2
K.E. Sanwald et al. / Journal of Catalysis xxx (2016) xxx–xxx
prior to C–C-cleavage. On the other hand, photoreforming of linear
aldehydes was reported to involve sequential cleavage of formic
acid to form the C1-deficient aldehyde in a single reaction pathway
[19,29].
reactor at water level is 8.08 ꢀ 1017 sꢁ1 (k < 390 nm). Typically,
75 mg of photocatalyst were ultrasonically dispersed in 100 mL
of a 20 mM aqueous reactant solution. The system was deaerated
by four consecutive evacuations and Ar filling cycles. All reactions
were carried out at 288 K and an Ar pressure of 1 bar.
Evolved gases during photocatalytic reactions were analyzed
online via gas chromatography (Shimadzu, GC 2010 Plus) on a
Chromosorb 101 and a Molsieve 5 Å column with a TCD, FID and
a methanizer catalyst unit. Ar was used as a carrier gas.
During aerobic photooxidation of oxygenates, multiple reaction
pathways were accounted for by a two-site model for direct and
indirect mechanisms [30–32]. Holes trapped at surface lattice oxy-
gen sites [Tiꢀ ꢀ ꢀOꢀ ꢀ ꢀTi] abstract a H-atom from a C–H bond whereas
direct hole transfer yields alkoxy radicals chemisorbed on terminal
OH-groups. We hypothesize that under photoreforming conditions
(anaerobic environment and hydrogen evolving) similar mecha-
nisms operate, which determine the routes toward complete oxi-
dation. We have shown in a preceding contribution that the
anodic transformations of ethylene glycol during photoreforming
may be rationalized on this basis [18]. We further propose that
identical anodic transformations are followed across families of
compounds. However, the impact of molecular polyol structure
and associated surface adsorption complexes on the contribution
of the different reaction pathways to the complete oxidation is lar-
gely unknown.
Aliquots of the liquid-phase were manually taken at regular
times from the photocatalyst suspension via a sample valve. The
solid was separated by filtering through 0.2 lm nylon filters.
Liquid-phase species were quantitatively analyzed by 1H NMR
spectroscopy. Additionally, high-performance liquid chromatogra-
phy (HPLC) analysis was performed for photoreforming experi-
ments with C4–C6 oxygenates.
Reactant conversions XA were calculated according to XAð%Þ ¼
NA
ð1 ꢁ ðtÞÞ ꢀ 100, where NA(t) is the time-dependent molar amount
NA;0
of reactant A and NA,0 is the initial molar amount of reactant A,
i.e. present at the beginning of the reaction.
Here, we explore the mechanisms and kinetics of photoreform-
ing of C3–C6 polyols on benchmark TiO2 P 25 with Rh as co-catalyst.
On the basis of quantitative analysis of gas- and liquid-phase spe-
cies we establish general relationships between structural reactant
functional groups, anodic reaction pathways and oxidation mecha-
nisms. We provide rationalization of the impact of anodic surface
chemistry on the photoreforming kinetics in terms of oxygenate
conversion and associated H2-evolution rates.
2.2.2. 1H NMR analysis
For quantitative 1H NMR measurements reactor aliquots were
mixed in a 1:1 volume ratio with an external standard that con-
tained 20 mM 1,3,5-trihydroxybenzene in D2O adjusted to pH 3
with DCl. 1H NMR spectra with water signal suppression were
recorded at 305 K using an Avance III HD 500 System (Bruker Bios-
pin, Rheinstetten, Germany) with an UltraShield 500 MHz magnet
(11.75 T) and a BBI 500 S2 probe head (5 mm, inverse 1H/X with Z-
gradient). The resonance frequency of 1H was 500.13 MHz. The
spectra were acquired using the one-dimensional NOESY sequence
from the Bruker library ‘‘noesygppr1d” with presaturation of the
residual water signal during the relaxation delay and the mixing
time using spoil gradients. Longitudinal relaxation times (T1) were
determined by the inversion recovery pulse method. Relaxation
delay and acquisition time were set to 26 s and 4.1 s, respectively.
The sum of the latter corresponds to at least three times T1 of the
slowest relaxing 1H-nucleus (formic acid) and ensures quantitative
analysis. Typically, 64 or 128 scans, with 64 k data points were col-
lected. An exponential window function with a line broadening of
0.2 Hz was applied prior to Fourier transformation and the spectra
were manually phased, baseline corrected and integrated using
Mestre-C 8.1.1 software package. Liquid-phase species were iden-
tified according to their chemical shifts (referenced to the internal
standard, see SI-Table 1) and in comparison with spectra of com-
mercial references recorded under identical conditions. Overlap-
ping signals were deconvoluted using Lorentzian-Gaussian shape
type fitting functions. Quantification was done on the basis of the
integrated signal intensities which were further calibrated against
prepared solutions of known concentration in order to account for
signal damping due to the water-suppression in close proximity to
the water resonance frequency.
2. Experimental
A comprehensive list of compounds used during the study, and
detailed experimental procedures regarding the characterization of
the photocatalyst are compiled in the Supporting Information.
Briefly, experiments are conducted over AEROXIDEÒ TiO2 P 25
(referred to as TiO2 hereafter), commonly employed as benchmark
semiconductor, decorated with nanoparticulate Rh as a co-catalyst
(1 wt.% loading, particle size 1.9 nm ( 0.7 nm), dispersion 57%).
Further physicochemical properties of the materials are described
in the Supporting Information.
2.1. Photocatalyst preparation
The 1 wt.% Rh-decorated P 25 photocatalyst, hereafter referred
to as Rh/TiO2, was prepared via incipient wetness impregnation.
TiO2 P 25 was dried under a static air atmosphere at 473 K for
2 h prior to impregnation. Subsequently, the semiconductor was
treated with appropriate amounts of an aqueous solution of RhCl3-
ꢀxH2O in ultrapure water. The resulting precursor was kept in syn-
thetic air at 383 K for 1 h (100 mL minꢁ1, 5 K minꢁ1) and heated to
623 K (100 mL minꢁ1, 5 K minꢁ1) for 1 h. The material was allowed
to cool to room temperature before treatment in H2 at 623 K
(100 mL minꢁ1, 5 K minꢁ1) for 1 h. A TiO2 reference was prepared
subjecting as-received TiO2 P 25 to the same temperature and
gas treatments described before.
2.2.3. 13C NMR analysis
For 13C NMR measurements, reactor aliquots were again mixed
in a 1:1 volume ratio with D2O adjusted to pH 3 with DCl. 13C NMR
spectra were recorded at 300 K using an Avance III 500 System
(Bruker Biospin, Rheinstetten, Germany) with an UltraShield
500 MHz magnet (11.75 T) and a Cryo-QNP probe head (5 mm,
direct 13C/31P/29Si/19F with Z-gradient). The resonance frequency
of 13C was 125.07 MHz. The spectra were acquired using the one-
dimensional ‘‘zgpg” sequence from the Bruker library using
waltz16 1H-decoupling and a 30° 13C-pulse. Relaxation delay and
acquisition time were set to 4 s and 1.2 s, respectively. Typically,
1024 scans with 64 k data points were collected. An exponential
2.2. Photocatalytic test
2.2.1. Photoreforming experiments
Kinetic experiments were performed in a Pyrex top-irradiation
photo-reactor connected to a closed gas-circulation system [18].
The setup is equipped with facilities for online gas-analysis and
liquid-phase sampling. Irradiation is provided by a 300 W Xe lamp
with a cold mirror 1 (CM 1). A water filter with quartz windows
closes the top of the photo-reactor. The photon flux within the
Please cite this article in press as: K.E. Sanwald et al., Catalytic routes and oxidation mechanisms in photoreforming of polyols, J. Catal. (2016), http://dx.