yetter-nano engineered energetic materials durint-muri review

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2004 ARMY ENERGETIC MATERIALS MURI AND DURINT REVIEW MEETING Picatinny Arsenal Officers’ Club 27-28 October 2004 NANO ENGINEERED ENERGETIC MATERIALS (NEEM) MURI Overview Richard A. Yetter The Pennsylvania State University and the NEEM MURI Team

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2004 ARMY ENERGETIC MATERIALS MURI AND DURINT REVIEW MEETING

Picatinny Arsenal Officers’ Club27-28 October 2004

NANO ENGINEERED ENERGETIC MATERIALS

(NEEM) MURIOverview

Richard A. YetterThe Pennsylvania State University

andthe NEEM MURI Team

Issues and Motivation

• Potential benefits of nano energetic materials:More powerful. Controlled rate of energy release. More reliable. Higher density. More reproducible. Reduced sensitivity. Reduced vulnerability. Increased storage lifetime. Safer to handle. Multi-functionality.

• Modest gains to date: While some performance improvement has been demonstrated, the full extent of the anticipated gains fromnanoscale energetic materials has not been realized in large part due to the incompatibility of length scales.

Objectives

• Develop new methodologies to assemblenano-energetic materials that provide concurrent increases in performance and managed energy release rate while reducing sensitivity.

• Obtain fundamental understanding of the relationship between the design of nano-engineered energetic materials and their reactive and mechanical behaviors.

Critical Technology Issues

• Self-assembly and supramolecular chemistry of the fuel and oxidizer elements of energetic materials have lagged far behind chemistries in other disciplines (e.g., microelectronics, biological systems, and pharmaceuticals).

• There is no fundamental understanding of what type of supramolecular structures provide desirable performance in combustion, mechanical, and hazard characteristics.

Design Possibilities

polymer binder

nano-metallicparticle

micron-crystallineoxidizer

nano-crystallineoxidizer

nano-energetic materials

nano Al & Bnano RDX, HMX, & ADN

carbon nanotubes

self-assembledmicron-to-millimeter scale

energetic structure

self-assembledenergetic material

with gradient in chemical composition

conventionally assembledenergetic material with

micron-to-millimeter scale energetic structures

Program Philosophy

• Bring together leaders in nanotechnology and propellants and explosives

• Couple multiscale modeling and multiscalediagnostics

• Research and develop new concepts for assembling and understanding the dynamics of nano engineered energetic materials

Participating MURI Team Members

• David Allara, PSU: chemistry, nanotechnology, self-assembly• Ralph Nuzzo, UIUC: chemistry, nanotechnology, self-assembly• Dana Dlott, UIUC: chemistry, energetic materials, ultrafast laser

spectroscopy• Priya Vashishta, USC: physics, materials, atomistic modeling• Rajiv Kalia, USC: physics, materials, multiscale modeling • Aiichiro Nakano, USC: physics, materials, multiscale modeling • Vigor Yang, PSU: engineering, energetic materials, combustion

modeling• Richard Yetter, PSU: engineering, energetic materials,

combustion diagnostics• Kenneth Kuo, PSU: engineering, energetic materials,

combustion and ballistics

Program Elements

• Synthesis and Assembly• Theoretical Analysis and Design• Experimental Characterization

Program Structure and Interactions

Synthesis & Assembly

Theoretical Experimental NEEM

nano

- mac

ro

PSUUIUC

Modeling &Simulation

Characteriz

macro

-na

nonano -USC

PSU

ation & Diagnostics

macro

UIUCPSU

Synthesis, Self-Assembly, andSupramolecular Chemistry of Nano-

Structured Energetic Materials

Significant Research Experience on Al Synthesis, Fabrication, and Surface Chemistry

Nuzzo – UIUC, Allara - PSU

• SAMs on Al(native oxide)/Al• Al(metal)-SAM Structures & Interactions• Al Vapor Deposition Processes• Al Surface Chemistry• Materials Characterization

Nano Scale Energetic Materials Synthesis and Passivation: Nuzzo-UIUC & Allara-PSU

H Si H

H

Si

3/2 H2

TMA +

3/2 H2

AlH3-TMA

H Si H

H

H Si H

H

Si

3/2 H2

TMA +

3/2 H2

AlH3-TMA

• High surface area aluminum nanoparticles would be ideal high-energy materials

• A few examples of small aluminum clusters have recently been described (reductive syntheses), but there are no investigations of their use as high energy materials

• The Al nanoparticles consist of metallic aluminum cores surrounded by a monolayer of a protective shell

• 10 and 100 aluminum atoms and particle diameters between 0.5 and 1.3 nm

Generalize and Expand Synthetic Approaches

Stabilized nano-clusters via metal ligand interactions

Potential route to capped Al nanocluster

Develop new synthetic methodologies for affecting the low temperature synthesis of highly reactive nanoclusters

Aluminum cluster (far right) consists of nested shells containing (from left to right) 13, 44, and 20 aluminum atoms

A. Ecker, E. Weckert, and H. Schnöckel Nature 1997, 387, 379.

AlI + LiN(SiMe3)2 →Al77[N(SiMe3)2]202-

Nano Scale Energetic Materials Synthesis and Passivation: Nuzzo-UIUC & Allara-PSU

Generalize and Expand Synthetic Approaches to Aluminum Clusters with Sizes Ranging to 100 nm

• New SAMs for Cluster Passivation and Size Control•Thermal Cluster Growth

• Ligand-Directed Association• Directed Synthesis

•Full Characterization/Understanding of Structure and Properties at all Length Scales

High Energy Content Nanocomposites: Nuzzo-UIUC

• Novel Growth Chemistries

• Composites from Aerosol and Particle Spray Deposition Processes, e.g., Nanoparticle Metal/Fluorocarbon Composites

Teflon telomerparticles

Swollenparticles

Al growthvia infusion

Encapsulation by vitrification

Dispersible to ~0.2 µm Particles

PFK/PFE

Thermal Spray Deposition(e.g. TMAA / TiCl4 / MP 1100)

Zonyl® MP 1100

• Sub �m Teflon particles swollen in solvent,

• Al nanoparticles grown & passivated in pores,

• Spherical particles packed to form lattice ofpassivated nanoparticles

Nano Structured Energetic Materials-Model Systems Nuzzo-UIUC

Develop strategies for manipulating the larger mesoscopic organization of high energy nanoscale materials by directed design

Fabrication of Energetic Structures Using a Soft Lithographic Patterning Technique

10µm

Master

Spin-CastPFSOx

UVO

AdhesiveContact

DecalTransfer

Sputter DepositAluminumx2

Weld TwoAluminum Films

Laminate Decal

Decal Release for 3D Integration

10µm

Master

Spin-CastPFSOx

UVO

AdhesiveContact

DecalTransfer

Sputter DepositAluminumx2

Weld TwoAluminum Films

Laminate Decal

Decal Release for 3D Integration

Bottom layer strong oxidant such as HMX, which is readily deposited in thin film form from the vapor phase

Nano Structured Energetic Materials-Model Systems Nuzzo-UIUC

Fabrication of Energetic Structures Using Decal Transfer Lithography

Si

Si

Si

“Master”

Photoresist pixel post array

Spin coat and cure thin PDMS film.

Remove PDMS membrane stencil mask.

Place PDMS membrane on substrate.

Evaporate layer through membrane.

5-250 �m (dia); 5-150 �m (ht)

3-100 �m (thick)

- Stacked disks of oxidizer, e.g., RDX- Al with 5 mm pitch- Si is a silicon wafer- PDMS is a conformal silicone polymer membrane

-capable of achieving submicron resolution in large pattern area

Effect depositions for sequential levels.

Lift-off membrane to reveal pixel array.

Cap or align second mask for 3D structures

Cap or align second mask for 3D structures

Nano Structured Energetic Materials-Model Systems Allara-PSU

• Thin film nanostacks [ fuel-(oxidizer-fuel)N- ] (~1-3 nm thick)

fuel (Al, etc.)

oxidizer layer (SAM)passivation layertemplate layer

• Interface/Surface characterization – static• Capabilities:

• in-situ (UHV): IR, XPS, ToF-SIMS, AFM• ultrasensitive BET for planar-scale surface/pore areas

• Model structure characterizations:• structures, chemical interactions at interfaces• T dependence of structures (stability, chem degradation)

Shock Precipitation and Supercritical Fluid (SCF) Processing of Nano-sized Oxidizers: Kuo-PSU

• Two solvent-based methods will be examined in this study– Shock precipitation (SP) technique; – Supercritical fluid (SCF) technique.– A combined SP/SCF processing technique will also be considered.

• Oxidizer crystals to be considered include: RDX, ADN (ammoniumdinitramide), HNF and FOX-7 (1,1-diamino-2,2-dinitroethylene).

• Two SCF methods will be investigated for application to energetic materials (w/ Victor Stepanov of ARDEC):– Rapid Expansion of Supercritical Solutions (RESS).– Supercritical Anti-Solvent precipitation (SAS). – Rapid mixing via opposed-jet impinging flows will be applied to increase the

rate of nucleation and thus reduce the particle size while increasing yield.

Theoretical Modeling of Nano-Structured Energetic Materials from the

Atomistic/Molecular Scale to the Macroscale

Coupled FE/MD/QM Simulations Vashishta, Kalia, Nakano - USC

Multiscale QM/MD/FE simulation (top) implemented on a Grid (bottom) of supercomputers, data archive, and virtual environment

Approach:• Finite element (FE)• Atomistic molecular dynamics (MD)• Quantum-mechanical (QM) calculation based on density functional theory (DFT)

Challenge: Seamlessly couple QM scheme & MD approach based on effective interatomic potentials

Collaboratory for Advanced Computing & Simulations (CACS)• 1,512 processor Intel Xeon Linux cluster at USC• 2.4 million processor-hours of computing on IBM SP4 & Compaq AlphaServer at DoD Major Shared Resources Centers

Nano Aluminum Particle OxidationVashishta, Kalia, Nakano - USC

Number of Atoms: ~ 250,000 Al, ~ 550,000 O; Initial Al cluster 100Å radius

Oxidative Percolation

Oxidation Under Closed ConditionsMetal Oxide Core-Shell Structure

No heat dissipation allows rapid T increase in surface and core. Larger spheres correspond to oxygen and smaller spheres to aluminum; color represents the T.

OAl4 clusters percolate to form a neutral shield around Al nanoparticle, which impedes oxidation

Oxide thickness saturates at 40Å after 0.5 ns – good agreement with experiment (Nieh et al., Acta mater. 44, 3781 (1996)

RDX Molecule on Al (111) SurfaceVashishta, Kalia, Nakano - USC

Quantum mechanical MD simulation in the framework of the densityfunctional theory (DFT)

NEEM Behavior in Two-Phase Flow Environments at Meso & Macro Scales : Yang - PSU

Al Particle Diameter (m)

Flam

eSp

eed

(m/s

)

10-6 10-5 10-4

10-2

10-1

100

101

10-2

10-1

100

101

� = 0.8

0

Analytical predictionNumerical predictionExperimental data

• Couple Relevant Processes at Micro and MesoLength Scales to Macroscale Phenomena

• Investigate the transport and combustion of nano-sized particles in reactive flow environments

• Establish general analysis accommodating particle & thermo-fluid dynamics for two-phase flow interactions

• Identify key mechanisms and parameters for maximizing energy release

Aerosol Al - Air Flame

~ 1 cm~ 1 cm 1.9 cm1.9 cm

HeterogeneousSolid Phase

Ts = ~ 700 K

Tmelt = 558 K

Tsf = ~ 2000 K

Tdark zone= ~ 1250 K

PrimaryFlame Zone

(HMX Vapor /Liquid Interface)

(HMX Melt Front)

GAP PolymerResidue

HMX GAP

Dark Zone

SecondaryFlame Zone

HCN, H CO, N O, H , CO2 2

2 2 22

Major Species in Dark Zone:N , H O, NO, CO,

Foam Layer

Rapid Consumption ofHCN and NO

Decomposition, Evaporation, and Gas-Phase Reactions (Bubble)

Combustion-Wave Structure of HMXGAP Pseudo-Propellant

Optimization of NEEM Fabrication Techniques based on Supercritical (SCF) Processing: Yang - PSU

Shadowgraph images for injection of supercritical methane/ethylene fluid into subcritical environments at various conditions xCH4=0.1 and d=1.0 mm.

Pinj/Pc 1.15 1.16Tinj /Tc 1.23 1.03Pinj/Pchm 35.7 36.7� (Cp/Cv) 1.56 5.51

• The Tinj/Tc=1.03 jet has a large jet expansion angle and opaque appearance due to condensation

• Jet expansion angle differences may come from differences in specific heat ratios and the pressure rise due to the release of latent heat during condensation

Numerical Modeling and Optimization of SCF Fabrication Techniques:

• Rapid expansion of supercritical solution (RESS)• Supercritical anti-solvent precipitation (SAS)

Modeling will include:• Important near- and super- critical fluid

phenomena, including transcriticalthermodynamic and transport anomalies

• Parametric studies will examine effects of flow parameters and hardware design attributes on production of nano-sized materials

• Outcome will be improvements to existing techniques and new innovative concepts

Density gradient field

Experimental Characterization of Reactive and Mechanical Behaviors ofNano-Structured Energetic Materials

Time and space resolved spectroscopy ofnanoenergetic materials: Dlott - UIUC

Approach• Picosecond laser flash-heating of nanoenergetic materials

(Picosecond CARS, time-resolved emission, streakscopefor long distance and directional propagation)

• Ultrafast (sub ns) microscopy of laser-initiated materials• Femtosecond IR laser, time resolved IR spectroscopy (C-

H, C-C, Al-O, Al-F, C-F, O-H, etc.)• Femtosecond laser-driven shock compression and shock

spectroscopy of nanoenergetic materials (pressure 5-10 GPa, material velocity ~0.8 km/s, shock velocity ~4 km/s (40Å/ps), compression factor �V = 0.2, rise time 2-3 ps, fall time 15 ps)

High repetition rate laser flash-heating (100/s) Dlott - UIUC

1 mm

oxidizer100 pspulse 100 nm

transparent polymer oxidizer

10 cm10 cm

40 mg sample (3 �m thick). Each shot 50ng (150 �mdiam). 105

shots per sample

100 ps heating pulse ismatched to metal particle thermal conduction.Particle is uniformly heated, surroundings cold

Fast Spectroscopy of Laser Initiated NanoenergeticMaterials: Dlott - UIUC

-1 0 1 2 3 4 50.0

0.2

0.4

0.6

0.8

1.0

delay time (ns)

ON

O2

surv

ival

frac

tion

0.2%0.5%1.0% 2.0%

J = 5.9 J/cm2

abrupt transition

when reactions coalsece~300 ps

conc.indep

-1 0 1 2 3 4 50.0

0.2

0.4

0.6

0.8

1.0

delay time (ns)

ON

O2

surv

ival

frac

tion

0.2%0.5%1.0% 2.0%

J = 5.9 J/cm2

abrupt transition

when reactions coalsece~300 ps

conc.indep

0 10 20 30time (ns)

1% in NC5.6 J/cm2

3.9 J/cm2

1.8 J/cm2

0.4 J/cm22nsseveral

ns

0 10 20 30time (ns)

1% in NC5.6 J/cm2

3.9 J/cm2

1.8 J/cm2

0.4 J/cm22nsseveral

ns

Energy release via time-resolved emission

inte

nsity

(arb

)

Nitrate group consumption in Alex/NC

Energy release ~2 ns at low concentrationSlows down at higher fluence as reaction propagates over greater distances

Surface and Subsurface Analysis of Nano Engineered Energetic Materials: Yetter - PSU

Microscope

MicroscopeObjectiveEpi-Fluorecent

Prism/Filter Cube

BeamExpander

CCD Camera

Energetic Material

Nd:YAG Laser

CO2 Laser Irradiation / Ignition Source/ / Flame Propagation

Microscope

MicroscopeObjective

Epi-FluorecentPrism/Filter Cube

Energetic Material

CO2 Laser Irradiation / Ignition Source / Flame Propagation

Spectrometer

CCD Camera

• In-situ reacting energetic material studies using upright and inverted optical microscopes with high speed photography, micro particle image velocimetry, micro laser induced fluorescence and micro Raman spectrometry

• In-situ studies of reacting energetic materials using environmental scanning electron microscope at surface and subsurface temperatures of bulk material

Examples of Diagnostics Implementation

ESEM

Heating Stage

Sample Crucible

Heated Cell of FEI Quanta 200 SEM for simulating surface processes during reaction

ICCD

Micro Burner for Combustion Analysis of Nano Composites and Nano Metallic - Metallic Oxidizer

Systems: Yetter - PSU

Optical Combustion Chamber– Ignite thermite mixture or pressed

pellet to study effect of pressure, initial temperature, trapped gas effect

– High-speed video records to determine regression rate

– Pyrometer to measure the surface temperature of the condensed phase products

– LIF to measure presence of AlO

High-SpeedCamera

IgniterOptical Combustion

Chamber

ThermiteMixture

Molten Product Container

Pyrometer

High-SpeedCamera

IgniterOptical Combustion

Chamber

ThermiteMixture

Molten Product Container

Pyrometer•Formulate and study the reaction dynamics of nano-composite thermite systems

• Investigate systems that produce significant gas at high-energy release rates

•Determine the effect of composition and physical characteristics of the trapped gas, initial temperature, and pressure on regression rates of mixtures

Formulation and Combustion Analysis of New and Advanced Nano-Energetic Materials and Propellants

Kuo - PSU

• Burning Rate Measurements of Newly Processed Propellants• Burning Surface Observation of Propellants with Nano-Particles• Laser Ignition Characteristics of New propellants with Nanosized

Energetic Particles

Propellant burning at 8,000 psi

Time [ms]:0 140 270 450 630

1 mm

0.1

1

10

100

0.8

1.2

1.6

2

2.4

2.8

3.2

1000 104 105

AME - RDX/BBA/Alex Nano-RDX/BBA/Alex AHE - HNF/RDX/BBA/AL

AHE/AMEAHE/Nano-RDX

Burn

Rat

e

Burning Rate R

atio

Pressure [psig]

Solid Propellant Strand Burner: capabilities/features� Optically accessible� Up to 9,500 psi capability� Temperature control –60oC < T < 80o

Interactions External to MURI TEAM

DoD and DoE Laboratories

Energetic Materials Design

ARO MURI

Synthesis & Assembly

Theoretical Simulation &

Modeling

Experimental Characterization &

Diagnostics

NEEM

Center for NanoEnergetic

MaterialsARO DURINT

Industry