Network


Latest external collaboration on country level. Dive into details by clicking on the dots.

Hotspot


Dive into the research topics where Joseph S. Jewell is active.

Publication


Featured researches published by Joseph S. Jewell.


Archive | 2012

Effect of Gas Injection on Transition in Hypervelocity Boundary Layers

Joseph S. Jewell; Ivett A. Leyva; N. J. Parziale; Joseph E. Shepherd

A novel method to delay transition in hypervelocity flows in air over slender bodies by injecting CO2 into the boundary layer is presented. The dominant transition mechanism in hypersonic flow is the inviscid second (Mack) mode, which is associated with acoustic disturbanceswhich are trapped and amplified inside the boundary layer [8]. In dissociated CO2-rich flows, nonequilibrium molecular vibration damps the acoustic instability, and for the high-temperature, high-pressure conditions associated with hypervelocity flows, the effect is most pronounced in the frequency bands amplified by the second mode [3].


16th AIAA/DLR/DGLR International Space Planes and Hypersonic Systems and Technologies Conference | 2009

On the Impact of Injection Schemes on Transition in Hypersonic Boundary Layers

Ivett A. Leyva; Joseph S. Jewell; Stuart Laurence; H. G. Hornung; Joseph E. Shepherd

Abstract : Three geometries are explored for injecting CO2 into the boundary layer of a sharp five degree half-angle cone. The impact of the injection geometry, namely discrete injection holes or a porous conical section, on tripping the boundary layer is examined, both with and without injected flow. The experiments are conducted at Caltechs T5 reflected shock tunnel. Two different air free-stream conditions are explored. For the discrete-hole injectors, the diameter for the injection holes is 0.75 mm nominally and the length to diameter ratio is about 30. One injector has a single row of holes and the other has four rows. With the 4-row geometry fully turbulent heat transfer values are measured within four centimeters of the last injection row for both free-stream conditions. The 1-row injector results on a reduction of 50% in the transition Reynolds number. The porous injector does not move the transition Reynolds number upstream by itself with no injection flow.


Journal of Fluid Mechanics | 2011

Bubbles emerging from a submerged granular bed

J.A. Meier; Joseph S. Jewell; Christopher E. Brennen; Jörg Imberger

This paper explores the phenomena associated with the emergence of gas bubbles from a submerged granular bed. While there are many natural and industrial applications, we focus on the particular circumstances and consequences associated with the emergence of methane bubbles from the beds of lakes and reservoirs since there are significant implications for the dynamics of lakes and reservoirs and for global warming. This paper describes an experimental study of the processes of bubble emergence from a granular bed. Two distinct emergence modes are identified, mode 1 being simply the percolation of small bubbles through the interstices of the bed, while mode 2 involves the cumulative growth of a larger bubble until its buoyancy overcomes the surface tension effects. We demonstrate the conditions dividing the two modes (primarily the grain size) and show that this accords with simple analytical evaluations. These observations are consistent with previous studies of the dynamics of bubbles within porous beds. The two emergence modes also induce quite different particle fluidization levels. The latter are measured and correlated with a diffusion model similar to that originally employed in river sedimentation models by Vanoni and others. Both the particle diffusivity and the particle flux at the surface of the granular bed are measured and compared with a simple analytical model. These mixing processes can be consider applicable not only to the grains themselves, but also to the nutrients and/or contaminants within the bed. In this respect they are shown to be much more powerful than other mixing processes (such as the turbulence in the benthic boundary layer) and could, therefore, play a dominant role in the dynamics of lakes and reservoirs.


48th AIAA Aerospace Sciences Meeting Including the New Horizons Forum and Aerospace Exposition | 2010

Carbon Dioxide Injection for Hypervelocity Boundary Layer Stability

Ross Wagnild; Graham V. Candler; Ivett A. Leyva; Joseph S. Jewell; H. G. Hornung

An approach for introducing carbon dioxide as a means of stabilizing a hypervelocity boundary layer over a slender bodied vehicle is investigated through the use of numerical simulations. In the current study, two different test bodies are examined. The first is a fivedegree-half-angle cone currently under research at the GALCIT T5 Shock Tunnel with a 4 cm porous wall insert used to transpire gas into the boundary layer. The second test body is a similar cone with a porous wall over a majority of cone surface. Computationally, the transpiration is performed using an axi-symmetric flow simulation with wall-normal blowing. The effect of the injection and the transition location are gauged by solving the parabolized stability equations and using the semi-empirical e N method. The results show transition due to the injection for the first test body and a delay in the transition location for the second test body as compared to a cone without injection under the same flight conditions. The mechanism for the stabilizing effect of carbon dioxide is also explored through selectively applying non-equilibrium processes to the stability analysis. The results show that vibrational non-equilibrium plays a role in reducing disturbance amplification; however, other factors also contribute.


51st AIAA Aerospace Sciences Meeting including the New Horizons Forum and Aerospace Exposition 2013 | 2013

Transition within a hypervelocity boundary layer on a 5-degree half-angle cone in air/CO2 mixtures

Joseph S. Jewell; Ross Wagnild; Ivett A. Leyva; Graham V. Candler; Joseph E. Shepherd

Laminar to turbulent transition on a smooth 5-degree half angle cone at zero angle of attack is investigated computationally and experimentally in hypervelocity flows of air, carbon dioxide, and a mixture of 50% air and carbon dioxide by mass. Transition N factors above 10 are observed for air flows. At comparable reservoir enthalpy and pressure, flows containing carbon dioxide are found to transition up to 30% further downstream on the cone than flows in pure air in terms of x-displacement, and up to 38% and 140%, respectively, in terms of the Reynolds numbers calculated at edge and reference conditions.


42nd AIAA Fluid Dynamics Conference and Exhibit | 2012

Turbulent Spot Observations within a Hypervelocity Boundary Layer on a 5-degree Half-Angle Cone

Joseph S. Jewell; Nicholaus J. Parziale; Ivett A. Leyva; Joseph E. Shepherd

Laminar to turbulent transition is a critically important process in hypersonic vehicle design. Higher thermal loads, by half an order of magnitude or more, result from the increased heat transfer due to turbulent flow. Drag, skin friction, and other flow properties are also significantly impacted. Transition to turbulence in initially laminar boundary layers can occur along many paths. In low-speed flow under ideal conditions (quiet freestream, nominally smooth surfaces with favorable or zero pressure gradient and minimal crossflow) transition occurs over a finite distance and is associated with the creation and growth of propagating patches of turbulent flow, known as turbulent spots. Spots may be due to the breakdown of linear instabilities or induced by “bypass mechanisms” associated with nonideal effects in the flow or model. H.W. Emmons (1951) was the first to propose that laminar boundary layers break down through the convergence of spots, after observations of a water-table analogy to air flow. Spot formation has been studied extensively in subsonic flows, a recent review of past and current work on spots in incompressible flows is given by Strand and Goldstein (2011).


Archive | 2012

Shock Tunnel Noise Measurement with Resonantly Enhanced Focused Schlieren Deflectometry

N. J. Parziale; Joseph S. Jewell; Joseph E. Shepherd; H. G. Hornung

The character of the boundary layer noise and ambient tunnel noise are of interest in the experimental study of laminar to turbulent transition. The instability mechanism in hypersonic flow over slender bodies is the acoustic mode. A number of investigations of flow over a slender cone in high-enthalpy facilities have been performed; however, measurements of the boundary layer noise and ambient tunnel noise have not been made. In cold hypersonic facilities the frequency range of the acoustic mode typically lies below 500 kHz; in high-enthalpy facilities, 5-20 MJ/kg, the most strongly amplified acoustic mode frequency is approximately 1-3 MHz. These high frequencies are well beyond the reach of the piezo-electric pressure transducers typically used in cold hypersonic facilities. A logical approach is to investigate the use of optical methods. Measurements of the boundary layer noise and ambient tunnel noise on a five degree half angle cone in the Caltech T5 hypervelocity shock tunnel are made with a single point focused schlieren system and a resonantly enhanced focused schlieren system.


Journal of Spacecraft and Rockets | 2017

Correlation of HIFiRE-5 Flight Data With Computed Pressure and Heat Transfer

Joseph S. Jewell; James H. Miller; Roger L. Kimmel

Flight pressure and heat flux data have been compared to angle-of-attack- and yaw-dependent computational-fluid-dynamics results for pressure distribution as well as laminar and turbulent heat-tran...


2018 AIAA Aerospace Sciences Meeting | 2018

Nosetip bluntness effects on transition at hypersonic speeds: experimental and numerical analysis under NATO STO AVT-240

Pedro Paredes; Meelan M. Choudhari; Fei Li; Joseph S. Jewell; Roger L. Kimmel; Eric C. Marineau; Guillaume Grossir

The existing database of transition measurements in hypersonic ground facilities has established that the onset of boundary layer transition over a circular cone at zero angle of attack shifts downstream as the nosetip bluntness is increased with respect to a sharp cone. However, this trend is reversed at sufficiently large values of the nosetip Reynolds number, so that the transition onset location eventually moves upstream with a further increase in nosetip bluntness. This transition reversal phenomenon, which cannot be explained on the basis of linear stability theory, was the focus of a collaborative investigation under the NATO STO group AVT-240 on Hypersonic Boundary-Layer Transition Prediction. The current paper provides an overview of that effort, which included wind tunnel measurements in three different facilities and theoretical analysis related to modal and nonmodal amplification of boundary layer disturbances. Because neither first and secondmode waves nor entropy-layer instabilities are found to be substantially amplified to initiate transition at large bluntness values, transient (i.e., nonmodal) disturbance growth has been investigated as the potential basis for a physics-based model for the transition reversal phenomenon. Results of the transient growth analysis indicate that disturbances that are initiated within the nosetip or in the vicinity of the juncture between the nosetip and the frustum can undergo relatively significant nonmodal amplification and that the maximum energy gain increases nonlinearly with the nose radius of the cone. This finding does not provide a definitive link between transient growth and the onset of transition, but it is qualitatively consistent with the experimental observations that frustum transition during the reversal regime was highly sensitive to wall roughness, and furthermore, was dominated by disturbances that originated near the nosetip.


AIAA Journal | 2017

Effects of Shock-Tube Cleanliness on Hypersonic Boundary Layer Transition at High Enthalpy

Joseph S. Jewell; Nicholaus J. Parziale; Ivett A. Leyva; Joseph E. Shepherd

The prediction of a high-speed boundary-layer transition (BLT) location is critical to hypersonic vehicle design; this is because the increased skin friction and surface heating rate after transition result in increased weight of the thermal protection system. Experimental studies using hypervelocity wind tunnels are one component of BLT research.

Collaboration


Dive into the Joseph S. Jewell's collaboration.

Top Co-Authors

Avatar

Roger L. Kimmel

Wright-Patterson Air Force Base

View shared research outputs
Top Co-Authors

Avatar

Ivett A. Leyva

Air Force Research Laboratory

View shared research outputs
Top Co-Authors

Avatar

Joseph E. Shepherd

California Institute of Technology

View shared research outputs
Top Co-Authors

Avatar

Matthew P. Borg

Air Force Research Laboratory

View shared research outputs
Top Co-Authors

Avatar
Top Co-Authors

Avatar

Ross Wagnild

Sandia National Laboratories

View shared research outputs
Top Co-Authors

Avatar
Top Co-Authors

Avatar

David Adamczak

Wright-Patterson Air Force Base

View shared research outputs
Top Co-Authors

Avatar

H. G. Hornung

California Institute of Technology

View shared research outputs
Top Co-Authors

Avatar

N. J. Parziale

California Institute of Technology

View shared research outputs
Researchain Logo
Decentralizing Knowledge