A virtual impactor aerosol concentrator has been developed that uses circumferential slots for acceleration of aerosol particles and for collection of the coarse fraction. This allows for accurate and economical machining of small slot widths, which leads to low-pressure losses for the separation process. One important application of the device is in the concentration of bioaerosols, especially for military field applications where minimization of power consumption is necessary. A prototype configuration of the circumferential slot virtual impactor (CSVI), which was designed using numerical methods, was constructed and tested. The device has a curvilinear slit nozzle with a diameter of 150.3 mm (5.918 in), which provides a total slot length of 472 mm. Its slot width was 0.499 mm (0.0197 in). According to Loo and Cork, for circular-jet virtual impactors the misalignment between the axis of the acceleration jet and the receiver nozzle will cause an increase in wall losses of about 1.6% for each 1% of misalignment. Measurements were made of the nozzle dimensions in the critical region of the CSVI that showed 1.8% relative misalignment. When this prototype was operated at a flowrate of 122 l/min and a flow fraction (minor air flowrate/total air-flowrate) of 10%, the cutpoint was 2.2 μm aerodynamic diameter and the corresponding cutpoint Stokes number was 0.58. The collection efficiency was greater than 72% for particle sizes larger than twice the cutpoint, up to the largest particle size tested (10 μm aerodynamic diameter). The peak collection efficiency was greater than 95%. For virtual impactors, a critical performance parameter is the loss of particulate matter to the inner walls of the system. For the prototype system, where numerical methods had been used to generate designs that reduced wall losses, the losses at the cutpoint size of 2.2 μm aerodynamic diameter, are approximately 3%. For an operational condition of a total flowrate of 122 l/min and a coarse particle flow fraction of 10%, the pressure drop across the major flow stream (fine particle stream) was 63 Pa (0.25 in of water), with an ideal power consumption of 0.14 watts.
[1]
L. Forney,et al.
Aerosol sizing with a slotted virtual impactor
,
1978
.
[2]
Q Wu,et al.
Intensities of E. coli nucleic acid Raman spectra excited selectively from whole cells with 251-nm light.
,
2000,
Analytical chemistry.
[3]
P. Koutrakis,et al.
DEVELOPMENT OF A DICHOTOMOUS SLIT NOZZLE VIRTUAL IMPACTOR
,
2000
.
[4]
B. T. Chen,et al.
An improved virtual impactor: design and performance
,
1987
.
[5]
P. Koutrakis,et al.
A HIGH-VOLUME SMALL CUTPOINT VIRTUAL IMPACTOR FOR SEPARATION OF ATMOSPHERIC PARTICULATE FROM GASEOUS POLLUTANTS
,
1994
.
[6]
B. T. Chen,et al.
A Study of Density Effect and Droplet Deformation in the TSI Aerodynamic Particle Sizer
,
1990
.
[7]
D. Blackstock.
Fundamentals of Physical Acoustics
,
2000
.
[8]
R. J. Han,et al.
Flow visualization inside a water model virtual impactor
,
1997
.
[9]
R J Sherwood,et al.
The cascade centripeter: a device for determining the concentration and size distribution of aerosols.
,
1965,
American Industrial Hygiene Association journal.
[10]
W. Conner.
An inertial-type particle separator for collecting large samples.
,
1966,
Journal of the Air Pollution Control Association.
[11]
Benjamin Y. H. Liu,et al.
Generation of monodisperse aerosol standards
,
1973
.