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Dive into the research topics where Michael John Murphy is active.

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Featured researches published by Michael John Murphy.


SHOCK COMPRESSION OF CONDENSED MATTER - 2011: Proceedings of the Conference of the American Physical Society Topical Group on Shock Compression of Condensed Matter | 2012

Simultaneous photonic doppler velocimetry and ultra-high speed imaging techniques to characterize the pressure output of detonators

Michael John Murphy; Steven A. Clarke

Detonator output directed into both ambient air and polymethylmethacrylate (PMMA) windows is simultaneously investigated using ultra-high speed, time-resolved imaging and photonic Doppler velocimetry (PDV) measurements. In air, one-dimensional measurements of detonator cup position are made from timeresolved image sequences and compared to time-integrated velocity curves obtained from the PDV data. The results demonstrate good agreement that validates using the two methods concurrently to measure the motion of the detonator free-surface. In PMMA windows, instantaneous shock velocities are calculated from 1-D time-resolved measurements of shock position and known velocity-Hugoniot data are utilized to map the shock velocity calculations to corresponding values of mass velocity and shock pressure. Simultaneous PDV data describing the motion of the detonator cup/PMMA interface are used to determine the mass velocity and pressure at the interface, and to compare to the mass and shock pressures calculated from...


Bulletin of the American Physical Society | 2008

USING SCHLIEREN VISUALIZATION TO TRACK DETONATOR PERFORMANCE

Steven A. Clarke; C. A. Bolme; Michael John Murphy; C. D. Landon; Thomas A. Mason; R. J. Adrian; A. A. Akinci; Michael Martinez; Keith A. Thomas

Several experiments will be presented that are part of a phased plan to understand the evolution of detonation in a detonator from initiation shock through run to detonation, to full detonation, to transition, to booster and booster detonation. High‐speed multiframe schlieren imagery has been used to study several explosive initiation events, such as exploding bridgewires (EBWs), exploding foil initiators (EFIs or “slappers”), direct optical initiation (DOI), and electrostatic discharge. Additionally, a series of tests has been performed on “cut‐back” detonators with varying initial pressing heights. We have also used this diagnostic to visualize a range of EBW, EFI, and DOI full‐up detonators. Future applications to other explosive events, such as boosters and insensitive high explosives booster evaluation, will be discussed. The EPIC finite element code has been used to analyze the shock fronts from the schlieren images to solve iteratively for consistent boundary or initial conditions to determine the ...


Bulletin of the American Physical Society | 2009

Characterizing Detonator Output Using Dynamic Witness Plates

Michael John Murphy; Ronald J. Adrian

A sub‐microsecond, time‐resolved micro‐particle‐image velocimetry (PIV) system is developed to investigate the output of explosive detonators. Detonator output is directed into a transparent solid that serves as a dynamic witness plate and instantaneous shock and material velocities are measured in a two‐dimensional plane cutting through the shock wave as it propagates through the solid. For the case of unloaded initiators (e.g. exploding bridge wires, exploding foil initiators, etc.) the witness plate serves as a surrogate for the explosive material that would normally be detonated. The velocity‐field measurements quantify the velocity of the shocked material and visualize the geometry of the shocked region. Furthermore, the time‐evolution of the velocity‐field can be measured at intervals as small as 10 ns using the PIV system. Current experimental results of unloaded exploding bridge wire output in polydimethylsiloxane (PDMS) witness plates demonstrate 20 MHz velocity‐field sampling just 300 ns after i...


Bulletin of the American Physical Society | 2018

Novel measurements of shock pressure decay in PMMA using detonator loading

Michael John Murphy; Mark Lieber; Matthew M. Biss

An empirical model equation for shock-pressure decay in PMMA was determined through a unique set of experiments employing detonator loading. Custom polymethyl methacrylate (PMMA) witness blocks were designed with monolithic architecture to house precise PMMA gaps with thicknesses ranging from 0-10 mm in nominal increments of 1 mm. The PMMA gaps separated detonator working surfaces from windowed photonic Doppler velocimetry (PDV) probes, and were designed to provide undistorted optical access for ultra-high-speed framing and digital-streak cameras. The shock wave image framing technique (SWIFT), and a new laser-backlit digital-streak diagnostic, simultaneously captured the temporal evolution of detonator-induced diverging shock waves within the PMMA gaps. The PDV diagnostic measured critical mass-velocity histories as the shocks exited the variable gap thicknesses. The multi-diagnostic data package was used to characterize the shock-pressure decay in PMMA as a function of shock-propagation time and PMMA thickness.An empirical model equation for shock-pressure decay in PMMA was determined through a unique set of experiments employing detonator loading. Custom polymethyl methacrylate (PMMA) witness blocks were designed with monolithic architecture to house precise PMMA gaps with thicknesses ranging from 0-10 mm in nominal increments of 1 mm. The PMMA gaps separated detonator working surfaces from windowed photonic Doppler velocimetry (PDV) probes, and were designed to provide undistorted optical access for ultra-high-speed framing and digital-streak cameras. The shock wave image framing technique (SWIFT), and a new laser-backlit digital-streak diagnostic, simultaneously captured the temporal evolution of detonator-induced diverging shock waves within the PMMA gaps. The PDV diagnostic measured critical mass-velocity histories as the shocks exited the variable gap thicknesses. The multi-diagnostic data package was used to characterize the shock-pressure decay in PMMA as a function of shock-propagation time and PMMA th...


Bulletin of the American Physical Society | 2009

DETONATOR PERFORMANCE CHARACTERIZATION USING MULTI‐FRAME LASER SCHLIEREN IMAGING

Steven A. Clarke; Colin Landon; Michael John Murphy; Michael Martinez; Thomas A. Mason; Keith A. Thomas

Several experiments that are part of a phased plan to understand the evolution of detonation in a detonator from initiation shock through run to detonation to full detonation to transition to booster and booster detonation will be presented. High speed laser schlieren movies have been used to study several explosive initiation events, such as exploding bridgewires (EBW), exploding foil initiators (EFI) (or slappers), direct optical initiation (DOI), and electrostatic discharge (ESD). Additionally, a series of tests have been performed on “cut‐back” detonators with varying initial pressing (IP) heights. We have also used this diagnostic to visualize a range of EBW, EFI, and DOI full‐up detonators. Future applications to other explosive events such as boosters and IHE booster evaluation will be discussed. The EPIC hydrodynamic code has been used to analyze the shock fronts from the schlieren images to reverse calculate likely boundary or initial conditions to determine the temporal‐spatial pressure profile ...


Proceedings of SPIE, the International Society for Optical Engineering | 2007

High-speed multi-frame laser schlieren for visualization of explosive events

Steven A. Clarke; Michael John Murphy; C. D. Landon; Thomas A. Mason; R. J. Adrian; A. A. Akinci; Michael Martinez; Keith A. Thomas

High-Speed Multi-Frame Laser Schlieren is used for visualization of a range of explosive and non-explosive events. Schlieren is a well-known technique for visualizing shock phenomena in transparent media. Laser backlighting and a framing camera allow for Schlieren images with very short (down to 5 ns) exposure times, band pass filtering to block out explosive self-light, and 14 frames of a single explosive event. This diagnostic has been applied to several explosive initiation events, such as exploding bridgewires (EBW), Exploding Foil Initiators (EFI) (or slappers), Direct Optical Initiation (DOI), and ElectroStatic Discharge (ESD). Additionally, a series of tests have been performed on cut-back detonators with varying initial pressing (IP) heights. We have also used this Diagnostic to visualize a range of EBW, EFI, and DOI full-up detonators. The setup has also been used to visualize a range of other explosive events, such as explosively driven metal shock experiments and explosively driven microjets. Future applications to other explosive events such as boosters and IHE booster evaluation will be discussed. Finite element codes (EPIC, CTH) have been used to analyze the schlieren images to determine likely boundary or initial conditions to determine the temporal-spatial pressure profile across the output face of the detonator. These experiments are part of a phased plan to understand the evolution of detonation in a detonator from initiation shock through run to detonation to full detonation to transition to booster and booster detonation.


Experiments in Fluids | 2007

Particle response to shock waves in solids: dynamic witness plate/PIV method for detonations

Michael John Murphy; Ronald J. Adrian


Archive | 2009

TCGX fall 2009 review optical diagnostics

Michael John Murphy; Steven A. Clarke


Archive | 2017

TCG-X Fall 2017 Subtask 1.2 Advanced Diagnostics Concepts

Michael John Murphy; Mark Lieber; Matthew M. Biss


Archive | 2015

Reactive Burn Modeling Applications and Experiments

Carl Johnson; Elizabeth Francois; Michael John Murphy; Mark Lieber; Scott I. Jackson; Richard L. Gustavsen

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Steven A. Clarke

Los Alamos National Laboratory

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Keith A. Thomas

Los Alamos National Laboratory

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Mark Lieber

Los Alamos National Laboratory

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Michael Martinez

Los Alamos National Laboratory

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Thomas A. Mason

Los Alamos National Laboratory

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A. A. Akinci

Los Alamos National Laboratory

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C. D. Landon

Brigham Young University

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Matthew M. Biss

Pennsylvania State University

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C. A. Bolme

Massachusetts Institute of Technology

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