Bulletin of the American Physical Society
71st Annual Meeting of the APS Division of Fluid Dynamics
Volume 63, Number 13
Sunday–Tuesday, November 18–20, 2018; Atlanta, Georgia
Session D03: Shock Waves & Explosions |
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Chair: Yue Ling, Baylor University Room: Georgia World Congress Center B204 |
Sunday, November 18, 2018 2:30PM - 2:43PM |
D03.00001: Critical ignition behind non-stationary curved shocks Matei Radulescu Gas ignition behind non-stationary curved shocks is treated analytically. The competition between thermal heating and gasdynamic expansion along a particle path controls the ignition. The relation between the Lagrangian rate of gas expansion and the shock dynamics parameters is established using the shock change equations. The critical conditions for ignition are derived in closed form for ignition described by global one and two step kinetics in terms of the shock speed, curvature and acceleration. Both models predict the same critical conditions for ignition in the limit of a high activation energy. The closed form solutions for critical gas expansion rate preventing ignition predicted by these models are found in excellent agreement with results from real gas calculations for ignition behind shocks in hydrocarbon-air mixtures. The model presented unifies previous models developed by Shepherd, Oppenheim and the author for critical ignition behind decaying shocks. |
Sunday, November 18, 2018 2:43PM - 2:56PM |
D03.00002: Lie Symmetry Analysis of Shock Problems Using Generalized Functions Joe Schmidt, Aurora Ireland, Harrison Davis Lie symmetry analysis depends on the calculation of derivatives to find and use the symmetries. Solutions to hydrodynamic shock problems have discontinuities which mean that the usual derivative cannot be calculated. The solution is to use symmetry analysis in the smooth regions between shocks and stitch them together using the Hugoniot jump conditions, which must also satisfy the symmetry conditions. In this work we use generalized functions to express the solution and then calculate the derivatives using generalized derivatives. This provides a concise framework for analyzing shock problems. We demonstrate the method on the Noh and shock tube problems. |
Sunday, November 18, 2018 2:56PM - 3:09PM |
D03.00003: Piston-driven converging shock wave in a stiff gas Scott D Ramsey, Roy S Baty The problem of a one-dimensional curvilinear shock wave converging into an ideal gas was first investigated by Guderley in 1942. Since then, many authors have discussed the practical notion of how Guderley-like flows might be generated. An obvious candidate is a ‘curvilinear piston,’ giving rise to a converging shock wave in the spirit of its planar counterpart. A limitation of existing analyses along these lines is the restriction to flows in materials described by an ideal gas equation of state (EOS) constitutive law. This choice is necessary for the direct comparison with the Guderley solution, which also features an ideal gas EOS. However, the ideal gas EOS is limited in its utility. The current work is thus intended to provide an extension of previous work to a non-ideal EOS. The stiff gas EOS is chosen as a logical starting point, due not only to its resemblance to the ideal gas law, but also its relevance to the shock compression of various liquid and solid materials. Given the stiff gas EOS is not otherwise expected to admit a Guderley-like solution when coupled to the inviscid Euler equations, this work provides the semi-analytical limiting behavior of a flow that cannot be otherwise captured using similarity analysis. |
Sunday, November 18, 2018 3:09PM - 3:22PM |
D03.00004: A small-disturbance model for transonic flow of a real gas around a thin airfoil Akashdeep Singh Virk, Zvi Rusak A small-disturbance model for a steady transonic flow of a real gas around a thin airfoil is presented. The model explores the nonlinear interactions among the near-sonic speed of the flow, the small thickness ratio and angle of attack of the airfoil, and the upstream properties of the gas. The flow thermodynamic properties are described by a general equation of state. The asymptotic analysis provides the similarity parameters that govern the flow problem. Also, the flow field can be described by a transonic small-disturbance (TSD) equation. The approach is applied to the perfect gas, van der Waals and Redlich-Kwong gas models and the relationships between these cases are explored. An iterative numerical scheme that is based on the Murman & Cole's (1971) method for the solution of the TSD equation is developed. The computed results describe the effect of the upstream flow pressure and temperature on the fields of flow properties and the on aerodynamic performance of airfoils. |
Sunday, November 18, 2018 3:22PM - 3:35PM |
D03.00005: Validation of Dalton's and Amagat's laws for gas mixtures with shock propagation Patrick J Wayne, Sean Cooper, Dylan Simons, Ignacio Trueba-Monje, Daniel Freelong, Gregory Vigil, Peter V Vorobieff, C Randall Truman, Timothy T Clark Dalton’s and Amagat’s laws are known as the law of partial pressures and the law of partial volumes, respectively. These well-known thermodynamic models are used to characterize the properties of gas mixtures. We conducted experiments to assess the accuracy of these laws in predicting the properties of gas mixtures with shock propagation. We present results for two gas mixtures of sulfur hexafluoride (SF6) and helium (He), with 50%/50% and 25%/75% SF6/He molar concentrations. Fast response pressure transducers are used to determine the pressure of each gas mixture both before and after the passage of the shock wave. Temperature readings are obtained using an ultra-fast response mercury cadmium telluride (MCT) infrared (IR) detector, with a response time on the order of 60 nanoseconds. Coupled with a stabilized broadband infrared light source (operating at 1500 K) the MCT detector provides pre- and post-shock line-of-sight readings of average temperature within the shock tube. These experimental results are compared with theoretical to determine if one of the thermodynamic models produces better agreement with experiment. |
Sunday, November 18, 2018 3:35PM - 3:48PM |
D03.00006: Post-shock flow effect in geometrical shock dynamics model Heng Liu, Shi Qiu, Veronica Eliasson Focusing of shock waves can generate extreme thermodynamic conditions, such as high pressure and temperature, at the focal region. Among all numerical approaches to simulate the propagation of shock waves, geometrical shock dynamics (GSD) is an appealing model to predict the shock motion. Compared to the traditional Euler method, such simplified model is much more computationally efficient especially for converging shock waves. Assuming uniform initial state behind the shock, GSD has shown its success in evaluating the effect of geometry change upon the shock, but the ignorance of the interaction between the shock front and non-uniform flow immediately behind it (post-shock flow effect) leads to a significant loss of accuracy when blast waves are considered, where an initial decay of all major flow properties is presented just behind the blast front. Such post-shock flow effect can be expressed as infinite number of coupled non-linear differential equations, and the influence of the order of completeness of such closed system on accuracy is studied in this work. Several comparisons are also performed with a similar approach that takes into account the post-shock flow effect by coupling the post-shock flow conditions obtained from existing data into the 0th-order GSD solution. |
Sunday, November 18, 2018 3:48PM - 4:01PM |
D03.00007: Post-shock Turbulence Structure and Dynamics in the Multi-fluid Shock-Turbulence Interaction Yifeng Tian, Farhad Jaberi, Daniel Livescu The variable density effects on the post-shock turbulence structure and dynamics are studied using accurate turbulence-resolving shock-capturing Eulerian simulations, together with a Lagrangian particle tracking algorithm. Detailed grid and statistical convergence tests are conducted to show that the simulations are insensitive to the grid resolution and the sample sizes are large enough for statistical analysis. Results show that the density variations not only affect the turbulence structure immediately after the shock wave but also significantly change the transient development in the post-shock region. The correlation between fluid density and flow topology is observed to be significant as the examination of the joint PDFs of the second and third invariants of the velocity gradient tensor indicates. This is identified to be caused by the different roles that density plays through the interaction with the shock wave, which results in a misalignment between the density gradient and vorticity. The dynamics of the turbulence structure in the post-shock region are further examined by the Lagrangian particle method. The variable density effects are found to be mainly manifested in the pressure Hessian contribution in the Lagrangian dynamical equations. |
Sunday, November 18, 2018 4:01PM - 4:14PM |
D03.00008: Assessing the Drag Law for an Explosively Driven Particle using Experiments and Uncertainty Quantification Joshua Garno, Frederick Ouellet, Rahul Babu Koneru, Thomas L Jackson, S Balachandar, Bertrand Rollin Although commonly used in point-particle simulations, analytic models expressing the hydrodynamic forces on a particle have not been thoroughly tested and validated in the extreme conditions of the explosive regime. Recent shock-tube experiments and simulations have shown that the Maxey-Riley-Gatignol particle force equation extended for compressible flows captures the evolution of particle force induced by the shock-particle interaction, but effects of the contact interface were not examined. The current work assesses the predictive capability of the model for the case where a particle is strongly affected by the shock and contact produced by the detonation of an explosive charge. Simulations are performed using a finite-volume, Euler-Lagrange code with the JWL EOS to handle explosive products. Accounting for various experimental uncertainties, simulated particle trajectories are compared with experimental particle positions following the explosive ejection of a particle from a rigid barrel into a region of ambient air. |
Sunday, November 18, 2018 4:14PM - 4:27PM |
D03.00009: Shock wave propagation and reflections in confined two- and three-dimensional geometries Sara DiGregorio, Michael John Hargather Explosively driven shock propagation was studied using a miniature shock demonstrator made from laser cut acrylic sheets to model various geometries in two and three dimensional space. Shock waves are produced using an electric spark gap on a detonator header which is driven by an FS-17 fire set. The spark causes an air shock which propagates through the demonstrator. Shock reflection, diffraction, and complex interactions are studied in the transition from two to three-dimensional space. The propagation is quantified in terms of velocity throughout the geometries. In addition, piezoelectric pressure gauges are used to measure static and reflected pressures at various locations in the geometries. The demonstrator is placed within a schlieren imaging system to obtain high speed images of the shock propagation caused by the explosive events. |
Sunday, November 18, 2018 4:27PM - 4:40PM |
D03.00010: Dynamics and attenuation of shock waves launched in liquid jets by X-ray laser pulses Claudiu Stan, Gabriel Blaj, Philip Willmot, Mengning Liang, Jason Koglin, Andrew Aquila, Joseph Robinson, Raymond Sierra, Sébastien Boutet Chemical and biological experiments performed at X-ray laser facilities embed the samples in liquid microjets to enable rapid sequential X-ray probing of fresh samples. The absorption of intense X-ray laser pulses generates shock waves that travel along the liquid jets, and may damage samples in MHz repetition rate experiments. We imaged optically these shock waves and determined their properties up to ~40 ns of travel along liquid water microjets with 14 or 20 µm diameters. The shock pressure was evaluated from the shock velocity and was found to decay rapidly from peak pressures around 1 GPa to pressures below 100 MPa; the latter value still exceeds the Vickers hardness of lysozyme protein crystals. The reflection of the shock at the surface of the jets leads to cavitation and to the generation of additional pressure waves, leading to a complex shock structure that is related to, yet different from, the one observed in supersonic gas jets. |
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