Beilstein J. Org. Chem. 2019, 15, 1141–1148.
the monoclinic phase. Subsequent milling causes this phase to processed using FIT2D [30]. In situ real-time Raman data were
transform abruptly to the triclinic phase. Due to the inclusion of collected using a non-contact probe (beam diameter 1 mm) and
base catalyst in the final product, we suggest this difference to excitation wavelength of 785 nm. Raman scattering was
be the result of a templating effect, which dominates at higher collected on a RXN1TM analyzer (Kaiser Optical systems,
concentrations. For the reaction of meta- and ortho-substituted France), equipped with a CCD detector (1024 × 1024 pixel).
substrates, crystallization occurs directly into the monoclinic Each Raman spectrum consists of 5 s accumulated scattering in-
phase, regardless of milling conditions or catalyst concentra- tensity, with successive Raman spectra collected every 30 s.
tion.
Chemometrics: The Raman spectra were evaluated using prin-
Multivariate analysis of in situ Raman spectra by both PCA and ciple component analysis (PCA) and multivariate curve resolu-
MCR suggests the formation of a transient product with almost tion (MCR) with the software The Unscrambler® X Vers. 10.5
identical spectral properties as the final product, the triclinic (CAMO). Prior to multivariate analysis, Raman spectra were
polymorph of 3a. These results are consistent with those of baseline corrected followed by unit vector normalization in the
XRPD analysis. Hence, we here identify a new approach to spectral range of 200–2500 cm−1. PCA was conducted with
monitoring mechanically-induced polymorphic transitions in mean centered data using cross validation with 20 randomly
situ and in real-time.
selected segments. MCR iterations were initialized with the
constraints of "non-negative spectra" and "non-negative concen-
trations", and sensitivity to pure compounds was set to 100. The
Experimental
Materials: All chemicals used in this work were taken as maximum number of iterations was set at 250.
supplied (>97% purity), without further purification.
Mass spectrometry: Mass spectra were recorded with electro-
our previous work [29]. Milling experiments were performed Ultima ESI-TOF mass spectrometer (Micromass, Germany)
using a commercially available vibratory ball mill (Pulverisette running at 4 kV capillary voltage and a cone voltage of 35 V
2
3, Fritsch, Germany). For each experiment, stoichiometric was used. The collision energy was set to 5 eV. The source tem-
quantities of reactants p-, m- and o- fluorobenzaldehyde perature was 120 °C whereas the desolvation temperature was
500 mg, ca. 4.03 mmol) and malonodinitrile (266.1 mg, adjusted to 150 °C. The mass spectrometer was operating in
(
ca. 4.03 mmol) were weighed into Perspex milling jars (10 mL). positive ion mode. Around 0.1 mg of the samples were weigh-in
To each jar, a quantity (defined in the main text) of piperidine and solved in methanol (HPLC grade).
was added as catalyst. Two stainless steel milling balls (4 g,
1
0 mm diameter) were also included in each milling jar. The
Supporting Information
reactions were conducted at 30 Hz or 50 Hz, as indicated in the
main text. The final products were characterized by XRPD.
Supporting Information File 1
X-ray powder diffraction (XRPD): All samples were charac-
terized by XRPD analysis using a Bruker D8 diffractometer
with Cu-Kα1 radiation (λ = 1.54106 Å) in a range of 5.0° ≤ 2 θ
≤
40°. The data were obtained in transmission mode with a step
size of 0.009° and an acquisition time of 3 s per step.
ORCID® iDs
In situ investigations: In situ and real-time monitoring of the
milling reactions was conducted at the mySpot Beamline
(
BESSY II, Helmholtz Centre Berlin for Materials and Energy).
The same mechanochemical reactor was used for these investi-
gations, as was used for laboratory synthesis reactions; i.e., a References
Pulverisette 23, Fritsch, Germany. Perspex milling jars were
good quality XRPD data during milling reactions [14]. Diffrac-
tion was collected using an incident beam of 12.4 keV. 2D scat-
tering images were recorded on a MarMosaic, CCD detector
1. James, S. L.; Adams, C. J.; Bolm, C.; Braga, D.; Collier, P.; Friščić, T.;
Grepioni, F.; Harris, K. D. M.; Hyett, G.; Jones, W.; Krebs, A.; Mack, J.;
Maini, L.; Orpen, A. G.; Parkin, I. P.; Shearouse, W. C.; Steed, J. W.;
2.
(
resolution 3072 × 3072 pixel). All scattering data were
1147