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HCCCH2-CH2NC
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Nitrogen |
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Nuclear
Quadrupole Coupling Constants |
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in 4-Isocyano-1-Butyne
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The microwave spectrum of 4-isocyano-1-butyne has been investigated by Samdal et al. [1]. Hyperfine structure due to 14N quadrupole coupling, however, was not resolved.
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Calculation of the 14N
nuclear quadrupole coupling constant tensor in each of the following rotamers of the title molecule was made here on ropt molecular
structures given by CCSD(T)/cc-pVTZ
optimization [1]:
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antiperiplanar (ap)
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synclinal (sc)
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In Tables 1 and 2 - which show the calculated nqcc tensors - subscripts a,b,c refer to the
principal axes of the inertia tensor; x,y,z to the principal axes
of the nqcc tensor.
Ø (degrees) is the angle between its subscripted
parameters. ETA = (Xxx - Xyy)/Xzz. Structure parameters are given in Z-matrix format in Table 3.
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RSD is the calibration residual standard
deviation of the B3PW91/6-311+G(df,pd) model for calculation of the efg's/nqcc's. |
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Table 1. Nitrogen nqcc's in antiperiplanar 4-isocyano-1-butyne (MHz). Calculation was made
on CCSD(T)/cc-pVTZ ropt structure.
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Calc
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Expt
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14N |
Xaa |
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0.428
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Xbb |
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0.199
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Xcc |
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0.229
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|Xab| |
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0.213
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RSD
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0.030 (1.3 %)
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Xxx |
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0.265
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Xyy |
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0.229
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Xzz |
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0.494
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ETA
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0.0720
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Øz,a
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17.08
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Øa,NC |
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18.90
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Øz,NC |
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1.82
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Table 2. Nitrogen nqcc's in synclinal 4-isocyano-1-butyne (MHz). Calculation was made
on CCSD(T)/cc-pVTZ ropt structure.
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Calc
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Expt
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14N |
Xaa |
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0.077
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Xbb |
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0.269
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Xcc |
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0.192
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Xab |
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0.364
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Xac |
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0.120
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Xbc |
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0.160
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RSD
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0.030 (1.3 %)
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Xxx |
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0.311
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Xyy |
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0.242
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Xzz |
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0.553
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ETA
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0.125
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Øz,NC |
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0.86
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Table
3. 4-Isocyano-1-butyne CCSD(T)/cc-pVTZ optimized structure
parameters (Å and degrees). Atomic numbering is shown above.
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# B3PW91/6-311+G(df,pd) prop scf=tight
4-Isocyano-1-butyne
0 1
C
C 1 B1
C 2 B2 1 A1
C 3 B3
2 A2 1
D1 0
N 1 B4
2 A3 3
D2 0
C 5 B5
1 A4 2
D3 0
H 4 B6
3 A5 2
D4 0
H 1 B7
5 A6 6
D5 0
H 1 B8
5 A7 6
D6 0
H 2 B9
1 A8 5
D7 0
H 2 B10 1
A9 5 D8 0
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antiperiplanar
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synclinal
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B1 1.53492603
B2 1.46682670
B3 1.21111471
B4 1.42978854
B5 1.17751428
B6 1.06337150
B7 1.09007157
B8 1.09007157
B9 1.09202047
B10 1.09202047
A1 110.55121654
A2 178.29890253
A3 110.36658404
A4 178.35811225
A5 179.30177046
A6 108.66430699
A7 108.66430699
A8 109.31019027
A9 109.31019027
D1 0.00000000
D2 180.00000000
D3 0.00000000
D4 180.00000000
D5 121.15141637
D6 -121.15141637
D7 58.68480457
D8 -58.68480457
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B1 1.53442821
B2 1.46643296
B3 1.21077555
B4 1.42842221
B5 1.17754863
B6 1.06326916
B7 1.09034436
B8 1.09066723
B9 1.09229121
B10 1.09295557
A1 112.41270353
A2 178.75375597
A3 111.37157904
A4 178.74311071
A5 179.48024946
A6 108.35861205
A7 108.23136028
A8 109.21235695
A9 108.02316640
D1 8.96751387
D2 64.50025736
D3 2.02765262
D4 -119.35566306
D5 123.56175131
D6 -118.75566925
D7 -57.66765835
D8 -174.39676763
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[1] S.Samdal, H.Møllendal, and J.C.Guillemin, J.Phys.Chem. A 117,10304(2013).
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CH3NC
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HCCNC
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C6H5NC
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CNCN
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CH3CH2NC
| CH2=CHNC
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CF3NC
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Table of Contents |
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Molecules/Nitrogen |
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HCCCH2CH2NC.html |
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Last
Modified 17 Oct 2013 |
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