Large Eddy Simulations (LESs) for a lean-direct injection (LDI) combustor are performed and compared
with experimental data. The LDI emissions characteristics, and radiation-spray coupling effect on the predictions
are analyzed. The flamelet progress variable approach is employed for chemistry tabulation coupled
with a stochastic secondary breakup model. Good comparisons are...
Large Eddy Simulations (LESs) for a lean-direct injection (LDI) combustor are performed and compared
with experimental data. The LDI emissions characteristics, and radiation-spray coupling effect on the predictions
are analyzed. The flamelet progress variable approach is employed for chemistry tabulation coupled
with a stochastic secondary breakup model. Good comparisons are...
In field studies of solute transport, transient storage within lateral cavities and other stream features generates
breakthrough curves (BTCs) with pronounced and persistent skewness. Current solute transport
theory requires that the coefficient of skewness (CSK) decrease over time because the system eventually
reaches Fickian conditions. However, published data show that...
Large Eddy Simulations (LESs) for a lean-direct injection (LDI) combustor are performed and compared
with experimental data. The LDI emissions characteristics, and radiation-spray coupling effect on the predictions
are analyzed. The flamelet progress variable approach is employed for chemistry tabulation coupled
with a stochastic secondary breakup model. Good comparisons are...
Surface transient storage (STS) and hyporheic transient storage (HTS) have functional significance in stream ecology and hydrology. Currently, tracer techniques couple STS and HTS effects on stream nutrient cycling; however, STS resides in localized areas of the surface stream and HTS resides in the hyporheic zone. These contrasting environments result...
Accurate estimates of mass-exchange parameters in transient storage zones are needed to better understand and quantify solute transport and dispersion in riverine systems. Currently, the predictive mean residence time relies on an empirical entrainment coefficient with a range in variance due to the absence of hydraulic and geomorphic quantities driving...
A numerical scheme for fully resolved simulation of particle–fluid systems with freely moving rigid particles is developed. The approach is based on a fictitious domain method wherein the entire particle–fluid domain is assumed to be an incompressible fluid but with variable density. The flow inside the particle domain is constrained...
The computation of Lagrangian coherent structures typically involves post-processing of experimentally or
numerically obtained fluid velocity fields to obtain the largest finite-time Lyapunov exponent (FTLE) field.
However, this procedure can be tedious for large-scale complex flows of general interest. In this work, an
alternative approach involving computation of the FTLE...
When a few bubbles are entrained in a travelling vortex ring, it has been shown that, even at extremely low volume loadings, their presence can significantly affect the structure of the vortex core (Sridhar & Katz, J. Fluid Mech., vol. 397, 1999, pp. 171-202). A typical Euler-Lagrange point-particle model with...
Surface transient storage (STS) has functional significance in stream ecosystems because it increases solute interaction with sediments. After volume, mean residence time is the most important metric of STS, but it is unclear how this can be measured accurately or related to other timescales and field-measureable parameters. We studied mean...