Structure determination of ylid with the Bruker SMART X2S benchtop crystallographic system
A yellow
crystal of ylid with the dimensions of 0.79 mm x 0.81 mm x 0.82 mm mounted on a Mitegen Micromount was automatically
centered on a Bruker SMART X2S benchtop crystallographic system. Intensity
measurements were performed using a monochromated (Doubly Curved Silicon
Crystal) Mo-Kα-radiation (0.71073 Å) from a sealed MicroFocus tube.
Generator settings were 50 kV, 1 mA. Data collection temperature was 23°C.
Data were acquired using three sets of Omega
scans at different Phi settings. The frame width was 0.5°
with an exposure time of 5.0 s.
The detailed data collection strategy was as follows:
Detector distance: 40 mm
Detector swing angle (fixed 2 Theta): -20°.
|
Run |
Omega (start) |
Omega (end) |
Phi |
Frames |
|
1 |
-20.0 |
-200.0 |
0.0 |
360 |
|
2 |
-20.0 |
-140.0 |
120.0 |
240 |
|
3 |
-20.0 |
-80.0 |
240.0 |
120 |
APEX2 software was used for preliminary determination of the unit cell. Determination
of integral intensities and unit cell refinement were performed using SAINT.
The integration of the data yielded a total of 6275 reflections
to a maximum θ angle of 25.10° (0.84
Å resolution).
The constants for the orthorhombic unit cell are a = 5.9732(9) Å, b = 9.0529(13) Å,
c = 18.431(3) Å, V = 996.7(3)
Å3. They are based upon the refinement
of the XYZ-centroids of 2872 reflections above 20.0
I/σ(I) with 2.21° ≤ θ ≤ 24.96°.
Data were corrected for absorption effects with SADABS using
the multiscan technique. The ratio of minimum to maximum apparent transmission
is 89.8:100. The average
residual for symmetry equivalent reflections is Rint = 3.15% and Rσ = 2.83%.
XPREP determined the space group to be P
21 21 21, with Z = 4 for the formula unit, C11H10O2S.
The structure was solved with XS and
subsequent structure refinements were performed with XL. The final anisotropic
full-matrix least-squares refinement on Fo2 with 130 variables converged at R1 = 2.80% for the observed data and wR2 = 9.24% for all data. The goodness-of-fit was 1.195. The largest peak on the final difference electron
density synthesis was 0.22 e-/Å3
and the deepest hole was -0.16 e-/Å3
with an RMS deviation of 0.05 e-/Å3.
On the basis of the final model, the calculated density is 1.375
g/cm3 and F(000) = 432.
APEX2 Version 2.2 (Bruker AXS
Inc., 2007)
SAINT Version 7.34a (Bruker AXS Inc., 2007)
SADABS Version 2007/2 (Sheldrick, Bruker AXS Inc.)
XPREP Version 2005/2 (Sheldrick, Bruker AXS Inc.)
XS Version 2008/1 (George M. Sheldrick, Acta Cryst. (2008). A64,
112-122)
XL Version 2008/1 (George M. Sheldrick, Acta Cryst. (2008). A64,
112-122)
|
|
|
|
Table 1. |
|
Identification
code |
ylid |
|
|
Empirical
formula |
C11 H10 O2 S |
|
|
Formula weight |
206.25 |
|
|
Temperature |
296(2) K |
|
|
Wavelength |
0.71073 Å |
|
|
|
Orthorhombic |
|
|
Space group |
P 21 21 21 |
|
|
Unit cell
dimensions |
a = 5.9732(9) Å |
α = 90° |
|
|
b = 9.0529(13) Å |
β = 90° |
|
|
c = 18.431(3) Å |
γ = 90° |
|
Volume |
996.7(3) Å3 |
|
|
Z |
4 |
|
|
Density
(calculated) |
1.375 Mg/cm3 |
|
|
Absorption
coefficient |
0.293 mm-1 |
|
|
F(000) |
432 |
|
|
|
0.79 x 0.81 x 0.82 mm3 |
|
|
Theta range for
data collection |
2.21 to 24.96° |
|
|
Index ranges |
-6<=h<=7, -10<=k<=10, -21<=l<=22 |
|
|
Reflections
collected |
6275 |
|
|
Independent
reflections |
1766 [R(int) = 0.0315] |
|
|
Completeness to
theta = 24.96° |
99.7% |
|
|
Absorption
correction |
Multiscan |
|
|
Max. and min.
transmission |
0.8016 and 0.7197 |
|
|
Refinement
method |
Full-matrix least-squares on F2 |
|
|
Data /
restraints / parameters |
1766 / 0 / 130 |
|
|
Goodness-of-fit
on F2 |
1.195 |
|
|
Final R indices
[I>2sigma(I)] |
R1 = 0.0280, wR2 = 0.0731 |
|
|
R indices (all
data) |
R1 = 0.0335, wR2 = 0.0924 |
|
|
Absolute
structure parameter |
0.02(9) |
|
|
Extinction
coefficient |
0.035(5) |
|
|
Largest diff.
peak and hole |
0.215 and -0.163 |
|
Rint = Σ|Fo2 - Fo2(mean)|
/ Σ[Fo2]
R1 = Σ||Fo| - |Fc|| / Σ|Fo|
GOOF = S = {Σ[w(Fo2 - Fc2)2]
/ (n - p)}1/2
wR2 = {Σ[w(Fo2 - Fc2)2]
/ Σ[w(Fo2)2]}1/2
w = 1 / [σ(Fo2) + (aP)2 +
bP] where P is [2Fc2 + Max(Fo2,
0)] / 3
|
Table 2. Atomic coordinates (x104) and equivalent isotropic displacement parameters (Å2x103) for ylid. |
|
U(eq) is defined as one third of the trace of the orthogonalized Uij tensor. |
|
|
|
|
x |
y |
z |
U(eq) |
|
S1 |
-1903(1) |
-8186(1) |
-7405(1) |
38(1) |
|
O1 |
-1587(3) |
-10890(2) |
-6292(1) |
52(1) |
|
O2 |
-6644(3) |
-6979(2) |
-6769(1) |
49(1) |
|
C1 |
-3506(6) |
-8239(3) |
-8227(1) |
60(1) |
|
C6 |
-7000(6) |
-10611(3) |
-4628(1) |
59(1) |
|
C10 |
-8499(5) |
-9509(3) |
-4777(1) |
56(1) |
|
C5 |
-5136(5) |
-10876(2) |
-5075(1) |
50(1) |
|
C7 |
-1646(5) |
-6233(2) |
-7292(1) |
49(1) |
|
C9 |
-8225(5) |
-8598(3) |
-5381(1) |
48(1) |
|
C4 |
-4896(4) |
-9978(2) |
-5681(1) |
38(1) |
|
C8 |
-6426(4) |
-8856(2) |
-5823(1) |
37(1) |
|
C3 |
-3105(4) |
-9989(2) |
-6253(1) |
36(1) |
|
C2 |
-3645(4) |
-8758(2) |
-6720(1) |
35(1) |
|
C11 |
-5657(4) |
-8053(3) |
-6498(1) |
36(1) |
|
Table 3. Bond lengths (Å) and angles (°) for ylid. |
|
S1-C2 |
1.716(2) |
|
S1-C7 |
1.787(2) |
|
S1-C1 |
1.794(3) |
|
O1-C3 |
1.222(3) |
|
O2-C11 |
1.242(3) |
|
C6-C10 |
1.368(4) |
|
C6-C5 |
1.406(4) |
|
C10-C9 |
1.395(3) |
|
C5-C4 |
1.389(3) |
|
C9-C8 |
1.368(3) |
|
C4-C8 |
1.391(3) |
|
C4-C3 |
1.502(3) |
|
C8-C11 |
1.513(3) |
|
C3-C2 |
1.444(3) |
|
C2-C11 |
1.421(3) |
|
|
|
|
C2-S1-C7 |
105.36(11) |
|
C2-S1-C1 |
106.86(13) |
|
C7-S1-C1 |
99.82(13) |
|
C10-C6-C5 |
121.7(2) |
|
C6-C10-C9 |
121.0(3) |
|
C4-C5-C6 |
116.9(2) |
|
C8-C9-C10 |
117.8(3) |
|
C5-C4-C8 |
120.7(2) |
|
C5-C4-C3 |
129.4(2) |
|
C8-C4-C3 |
109.96(18) |
|
C9-C8-C4 |
122.0(2) |
|
C9-C8-C11 |
130.2(2) |
|
C4-C8-C11 |
107.8(2) |
|
O1-C3-C2 |
130.2(2) |
|
O1-C3-C4 |
125.0(2) |
|
C2-C3-C4 |
104.7(2) |
|
C11-C2-C3 |
111.4(2) |
|
C11-C2-S1 |
126.08(17) |
|
C3-C2-S1 |
122.38(17) |
|
O2-C11-C2 |
129.6(2) |
|
O2-C11-C8 |
124.2(2) |
|
C2-C11-C8 |
106.1(2) |
|
Table 4. Anisotropic displacement parameters (Å2x103) for ylid. |
|
The anisotropic displacement factor exponent takes the form: -2π2[ h2 a*2 U11 + ... + 2 h k a* b* U12 ] |
|
|
U11 |
U22 |
U33 |
U23 |
U13 |
U12 |
|
S1 |
40(1) |
34(1) |
40(1) |
4(1) |
9(1) |
5(1) |
|
O1 |
59(1) |
44(1) |
52(1) |
10(1) |
9(1) |
17(1) |
|
O2 |
42(1) |
48(1) |
57(1) |
12(1) |
1(1) |
11(1) |
|
C1 |
87(2) |
55(2) |
37(1) |
2(1) |
-2(1) |
-3(2) |
|
C6 |
92(2) |
47(1) |
38(1) |
-1(1) |
19(2) |
-15(2) |
|
C10 |
65(2) |
56(2) |
47(1) |
-8(1) |
24(1) |
-12(2) |
|
C5 |
73(2) |
37(1) |
38(1) |
3(1) |
7(1) |
-1(1) |
|
C7 |
49(2) |
37(1) |
61(1) |
2(1) |
12(1) |
-10(1) |
|
C9 |
44(1) |
51(1) |
48(1) |
-5(1) |
9(1) |
-6(1) |
|
C4 |
50(2) |
31(1) |
32(1) |
-4(1) |
3(1) |
-5(1) |
|
C8 |
40(1) |
36(1) |
34(1) |
-4(1) |
1(1) |
-8(1) |
|
C3 |
44(1) |
31(1) |
35(1) |
-0(1) |
0(1) |
1(1) |
|
C2 |
39(1) |
34(1) |
34(1) |
3(1) |
3(1) |
-1(1) |
|
C11 |
34(1) |
34(1) |
39(1) |
0(1) |
-3(1) |
-3(1) |
|
Table 5. Hydrogen coordinates (x104) and isotropic displacement parameters (Å2x103) for ylid. |
|
|
x |
y |
z |
U(eq) |
|
H1A |
-3695 |
-9247 |
-8378 |
90 |
|
H1B |
-2734 |
-7699 |
-8599 |
90 |
|
H1C |
-4947 |
-7801 |
-8145 |
90 |
|
H6 |
-7220 |
-11199 |
-4220 |
71 |
|
H10 |
-9718 |
-9365 |
-4471 |
67 |
|
H5 |
-4111 |
-11619 |
-4970 |
59 |
|
H7A |
-3108 |
-5793 |
-7286 |
73 |
|
H7B |
-793 |
-5830 |
-7686 |
73 |
|
H7C |
-899 |
-6026 |
-6842 |
73 |
|
H9 |
-9232 |
-7841 |
-5480 |
57 |