Just Because It’s Small Doesn’t Mean It’s Well Mixed: Ensuring
Good Mixing in Mesoscale Reactors
J. F. Hall,
†,‡
M. Barigou,
†
M. J. H. Simmons,*
,†
and E. H. Stitt
§
Centre for Formulation Engineering, Department of Chemical Engineering, University of Birmingham,
Edgbaston, Birmingham B15 2TT, U.K., and Johnson Matthey Catalysts, P. O. Box 1, Belasis Avenue,
Billingham, Cleveland TS23 1LB, U.K.
The advent of high throughput experimentation (HTE) for molecular discovery and rapid
screening of new catalyst formulations has led to interest in the mixing characteristics of small
stirred vessels at scales below those previously studied. In this paper, particle image velocimetry
(PIV) is used to obtain macromixing characteristics for single phase fluids of two different
viscosities (µ ) 0.001 and 0.433 Pa s) and for two-phase air-water mixtures in a 45 mm diameter
vessel using a 6 blade up-pumping pitched-blade turbine. Eccentric agitation is examined as a
means of improving the mixing performance since the vessels are used without baffles, and the
global circulation of the fluid was comparable with that of a conventional baffled configuration
for single-phase mixing at a constant power input per unit mass (0.168-5.5 W kg
-1
). For high
viscosity fluids, the characteristic flow patterns resembled those for a radial device. For two-
phase mixing at gassing rates of 0.25 and 0.5 vvm, two sparger configurations were used with
the sparger being placed either beneath the impeller axis (R) or away from the impeller (). The
configuration appeared to be a better choice because of the smaller size of bubbles generated
compared with the R configuration and the satisfactory levels of global mixing observed in the
vessel.
1. Introduction
The control of the degree and rapidity of mixing is
essential for the successful operation of any industrial
process. The complex nature of the flow field within
most industrial equipment, in particular, the ubiquitous
stirred tank, has led to considerable research effort to
obtain an understanding of the mixing length-scales and
time-scales of both single and multiphase mixtures.
Several books have been written on the subject.
1-3
The
general approach taken for the translation of a devel-
opmental process from the initial laboratory scale to the
industrial scale of production is to attempt to mimic the
operational conditions in the pilot vessel at the produc-
tion scale. This has been a perfectly valid assumption
for scenarios involving the development and testing of
a process at vessel scales on the order of 10
-3
to 10
-2
m
3
upward, as the large number of previous studies
(both academic and industrial) have proved.
However, the advent of revolutionary high throughput
experimentation (HTE) techniques requires a reexami-
nation of this approach. HTE offers the potential to
dramatically reduce the time-scales currently required
for the screening of novel molecules and catalysts, and
as such, significant benefits are anticipated via the
implementation of the HTE protocol in the worldwide
chemicals industry. Many commercially available HTE
units are based upon small agitated stirred vessels with
typical volumes of 10
-5
to 10
-4
m
3
, an order of magni-
tude below existing well-researched lab-scale mixers.
The mixing performance of these units is not optimal
because of two primary factors:
4-6
First, the small scale
of the reactors precludes the generation of high Rey-
nolds numbers, even at high agitation speeds. Second,
the HTE reaction vessels are generally unbaffled, to
facilitate automated loading and cleaning cycles by
robotic server units, as well as to prevent fouling/con-
tamination and excessive particle attrition. Without baf-
fles to break up the dominant tangential flow, efficient
mixing cannot be achieved in conventional unbaffled
vessels where the impeller shaft is placed at the vessel
axis. Since decisions regarding the viability of a certain
process or operating condition requirements are often
made based on the information generated by the HTE
unit, it is vital that the hydrodynamic behavior and fluid
mixing performance of these small vessels are fully
quantified. Without this information, there is no way
for the operator to discern the parametric sensitivity of
the process under investigation and differentiation be-
tween mass transfer effects and/or kinetic effects be-
comes impossible.
Studies by previous authors based upon conventional
vessel configurations at the laboratory and pilot scale
(H ) T, C )
1
/
3
H, D )
1
/
3
T, fully baffled conditions) for
both radial and axial impeller types using flow visual-
ization techniques and computational fluid dynamics
have characterized the macroflow behavior in terms of
mean flow patterns,
7-12
the microflow qualities in terms
of the turbulence parameters,
13-18
and the mixing per-
formance in terms of the concentration fields.
19-23
Laser
Doppler velocimetry (LDV) and particle image veloci-
metry (PIV), in particular, have enabled researchers to
obtain high-resolution velocity fields and, hence, develop
a thorough understanding of both the global flow
patterns and the behaviour of the fluid within the highly
energetic regions, such as the impeller discharge jet.
* Corresponding author. Dr. Mark Simmons. Tel.: +44 (0)
121 4145371. E-mail: m.j.simmons@bham.ac.uk.
†
University of Birmingham.
‡
Current address: Johnson Matthey Catalysts, P. O. Box
1, Belasis Ave, Billingham TS23 1LB, U.K.
§
Johnson Matthey Catalysts.
9695 Ind. Eng. Chem. Res. 2005, 44, 9695-9704
10.1021/ie050224w CCC: $30.25 © 2005 American Chemical Society
Published on Web 07/08/2005