Janine Chungyin Cheng’s research while affiliated with Iowa State University and other places

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Publications (5)


Figure 1. The FNP process. 
Figure 2. Schematic (top left) and photograph (top right) of the MIVM and schematic of the μ -PIV setup (bottom). 
Table 2 . Time between pulses chosen at different Re j and corresponding uncertainty due to Brownian motion.
Figure 3. Instantaneous velocity field at the midplane (top left), and mean tangential (top right) and radial (bottom) velocity profiles of center lines at three data acquisition planes at Re j = 53. In the legend, m ( ) represents the midplane, q2b ( ♦ ) the quarter-of-reactor-height- to-bottom plane and q2t ( ) the quarter-of-reactor-height-to-top plane. 
Figure 4. Instantaneous velocity field at the midplane (top), and mean tangential (middle) and radial (bottom) velocity profiles of center lines at three data acquisition planes at Re j = 93. 

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Measurements of turbulence in a microscale multi-inlet vortex nanoprecipitation reactor
  • Article
  • Full-text available

June 2013

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517 Reads

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26 Citations

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Janine Chungyin Cheng

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The microscale multi-inlet vortex reactor (MIVR) is designed for use in Flash NanoPrecipitation (FNP), a promising technique for producing nanoparticles within small particle size distribution. Fluid mixing is crucial in the FNP process, and due to mixing's strong dependence upon fluid kinematics, investigating velocity and turbulence within the reactor is crucial to optimizing reactor design. To this end, microscopic particle image velocimetry has been used to investigate flow within the MIVR. Three Reynolds numbers are studied, namely, Rej = 53, 93 and 240. At Rej = 53, the flow is laminar and steady. Due to the strong viscous effects at this Reynolds number, distinct flow patterns are observed at different distances from the reactor top and bottom walls. The viscous effects also retard the tangential motions within the reactor, resulting in a weaker vortex than appears at the higher Reynolds numbers. As the Reynolds number is increased to 93, the flow becomes more homogeneous over the depth of the reactor due to weaker viscous effects, yet the flow is still steady. The diminishing effects of viscosity also result in a stronger vortex. At the highest Reynolds number investigated, the flow is turbulent. Turbulent statistics including tangential and radial velocity fluctuations and Reynolds shear stresses are analyzed for this case in addition to the mean velocity field. The tangential motions of the flow are strongest at Rej = 240. Both the tangential and radial velocity fluctuations increase as the flow spirals toward the center of the reactor. The magnitudes of the tangential and radial velocity fluctuations are similar, suggesting that the turbulence is locally isotropic.

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A competitive aggregation model for Flash NanoPrecipitation

November 2010

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25 Reads

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62 Citations

Journal of Colloid and Interface Science

Flash NanoPrecipitation (FNP) is a novel approach for producing functional nanoparticles stabilized by amphiphilic block copolymers. FNP involves the rapid mixing of a hydrophobic active (organic) and an amphiphilic di-block copolymer with a non-solvent (water) and subsequent co-precipitation of nanoparticles composed of both the organic and copolymer. During this process, the particle size distribution (PSD) is frozen and stabilized by the hydrophilic portion of the amphiphilic di-block copolymer residing on the particle surface. That is, the particle growth is kinetically arrested and thus a narrow PSD can be attained. To model the co-precipitation process, a bivariate population balance equation (PBE) has been formulated to account for the competitive aggregation of the organic and copolymer versus pure organic-organic or copolymer-copolymer aggregation. Aggregation rate kernels have been derived to account for the major aggregation events: free coupling, unimer insertion, and aggregate fusion. The resulting PBE is solved both by direct integration and by using the conditional quadrature method of moments (CQMOM). By solving the competitive aggregation model under well-mixed conditions, it is demonstrated that the PSD is controlled primarily by the copolymer-copolymer aggregation process and that the energy barrier to aggregate fusion plays a key role in determining the PSD. It is also shown that the characteristic aggregation times are smaller than the turbulent mixing time so that the FNP process is always mixing limited.


Kinetic Modeling of Nanoprecipitation using CFD Coupled with a Population Balance

August 2010

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70 Reads

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62 Citations

Industrial & Engineering Chemistry Research

A model study has been conducted for Flash Nanoprecipitation (FNP)—a novel approach to produce functional nanoparticles. A population balance equation with the FNP kinetics has been integrated into a computational fluid dynamics (CFD) simulation of a custom-designed microscale multi-inlet vortex reactor (MIVR) to yield conditions comparable to the real experimental settings. In coping with the complicated aggregation model in the CFD code, a new numerical approach, the conditional quadrature method of moments (CQMOM), has been proposed, which is capable of solving the multivariate system efficiently and accurately. It is shown that the FNP process is highly influenced by mixing effects in the microreactor, and thus coupling CFD with the kinetics model is essential in obtaining valid comparisons with experiments.


A comrehensive model study for Flash Nanoprecipitation: computational fluid dynamics, micro- particle image velocimetry, and population balance modeling

January 2010

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23 Reads

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1 Citation

A model study has been conducted for Flash Nanoprecipitation(FNP)) - a novel approach to produce functional nanoparticles. A mixing study has been conducted in a custom-designed microscale multi-inlet vortex reactor (MIVR) and a scalar mixing model was validated against experimental data. A microPIV experiment was conducted to further validate the turbulent model. A population balance equation (PBE) has been proposed to model the FNP process. It was furthermore, integrated into a computational fluid dynamics (CFD) simulation of to yield conditions comparable to the real experimental settings. In coping with the complicated aggregation model in the CFD code, a new numerical approach, conditional quadrature method of moments (CQMOM), has been proposed, which is capable of solving the multivariate system efficiently and accurately. It is shown that the FNP process is highly influenced by mixing effects in the microreactor and thus coupling CFD with the kinetics model is essential in obtaining valid comparisons with experiments.


A microscale multi-inlet vortex nanoprecipitation reactor: Turbulence measurement and simulation

May 2009

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76 Reads

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59 Citations

Microscale reactors capable of generating turbulent flow are used in Flash NanoPrecipitation, an approach to produce functional nanoparticles with unique optical, mechanical and chemical properties. Microreactor design and optimization could be greatly enhanced by developing reliable computational models of the nanoprecipitation process. A microscale multi-inlet vortex nanoprecipitation reactor was investigated using microscopic particle image velocimetry and computational fluid dynamics. Velocity data such as the mean velocity and turbulent kinetic energy displayed good agreement between experiment and simulation over flow conditions ranging from fully laminar to turbulent, demonstrating the accuracy of the simulation model over the entire turbulent transition range.

Citations (4)


... As a further development of the nanoprecipitation method in advanced LCHNPs fabrication, macro-scale devices, called Multi-Inlet Vortex Reactors (MIVRs), can be used. [94][95][96] The device can be made with either two or four radially symmetric inlets that lead into a circular reaction chamber (Fig. 6B). Rapid nanoprecipitation, with high production and improved size homogeneity, can be achieved to form polymeric particles with an organic phase containing the polymer, and an aqueous phase acting as the anti-solvent is added into separate inlets. ...

Reference:

Therapeutic lipid-coated hybrid nanoparticles against bacterial infections
Measurements of turbulence in a microscale multi-inlet vortex nanoprecipitation reactor

... There are few references in the literature regarding the application of CFD + PBM for nanoparticle production processes (~10 1 -10 2 nm), particularly involving high-shear agitators [45]. The existing studies primarily focus on supercritical anti-solvent [46] and flash nanoprecipitation processes [47,48]. For microcapsule production via continuous emulsion, CFD + PBM approaches have been employed to determine power consumption scale-up parameters [49]. ...

Kinetic Modeling of Nanoprecipitation using CFD Coupled with a Population Balance
  • Citing Article
  • August 2010

Industrial & Engineering Chemistry Research

... The contribution from the various mechanisms can be captured additively in the expression for β (e.g., see [231,235,236]). For modeling flash nanoprecipitation, a process closely related to LNP production, Cheng et al. [237] and Cheng & Fox [238] developed an aggregation model that incorporates significant mechanistic insight of the agglomeration process specific to polymeric nanoparticles containing a diblock copolymer. ...

A competitive aggregation model for Flash NanoPrecipitation
  • Citing Article
  • November 2010

Journal of Colloid and Interface Science