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HONO2 |
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Deuterium
and Nitrogen
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Nuclear
Quadrupole Coupling Constants |
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in
Nitric Acid |
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Deuterium and nitrogen nqcc's in
normal and isotopic nitric acid have been reported by Ott et al. [1],
Fliege et al. [2], and Albinus et al. [3]. Molecular structures
were determined by Cox and Riveros [4], Cox et al. [5], Ghosh et al.
[6], and Gutle et al. [7]. |
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Calculation was made here of
the deuterium and nitrogen nqcc's on the equilibrium structure of Gutle
et al. These are compared with the experimental nqcc's in Tables
1 - 7. Equilibrium structure parameters are given in Table 8. |
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In Tables 1 - 7, subscripts a,b,c
refer to the principal axes of the inertia tensor, subscripts x,y,z to
the principal axes of the nqcc tensor. The nqcc y-axis is chosen
coincident with the inertia c-axis, these are perpendicular to the
plane of the molecule. Ø (degrees) is the angle between
its subscripted parameters. ETA = (Xxx - Xyy)/Xzz. |
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RMS is the root mean square
difference between calculated and experimental diagonal nqcc's
(percentage of the average of the magnitudes of the experimental
nqcc's). RSD is the calibration residual standard deviation of
the model for calculation of the nqcc's: B3LYP/6-31G(df,3p) for
deuterium, and B3PW91/6-311+G(df,pd) for nitrogen. |
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Table 1. Deuterium nqcc's
in DONO2 (kHz). Calculation was made on the re
structure [7]. |
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Calc. |
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Expt. [1] |
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2H |
Xaa |
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37.5 |
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35.0(16) |
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Xbb |
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118.8 |
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113.6 * |
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Xcc |
- |
156.3 |
- |
148.6 * |
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|Xab| |
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179.4 |
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RMS |
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5.6 (5.6 %) |
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RSD |
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1.1 (0.9 %) |
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Xxx |
- |
105.8 |
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Xyy |
- |
156.3 |
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Xzz |
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262.1 |
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ETA |
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0.193 |
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Øz,a |
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128.61 |
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Øa,OD |
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127.35 |
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Øz,OD |
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1.26 |
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* Calculated here from Xaa
(= - Xbb - Xcc) and Xbb -
Xcc = 262.2(60) kHz [1]. |
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Table 2. Deuterium nqcc's
in DO15NO2 (kHz). Calculation was made
on the re structure [7]. |
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Calc. |
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Expt. [2] |
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2H |
Xaa |
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37.2 |
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31.1(24) |
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Xbb |
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119.2 |
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118.5(29) |
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Xcc |
- |
156.3 |
- |
149.6(29) |
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|Xab| |
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179.3 |
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RMS |
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5.2 (5.3 %) |
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RSD |
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1.1 (0.9 %) |
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Table 3. 14N nqcc's in DONO2
(MHz). Calculation was made on the re structure
[7]. |
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Calc. |
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Expt. [1] |
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Expt. [3] |
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Xaa |
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0.702 |
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0.7266(36) |
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0.7311(56) |
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Xbb |
- |
0.595 |
- |
0.64885 * |
- |
0.6534(81) |
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Xcc |
- |
0.107 |
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0.07775 * |
- |
0.0777(81) |
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|Xab| |
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0.873 |
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RMS |
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0.038 (7.8 %) |
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0.041 (8.4 %) |
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RSD |
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0.030 (1.3 %) |
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0.030 (1.3 %) |
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* Calculated here from Xaa
(= - Xbb - Xcc) and Xbb -
Xcc = - 0.5711(62) MHz [1]. |
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Table 4. 14N nqcc's in HONO2
(MHz). Calculation was made on the re
structure [7]. |
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Calc. |
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Expt. [1] |
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Expt. [3] |
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Xaa |
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0.914 |
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0.9450(51) |
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0.929(6) |
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Xbb |
- |
0.807 |
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0.86775 * |
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0.859(8) |
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Xcc |
- |
0.107 |
- |
0.07725 * |
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0.070(8) |
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|Xab| |
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0.665 |
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RMS |
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0.043 (6.8 %) |
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0.038 (6.1 %) |
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RSD |
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0.030 (1.3 %) |
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0.030 (1.3 %) |
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Xxx |
- |
1.034 |
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Xyy |
- |
0.107 |
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Xzz |
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1.141 |
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ETA |
- |
0.812 |
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Øz,a |
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18.85 |
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Øa,N-O |
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17.29 |
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Øz,N-O |
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1.56 |
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* Calculated here from Xaa
(= - Xbb - Xcc) and Xbb -
Xcc = - 0.7905(89) MHz [1]. |
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Table 5. 14N nqcc's in H18ONO2
(MHz). Calculation was made on the re structure
[7]. |
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Calc. |
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Expt. [1] |
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14N |
Xaa |
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1.085 |
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1.0820(54) |
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Xbb |
- |
0.978 |
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1.0045 * |
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Xcc |
- |
0.107 |
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0.0775 * |
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|Xab| |
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0.345 |
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RMS |
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0.023 (3.2 %)
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RSD |
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0.030 (1.3 %) |
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* Calculated here from Xaa
(= - Xbb - Xcc) and Xbb -
Xcc = - 0.927(11) MHz [1]. |
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Table 6. 14N nqcc's in syn-HONO18O
(MHz). Calculation was made on the re structure
[7]. (syn refers to 18O on the same side of the
molecule as H.) |
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Calc. |
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Expt. [1] |
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14N |
Xaa |
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0.746 |
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0.8002(55) |
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Xbb |
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0.639 |
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0.7121 * |
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Xcc |
- |
0.107 |
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0.0881 * |
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|Xab| |
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0.838 |
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RMS |
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0.053 (10.0 %) |
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RSD |
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0.030 (1.3 %) |
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* Calculated here from Xaa
(= - Xbb - Xcc) and Xbb -
Xcc = - 0.6240(91) MHz [1]. |
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Table 7. 14N nqcc's in anti-HONO18O
(MHz). Calculation was made on the re structure
[7]. (anti refers to 18O on the opposite side of the
molecule as H.) |
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Calc. |
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Expt. |
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14N |
Xaa |
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0.154 |
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Xbb |
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0.047 |
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Xcc |
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0.107 |
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|Xab| |
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1.083 |
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RSD |
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0.030 (1.3 %) |
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Table 8. Molecular
structure parameters, semi-experimental re [7] (Å and
degrees). |
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HO |
0.9683 |
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O-N |
1.3968 |
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N=Osyn |
1.2085 |
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N=Oanti |
1.1944 |
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HON |
102.22 |
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OsynNO |
115.80 |
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OantiNO |
114.15 |
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[1] M.E.Ott, M.B.Craddock, and
K.R.Leopold,
J.Mol.Spectrosc. 229,286(2005). |
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[2] E.Fliege, H.Dreizler,
S.Gerber, H.Huber, J.Mol.Spectrosc. 137,24(1989); E.Fliege and
H.Dreizler, Z.Naturforsch. 39a,630(1984). |
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[3] L.Albinus, J.Spieckermann,
and D.H.Sutter, J.Mol.Spectrosc. 133,128(1989). |
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[4] A.P.Cox and J.M.Riveros,
J.Chem.Phys. 42,3106(1965) |
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[5] A.P.Cox, M.C.Ellis, C.J.Attfield,
and A.C.Ferris, J.Mol.Struct. 320,91(1994) |
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[6] P.N.Ghosh, C.E.Blom, and
A.Bauder, J.Mol. Spectrosc.
89,159(1981) |
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[7] C.Gutle, J.Demaison, and
H.D.Rudolph, J.Mol.Spectrosc. 254,99(2009) |
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D.J.Millen and J.R.Morton, J.Chem.Soc. 1523(1960).
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ClNO3 |
CH3NO3 |
HCOOD |
CH2NOH |
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Table of Contents |
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Molecules/Deuterium |
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Molecules/Nitrogen |
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DNO3.html |
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Last
Modified 2 Feb 2009 |
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