, Jiménez P, Dávalos JZ, Ribeiro da Silva MAV, Ribeiro da Silva
MDMC, Matos MAR, Amaral LMPF, Sánchez-Migallón A, Cabildo P, Claramunt R, Elguero J,
Liebman JF. Enthalpies of formation of N-substituted pyrazoles and imidazoles. J Phys Chem A.
1999;103:9336-44.
36. Freitas VLS, Gomes JRB, Ribeiro da Silva MDRS. Energetics and reactivity of morpholine
and thiomorpholine: A joint experimental and computational study. J Chem Eng Data. 2014;59:312-
22.
37. Jiménez P, Roux MV, Turrión C. Thermochemical properties of N-heterocyclic compounds I.
Enthalpies of combustion, vapour pressures and enthalpies of sublimation, and enthalpies of
formation of pyrazole, imidazole, indazole, and benzimidazole. J Chem Thermodyn. 1987;19:985-
92.
38. Freitas VLS, Monte MJS, Santos LMNBF, Gomes JRB, Ribeiro da Silva MDMC. Energetic
studies and phase diagram of thioxanthene. J Phys Chem A. 2009;113:12988-94.
39. NIST Computational Chemistry Comparison and Benchmark Database, NIST Standard
Reference Database Number 101, Release 16a, August 2013, Editor: Russell D. Johnson III
(http://cccbdb.nist.gov/).