Angewandte
Chemie
Since the molar extinction coefficient for [RuL3]2+ com-
plexes are high (17000mÀ1 cmÀ1 for [Ru(dmb)3]2+), we con-
sidered the possibility that the reaction was light-starved and
the light source thus fails to irradiate the entire volume of the
solution.[18] A simple analysis of the absorption profile of
a theoretical vessel using the Beer–Lambert law at relevant
concentrations of [Ru(dmb)3]2+ is shown in Figure 1. This
Figure 2. Diagram of the designed photoflow reactor.
modules to be connected in series to increase residence time
without decreasing the flow rate.
By running the reaction depicted in Scheme 2, the
efficiency of the photoflow reactor was examined for different
concentrations of [Ru(dmb)3]2+ using two different tubing
diameters (Figure 3). For tubing having a 1.6 mm interior
diameter and 1.1 mm [Ru(dmb)3]2+ a TOF of 30 hÀ1 was
Figure 1. The percent transmittance versus distance from the wall (d)
2+
*
as calculated from the Beer–Lambert law. 0.5 mm [Ru(dmb)3]
,
2+
2+
~
&
1 mm [Ru(dmb)3]
,
2 mm [Ru(dmb)3] .
analysis indicates that the vast majority of the reaction vessel
receives negligible amounts of light. At a catalyst concen-
tration of 1 mm, 98% of the incident light is absorbed within
1 mm of the vessel wall, while at 2 mm, this occurs within
0.5 mm. Since the light initiates the cascade of events that
leads to free radical generation, the “active volume” is
effectively determined by the surface area of the glass being
irradiated; the remaining volume is not effectively irradiated.
This analysis suggests that decreasing the diameter of the
reaction vessel should increase the flux of photons throughout
the vessel and thereby increase the effective concentration of
active catalyst and thus the rate of the reaction. The data in
Figure 1 suggest that achieving reasonable irradiation of the
entire reaction volume would require a vessel having a sub-
millimeter diameter. Our solution to the problem of obtaining
sufficiently thin diameters without sacrificing reactor volume
was a photoflow reactor, which allows the continuous
irradiation of a reaction mixture as it flows around a light
source.
The basic design principle was initially demonstrated by
Booker-Milburn,[11a] and several other examples of photoflow
reactors for UV-light irradiation have since been
reported.[10,11] As a result of the weak absorptivity of the
reactants in these examples, these reactors are limited only by
the flux of the light source and benefit from tubing with
a thicker diameter and multiple layers of wrapping around the
light source. In contrast, the above analysis suggested the
optimal design would utilize tubing with a thin diameter and
a single wrap around the light source.
Figure 3. TOF versus [Ru(dmb)3]2+ for FEP tubing of two different
inner diameters.
obtained with one module. At the same flow rate of
0.1 mLminÀ1 and an increased [Ru(dmb)3]2+ concentration
(2.2 mm) the rate of conversion was lower (TOF = 17 hÀ1),
whereas a lowered concentration increased the rate (TOF =
50 hÀ1 at 0.5 mm). Consistent with the analysis in Figure 1, the
reaction rate increased upon decreasing the inner diameter of
the FEP tubing, that is, at 1.1 mm [Ru(dmb)32+] and with
tubing having an inner diameter of 0.8 mm the TOF was
72 hÀ1. Again, an inverse relationship between catalyst
concentration and TOF was observed, with 0.5 mm [Ru-
(dmb)3]2+ giving the highest observed TOF (120 hÀ1). These
flow reactions demonstrated higher TOFs than either the
flask or batch reactor. More importantly, the TOFs increase
significantly with decreasing tubing diameter, thus supporting
the prediction provided from the data in Figure 1 of a photon-
starved reaction. Decreasing the catalyst concentrations also
led to an increase in the TOF, which is consistent with
a previously photon-starved reaction which now enjoys an
increase in photon flux throughout the diameter of the
vessel.[20,21]
As shown in Figure 2, our simple design utilizes clear
fluorinated ethylene propylene (FEP)[19] tubing coiled once
around a Liebigs condenser, three strips of blue LEDs placed
inside the condenser, cool water passing through the con-
denser jacket for temperature control, and a flow rate that is
controlled by the pump of a preparatory HPLC. The ends of
the tubing are fitted to Swagelok connectors, which enable the
For our final reactor design, we chose a FEP tubing with
a 1.6 mm inner diameter and a concentration of 1 mm
Angew. Chem. Int. Ed. 2012, 51, 4140 –4143
ꢀ 2012 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
4141