adsorption on single-walled carbon nanohorns

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Adsorption on Single- Walled Carbon Nanohorns Adam Scrivener

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Adsorption on Single-Walled Carbon Nanohorns. Adam Scrivener. What are carbon nanohorns?. Nanostructures made from graphene sheets, forming a dahlia-like structure. Surface area is much greater than graphene, which makes nanohorns a promising material for gas adsorption. What is adsorption?. - PowerPoint PPT Presentation

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Page 1: Adsorption on Single-Walled Carbon Nanohorns

Adsorption on Single-Walled Carbon NanohornsAdam Scrivener

Page 2: Adsorption on Single-Walled Carbon Nanohorns

What are carbon nanohorns?● Nanostructures made from graphene sheets,

forming a dahlia-like structure.● Surface area is much

greater than graphene, which makes nanohorns a promising material for gas adsorption.

Page 3: Adsorption on Single-Walled Carbon Nanohorns

What is adsorption?● Adsorption is the adhesion of atoms or

molecules from a gas, liquid, or dissolved solid to a surface.

● Caused by van der Waals force between an adsorbate (gas molecules/atoms) and an adsorbent (Carbon atoms).

Page 4: Adsorption on Single-Walled Carbon Nanohorns

Applications of adsorption● Gas storage: gas particles can be stored at very high density using

nanohorns, due to the adsorption process and high surface area per volume ratio.

● Gas separation: Several materials, including carbon nanohorns, can be used as a filter in factories to reduce greenhouse gas emissions such as methane and CO2.

● Gas sensing: The ability to monitor how much gas is in a system is invaluable, and carbon-based materials such as carbon nanohorns are perfect for this because of their large specific surface areas.

Page 5: Adsorption on Single-Walled Carbon Nanohorns

The van der Waals force● The van der Waals force is the sum of the

attractive forces between molecules other than those due to covalent bonds or electrostatic interactions involving ions.

● There are no covalent bonds or ions involved in the systems which we deal with, so the electrostatic forces can be disregarded.

Page 6: Adsorption on Single-Walled Carbon Nanohorns

The Lennard-Jones potential● Approximates the interactions between the Carbon

atoms in the nanohorns and the gaseous adsorbate● Incorporates the attractive portion of the van der

Waals force and the repulsive forces caused by overlapping electron orbitals.

Page 7: Adsorption on Single-Walled Carbon Nanohorns

Monte Carlo Simulations● An efficient method of observing the equilibrium properties of the

nanohorn/gas system.● Simulations can be combined with experiments to make it easier to

interpret the results● Using simulations, we can explore parameters that are not possible

in a real-world experiment. E.G., we can set any temperature or pressure that we want, or add impurities to the adsorbent easily.

Page 8: Adsorption on Single-Walled Carbon Nanohorns

The Grand Canonical Monte Carlo Algorithm1. Start with an arbitrary configuration of particles.

Page 9: Adsorption on Single-Walled Carbon Nanohorns

The Grand Canonical Monte Carlo Algorithm1. Start with an arbitrary configuration of particles.2. Randomly choose whether to:

a. Move a particle from the vapor into the system in a random location.

Page 10: Adsorption on Single-Walled Carbon Nanohorns
Page 11: Adsorption on Single-Walled Carbon Nanohorns

The Grand Canonical Monte Carlo Algorithm1. Start with an arbitrary configuration of particles.2. Randomly choose whether to:

a. Move a particle from the vapor into the system in a random location.

b. Move a random particle from the system into the vapor.

Page 12: Adsorption on Single-Walled Carbon Nanohorns
Page 13: Adsorption on Single-Walled Carbon Nanohorns

The Grand Canonical Monte Carlo Algorithm1. Start with an arbitrary configuration of particles.2. Randomly choose whether to:

a. Move a particle from the vapor into the system in a random location.

b. Move a random particle from the system into the vapor.c. Choose a random particle already in the system and move

it in a random direction within some fixed distance ∆.

Page 14: Adsorption on Single-Walled Carbon Nanohorns

Page 15: Adsorption on Single-Walled Carbon Nanohorns

The Grand Canonical Monte Carlo Algorithm1. Start with an arbitrary configuration of particles.2. Randomly choose whether to:

a. Move a particle from the vapor into the system in a random location.

b. Move a random particle from the system into the vapor.c. Choose a random particle already in the system and move it in

a random direction within some fixed distance ∆. 3. Repeat until the system is in equilibrium.

Page 16: Adsorption on Single-Walled Carbon Nanohorns

(After many iterations)

Page 17: Adsorption on Single-Walled Carbon Nanohorns

Energy of Krypton-nanohorn system

40K 60K 77.4K

Egg EggEgg

EgsEgs

Egs

Page 18: Adsorption on Single-Walled Carbon Nanohorns

Krypton Adsorption - Pressure vs. Temperature

40K 60K 77.4K

Page 19: Adsorption on Single-Walled Carbon Nanohorns

Atoms inside

Page 20: Adsorption on Single-Walled Carbon Nanohorns

Krypton Adsorption - Pressure vs. Temperature

40K 60K 77.4K

Page 21: Adsorption on Single-Walled Carbon Nanohorns

Atoms insideand in between

nanohorns

Page 22: Adsorption on Single-Walled Carbon Nanohorns

Krypton Adsorption - Pressure vs. Temperature

40K 60K 77.4K

Page 23: Adsorption on Single-Walled Carbon Nanohorns

Atoms inside and on surface of nanohorns

Page 24: Adsorption on Single-Walled Carbon Nanohorns

Future plans● Simulate Neon instead of Krypton ● Use Neon data to compare to already observed data

from real-world experiments.● This will further affirm that our simulations accurately

represent the equilibrium state of the nanohorn adsorption systems.

● We plan to simulate CO2 as well, and, similarly to Neon, compare to data from real-world experiments.