Dla

  • Uploaded by: api-3837919
  • 0
  • 0
  • July 2020
  • PDF

This document was uploaded by user and they confirmed that they have the permission to share it. If you are author or own the copyright of this book, please report to us by using this DMCA report form. Report DMCA


Overview

Download & View Dla as PDF for free.

More details

  • Words: 1,569
  • Pages: 23
MONTE CARLO SIMULATION to study surface diffusion and reaction processes on a fractal catalyst

-Diffusion Limited Aggregation (DLA)

Rajarshi Guha(07302009) Ankit Sharma (07302011) Rahul Kumar (07302006) M.Tech. 2nd Year CL 676 course project

What is a fractal • A fractal is a shape made of parts similar to the whole in some way. It is characterized by self-similarity. • Benoit Mandelbrot lists two qualities that are frequently associated with fractals:  Invariance under displacement: under motion different regions of the object must look similar to each other.  Invariance under scaling: selfsimilarity. Take a large DLA-cluster and simplify it's contour, scale it down to the size of a small DLA-cluster, they will look quite similar.

What is DLA • Diffusion Limited Aggregation (DLA) occurs when a particle undergoes Brownian motion until it makes contact with and sticks to a free-floating cluster of particles. • DLA- “a kinetic critical phenomenon” was invented by two physicists, T.A. Witten and L.M. Sander in 1981. • There are 3 methods of fractal growth1. Percolation 2. Particle-Cluster Aggregation (PCA) 3. Cluster-Cluster Aggregation (CCA) • DLA comes under the category of PCA.

Applications of DLA Physical Processes: • Electrochemical Deposition • Viscous Fingering • Dielectric Breakdown • Monolayer formation on surface (Catalyst formation, carbon deposits etc.) • Polymer generation from solution • Protein Folding etc. Natural Processes: • Snow Flakes • Lichen, Fern and Pine growth • Coral Growth • Creation of planets • Lightning • Corneal neovuscularization etc.

80 100 120

100 120

140 160

Real World Phenomena: • Geographical boundary of a country • Rural to urban migration and continuous growth • Web page and computer game design etc.

140

180 160

200

180

200 -1 0 1

Simulation Generated Christmas Tree

Applications Continued..

Applications continued (simple computer simulations)..

Laws of DLA Fractal growth laws: Power law: If N(r) denotes the number of particles within radius r of a circle (or sphere) encircling a DLA then d N(r)= k r For cluster in a plane d = dm ~ 1.71 is the Fractal dimension. Density-Density correlation: The density-density correlation is defined by Where N is the number of particles and p(r)=1 when lattice node is occupied and p(r)=0 when empty. Power law correlation: C(r) and r in a special range (l
Laws of DLA continues..

Mean square displacement (<X²(t)>)Power law: When diffusion occurs on the ideal surface, the diffusion follows Einstein relation given by in one dimensionA growth process is called diffusion-limited when the aggregate increases in size by one particle at a time rather than by bunches. This happens since the density of particles is low and thus the particles do not come into contact with each other before reaching the aggregate. On a fractal surface Einstein relation does not hold. A power law type correlation can be written asWhere d w >2 is anomalous (or walk) diffusion exponent.

DLA Characteristics Lacunarity effect:

• Lacunarity is a counterpart to the fractal dimension, and describes the degree of gappiness of a fractal. • A fractal is very lacunar if its holes tend to be large. • Recent analysis by Benoit Mandelbrot et al. of very large simulated clusters (more than millions of particles) seem to show, that the cluster becomes more compact while growing.

Radius of Gyration :

The fractal dimension D for a cluster can be defined by the expression

where rg is the radius of gyration for the cluster and N(rg) is the total number of particles within that cluster.

DLA Characteristics continues..

Sticking Coefficient: • Stickiness describes the probability that if a particle strikes the cluster, what is the chance of getting added.

S=0.05

• Stickiness=1 => Wandering particle struck part of the existing structure it always stuck.

S=0.01

Symmetric DLA – Simulation Results1 200 180

Iterations =10000

160 140 120 100 80 60 40 20 0 0

20

40

60

80

100

120

140

160

180

200

Number of Particles = 3789, 200 x 200 grid, Seed at the center, Sfactor= 3.

Simulation Continues.. 1

Density-Density Correlation Function

0.9

Fractal Dimension d = 2 - a 0.85

0.8

0.75

0.7

1200

1000

0

10

20

30

40

50 distance

60

70

80

90

100 mean square displacement

density-density correlation

0.95

800

600

400

200

Brownian Motion of 100th particle before sticking

0 0

10

20

30

40 time

50

60

70

Symmetric DLA – Simulation Results2 200

Iterations =30000

180 160 140 120 100 80 60 40 20 0 0

20

40

60

80

100

120

140

160

180

200

Number of Particles = 21234, 200 x 200 grid, Seed at the center, Sfactor= 3.

Simulation Continues... 1200

Brownian Motion of 100th particle before sticking

800

600

400 1

200 0.99

0 0

10

20

30

40

50

60

70

time

density-density correlation

mean square displacement

1000

0.98

0.97

0.96

0.95

Density-Density Correlation Function

0.94

0

10

20

30

40

50 distance

60

70

80

90

100

Asymmetric DLA – Simulation Results1

5 Seeds Asymmetric growth from seeds

4 Seeds

Asymmetric DLA-Simulation Results2 2.5

10000 particles

-1

40 60 80

mean square displacement

0

50

5

2

1

0

x 10

100

1.5

1

0.5

120

100

140

4 seeds

160

150

0 0

1000

2000

3000

180 200

1 0.5 0

160

-0.5 150 -1

140 160

130

140 120

120

1 seed

5000

6000

7000

8000

Brownian motion of 100th particle 3

x10

5

2.5 mean square displacement

1000 particles Seed oriented growth

4000 time

2

1.5

1

0.5

110

100 100 8

0 0

1000

2000

3000

4000

5000 tim e

6000

7000

8000

9000

10000

Analysis of asymmetric fractals generated 1

3600 particles on 200 x 200 grid

0.9

density-density correlation

0.8

1 seed 190

190

180

180

170

170

160

160

150

140

130

1

130

120

0

120

-1

110 100

110

120

130

140

150

160

170

180

0.3

Correlation 0.1

0 0

180

160

20

40

60 distance

140

120

100

80

100

120

100 80

Fractal Dimension = 2-0.25=1.75 0.1

y vs. x fit 2

5

0

2.5

-0.1

R q eanvs. t s m

fit 1

-0.2

2

-0.3 ln(C(r))

Mean Square Displacement

0.4

190

Brownian motion Of 100th particle x10

0.5

110

200

90 100

0.6

0.2

150

140

0.7

1.5

-0.4

-0.5 Power correlation law: -0.6 C(r)=1.56 x r^(-0.25) -0.7

1

Brownian Motion <X²(t)>=88.13 x t^(0.87) dw = 2.29

0.5

0 0

1000

2000

3000

4000

5000 time

6000

7000

8000

9000

-0.8 -0.9 1.5

2

2.5

3 ln(r)

3.5

4

Analysis of symmetric fractals generated 1200 200 180

1000 mean square displacement

160 140 120 100 80 60 40

800

600

Brownian motion Of 100th particle

400

200

20

20

40

60

80

100

120

140

160

180

0 0

200

10

20

30

40

50

60

tim e 1

0 .9 density-density correlation

0 0

0 .8

0 .7

1450 particles Sfactor=3

0 .6

Correlation

0 .5

0 .4

0 .3

0

1 0

2 0

3 0

4 0

5 0 d is ta n c e

6 0

7 0

8 0

9 0

1 0 0

70

Analysis continues.. y vs. x fit 1

0.1 0

Analyzing by curve fitting we geta = 0.35. hence fractal dimension = 2-0.35 = 1.65

-0.1

ln (C(r))

-0.2 -0.3 -0.4 -0.5

Power correlation law: C(r)=2.64 x r^(-0.35)

-0.6 -0.7 -0.8 2.4

2.6

2.8

3

3.2

3.4 3.6 ln (r)

3.8

4

4.2

4.4

1200

Mean square displacement

1000

800

Mean square Displacement: <X²(t)>=207 x t^(0.41) dw = 4.88

600

400

200

0 0

10

20

30

40 time

50

60

70

Simulation Procedure (Algorithm) Symmetric DLA

Asymmetric DLA



Initialize the grid and define necessary variables (eg. Define diffusion time, seed etc.)



Initialize grid, define necessary variables and distribute seeds randomly.



Release particles from the periphery of the circle.





Apply Brownian motion until it finds the cluster.

Generate a particle within grid and put it in random walk until a particle is encountered.



It sits beside the encountered particle.



The process continues until definite number of particles is attained.



Keep on tracking distance from seed and kill particle if it goes outside.



If particle satisfies Sfactor criteria it is allowed to proceed.



Then particle adheres to one of the free available sites.



The process goes on until the grid circumference is reached.

Application N2O decomposition kinetics by MC simulation (Guo et al., 1994): 2 step kinetics :

Surface coverage θ, when R1=R2 can be expressed as Theoretically: For the 2 step reaction mechanism 2nd step occurs on Catalyst surface. Rate constant K2 is related to speed of surface diffusion v2D by-

Speed of surface diffusion is directly proportional to surface diffusion coefficient. Hence, At constant temperature K2 ∞ D. This approach gives K2 = 0.6

Application Continues.. Ideal surface: Overall rate law by MC simulation Fractal Surface:

Figure showing the DLA fractal generated By Guo et al. (Fractal dimension 1.72) Monte Carlo simulation generated K2 = 0.58 Theoretical K2 = 0.6

Conclusions • Many physiconatural processes are random and MC DLA simulation can actually represent those processes computationally.

• DLA fractals are recognized by their fractal dimension and power law correlation.

• An important application of DLA is to simulate fractal catalyst surface and thereby modifying the rate law of surface reaction.

Related Documents

Dla
June 2020 22
Dla
July 2020 22
Dla Sylwii
June 2020 16
Dla Odwanych1
October 2019 35
Dla Training
May 2020 18
Dla Odwanych
November 2019 21