structure and density predictions for energetic materials

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Structure and Density Predictions for Structure and Density Predictions for Energetic Materials Energetic Materials Zuyue Du, Sayta Prasad, Ed Wells and Herman L. Ammon Department of Chemistry & Biochemistry, University of Maryland College Park, MD 20742 Picatinny Arsenal, NJ Oct. 27, 2004

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Structure and Density Predictions for Energetic Materials. Zuyue Du, Sayta Prasad, Ed Wells and Herman L. Ammon Department of Chemistry & Biochemistry, University of Maryland College Park, MD 20742 Picatinny Arsenal, NJ Oct. 27, 2004. pt grp. r g/cc. r VA ***. RDX. C s. 1.806*. - PowerPoint PPT Presentation

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Page 1: Structure and Density Predictions for Energetic Materials

Structure and Density Predictions forStructure and Density Predictions forEnergetic MaterialsEnergetic Materials

Zuyue Du, Sayta Prasad, Ed Wells and Herman L. Ammon

Department of Chemistry & Biochemistry,University of MarylandCollege Park, MD 20742

Picatinny Arsenal, NJOct. 27, 2004

    

Page 2: Structure and Density Predictions for Energetic Materials

computer modeling &

simulations

quantitative estimation

key properties & characteristics... conformation stability/reactivity Hf crystal structure/habit microstructure detonation behavior sensitivity

elemental composition&

molecular structure+

Identification,Design andDevelopment

of new energeticmaterials

Page 3: Structure and Density Predictions for Energetic Materials

Cyclic nitramines, (CH2NNO2)n units

1.810

1.829

1.847

1.838

VA***

1.750**

1.668**

1.759*

1.902*

1.839*

1.806*

g/cc

C1

~Ci

C2v

Ci

C2

Cs

pt grp

10-ring

4-ring

-HMX

-HMX

-HMX

RDX

*exptl **structure prediction

*** VA = mass / (atom/group volumes)

N

N

NNO2

NO2

O2N

NN

NN NO2

O2N

O2N

NO2

RDX

HMX

NN

NN

N

O2N

NO2

NO2O2N

O2N 10N

N

O2N

NO2

4

DensityDensity --> "primary physical parameter in detonation performance"

Page 4: Structure and Density Predictions for Energetic Materials

problems withproblems with constitutional isomers….constitutional isomers….

O2N NO2 O2N

O2NNO2 NO2

exptl : 1.573 1.569 1.651 g/cc

the solutionsolid state

structure prediction

many variables:atom types,

structure/conformation,packing efficiency

MOLPAKROTPAKMOLPAK-2

Page 5: Structure and Density Predictions for Energetic Materials

Crystal Structure Prediction…Crystal Structure Prediction…

model

MOLPAK

refinement

ab initio geometry optimization;usually G03, b3lyp/631g*

Mimic exptl crystal structures for triclinic -> orthorhombic sp grps;Use exptl coordn geom patterns; Create hypothetical crystal structures for 29 coordination geometries;~6,900 structures/coordn geom

Optimize unit cell parameters, model orientation & position by lattice E minimization;

WMIN: atom-centered charge electrostaticsDMAREL: distributed multipole electrostatics

400-900highest each geom

Page 6: Structure and Density Predictions for Energetic Materials

   0.114C222120

5.2714Pbca [2]6123.23210P212121 [2]19

0.462Pbcn [2]600.457P21212 [3]18

0.335Pccn564.0557C2/c [3]15

0.011Pncn5237.25157P21/c [5]14

0.19Iba2450.112P2/c13

0.110Aba2411.0135Cc [1]9

0.012Pnn2340.346Pc7

1.8253Pna21 [3]330.9125C2 [1]5

1.0137Pca21 [2]2910.91507P21 [2]4

0.012I2222312.61747P-1 [2]2

0.011C222210.458P1 [1]1

MOLPAK coverageMOLPAK coverage… all triclinic to Z = 8 orthorhombic space groups

For C-H-N-O-F molecules, space group frequencies are…

# Sp Grp N % # Sp Grp N %

MOLPAK coordination geometries = [29] ~ 99%

Page 7: Structure and Density Predictions for Energetic Materials

WMIN LE potential…WMIN LE potential…

Optimize crystal structure…Adjust unit cell, model position & orientation

LE = [QiQj*Rij-1 - Aij*Rij

-6 + Bij*exp-(Rij(Ci+Cj))]

A, B, C: empirical coefficients…Aij = (Aatom_type_i * Aatom_type_j)1/2

Currently have 69 atoms types…

Eg, C-NO2, N-NO2, cubane-NO2, N-NO2 R3N, C(=O)NR2

N N

O

Page 8: Structure and Density Predictions for Energetic Materials

Calcd vs. X-ray Density, 352 Crystals

R2 = 0.99

1

1.2

1.4

1.6

1.8

2

2.2

2.4

1 1.5 2

X-ray Density (g/cc)

Cal

cd D

ensi

ty (

g/c

c)

Page 9: Structure and Density Predictions for Energetic Materials

Crystal structure prediction…Crystal structure prediction… successes and problems…successes and problems…

X-ray model

In 80%smallest LE ->exptl structure

Examples..(CH3)2NNO2 *TNAZ *RDX *-CL20 *FOX7 # 2, +0.4

In 20%exptl structurein top 6 lowestLE solutions

MOLPAK+

WMIN

29 coordination geometries +193 = 6,859/geometry ~ 200,000 hypothetical crystal structures

29*400-900/geom -> latticerefinement & LE calcns

Page 10: Structure and Density Predictions for Energetic Materials

# E Space # E Space group group

1 1.996 -43.56 P21/c 16 1.856 -36.46 C2/c 2 1.966 -42.28 P212121 17 1.870 -35.92 P21

3 1.965 -42.20 P212121 18 1.777 -35.85 P21

4 1.898 -39.63 P21/c 19 1.856 -35.56 Cc

5 1.898 -39.63 P21/c 20 1.804 -35.50 Pbcn

6 1.838 -38.07 C2/c 21 1.783 -35.32 Pna21

7 1.851 -37.99 Pbca 22 1.817 -34.63 Pbcn

8 1.875 -37.81 Pca21 23 1.721 -33.68 P21212

9 1.901 -37.68 P21/c 24 1.734 -33.57 C2

10 1.832 -37.34 C2/c 25 1.690 -32.56 Pna21

11 1.802 -37.24 Pbca 26 1.799 -31.96 Pca21

12 1.877 -37.18 P-1 27 1.706 -31.34 P1

13 1.877 -37.18 P-1 28 1.656 -31.04 P21212

14 1.835 -37.11 Pna21 29 1.693 -29.85 P21212

15 1.810 -36.54 P21/c Cell Parameters: a b c X-ray 8.852 Å 12.556 13.386 106.82o

Predicted (%) 1.55 -0.53 0.98 -0.65

obsd = 2.043 g/cc

Structure prediction example, Structure prediction example, -CL20 from B3lyp/631g* model-CL20 from B3lyp/631g* model

Page 11: Structure and Density Predictions for Energetic Materials

-(NO2)8

= 2.008 g/cc

det P = 32.72 gPa

det V = 8.25 km/s

Isp = 229.7 s

-(NO2)8

= 2.105 g/cc

det P = 55.88 gPa

det V = 9.75 km/s

Isp = 266.7 s

-(NO2)12

= 1.981 g/cc, exptl = 1.978

det P = 48.74 gPa

det V = 9.35 km/s

Isp = 267.5 s

= 1.856 g/cc

det P = 32.91 gPa

det V = 8.76 km/s

Isp = 260.7 s

-(NO2)8

= 1.818 g/cc

det P = 35.21 gPa

det V = 9.08 km/s

Isp = 272.1 s

C C NO2O2N

= 1.936 g/cc

det P = 29.56 gPa

det V = 8.00 km/s

Isp = 232.3 s

C C

NO2

O2N NO2

O2N

Structure prediction -> new molecule evaluation…Structure prediction -> new molecule evaluation…

Page 12: Structure and Density Predictions for Energetic Materials

ROTPAKROTPAK……pack & adjust conformation, minimize Etotal…

Criterion: Etotal = Einter + Eintra ~ Ethresh

orientedmolecule at origin

orientedmoving molecule

move togetheruntil

Etotal ~ Ethresh

alter conformationcalc new Etotal

> Ethresh< Ethresh

Ethresh = 0.5

kcal/molfor line

no further improvement in Etotal

new orientation

closest approach

Page 13: Structure and Density Predictions for Energetic Materials

# G03 RPK Xray # G03 RPK Xray # G03 RPK Xray

1 29.4º-> 26.0 20.9 1 -5.4º-> -5.2 -6.0 1 11.6º-> 11.6 9.6 2 0.0 -> 11.4 19.4 2 167.4 -> 173.6 179.3 2 -76.6 -> -1.6 -5.0 3 21.6 -> 10.3 7.2 3 -108.5 -> -30.6 -32.6 4 1.3 -> 1.8 13.5 5 30.0 -> -17.7 -16.4 6 -1.5 -> 30.3 25.4 7 38.3 -> -12.9 -9.2

ROTPAK examples…ROTPAK examples…

O2N NO2

NO2

CUGCOW DUYREU

1

2

3 NCN

NO212

KASBAH

(NO2)7

Model (G03), ROTPAK/WMIN and X-ray torsion angle comparison…

Page 14: Structure and Density Predictions for Energetic Materials

X-ray

B3lyp/631g*model

1

2 3 NH

CH3

O

CH3

O2N

NO2

ROTPAK example…ROTPAK example…

24.6

47.1

0.0o

B3…

22.9

51.9

41.4o

X-ray

3

2

1

29.0

48.6

45.0o

RPK/ WMIN

Page 15: Structure and Density Predictions for Energetic Materials

X-ray G03 + ROTPAK + WMIN

-6.31.53

2.9119.9o

1.819.67c

1.44.85b

6.8%12.57 Åa

1.87 Å1.93 Åa

b

c

Page 16: Structure and Density Predictions for Energetic Materials

X-raymodel

G03B3lyp/631g*model

ROTPAK + WMIN

bend ~20o + N-NO2 twist

ROTPAK example…RDX bond bending…ROTPAK example…RDX bond bending…

Page 17: Structure and Density Predictions for Energetic Materials

RDX X-ray and ROTPAK-modified overlays…RDX X-ray and ROTPAK-modified overlays…

-1.31.806 (g/cc)

-0.610.709c

0.711.574b

1.213.182a (Å)

ROTPAK-

X-ray (%)

X-raydimension

RDX space group: Pbca

unit cellcomparison

Page 18: Structure and Density Predictions for Energetic Materials

Some ROTPAK challenges…Some ROTPAK challenges…

O2NC(NO2)3

O2N

O2N

NO2

N3N3

N3

N3

O

N3N3

N3

NO2

O

O

CH2-N=N=N

CH2-N=N=N

CH2-N=N=N

Page 19: Structure and Density Predictions for Energetic Materials

MOLPAK, the old and the new…MOLPAK, the old and the new…

MOLPAK-1 •Uses pre-established coordn geoms (CN = 14)•Coordn geom sub-programs are hand-coded•Some structures don’t fit the rules•Structures built with repulsion-only potential

MOLPAK-2•Build structures from crystal space group symmetry•One program does all symmetries•Structures built with 3-term potential•Special features more easily handled, eg H-bonding, molecule-solvent complexes, ionic materials

Page 20: Structure and Density Predictions for Energetic Materials

Determine length of an axis ->make line of C1 or Ci images; assume line is a/c or b axis

For each grid, fill unit cell;calculate lattice energy

Lowest LE ->correct structure

Criteria: van der Waals radii repulsion energy total energy

Pre-LE calcn criteria:van der Waals radiicrystal density range

C1/Ci image at origin & each grid point in succession

order surviving unit cells on basis of LE

MOLPAK-2 flowchart for P2MOLPAK-2 flowchart for P211/c…/c…

Symmetry elements: inversion center,2-fold screw axis, glide plane

Make rectangular boxaround origin,0.5 Å spacing

Page 21: Structure and Density Predictions for Energetic Materials

MOLPAK-2 examples…MOLPAK-2 examples…

MOLPAK-1 failed ->no axial repeatmolecules in coodnsphere

NO2

P-1 P21

1

23

7

5

5(NO2)

P21/c

N

O

CH3

NO2

P212121

NH

HNO O

C2/c

Page 22: Structure and Density Predictions for Energetic Materials

Continuing and future work and goals…Continuing and future work and goals…

•Global atom type parameterization for both WMIN and DMAREL -> new atom types potential function cross-terms anisotropic potential coefficients

•Identification of the best/correct structure -> LE’s and ‘s used currently patterns of intermolecular contacts? crystal habits/crystal face E’s?

•ROTPAK & conformational flexibility -> continue development -> focus on intramolecular E evaluation & multi-bond flexibility

•MOLPAK-2 -> continue development -> handle all space groups extensive testing

Page 23: Structure and Density Predictions for Energetic Materials

•Extend to ionics (eg ADN), H-bonding, high N compounds

•New lattice energy refinement code (WMIN replacement) -> modern fortran

analytical derivatives automate use of individual atom types/ cross-terms in LE potential facilitate conformational refinement

•Sensitivity -> density of states impact/shock & friction – weakest bond + lattice E steric hindrance to sheer

•CHSSI: Super parallel MOLPAK/WMIN w/ B. Rice & W. Mattson

thanks

ARL, Picatinny Indian HeadB. ChapmanK. BaumH. ShechterP. EatonJ. Bottaro