The document analytically studies the unit cell and molecular structures of single-walled carbon nanotubes (SWCNTs) at different chirality values. It finds that the total number of unit cells, carbon atoms, and hexagons in each SWCNT structure changes with chirality. Analytical expressions are derived for the overall unit cell structure, molecular structure, chiral angle, and diameter of SWCNTs. Simulated results for different SWCNT chiralities match the mathematical results, validating both the simulations and expressions.
Periodic material-based vibration isolation for satellitesIJERA Editor
The vibration environment of a satellite is very severe during launch. Isolating the satellitevibrations during
launch will significantly enhance reliability and lifespan, and reduce the weight of satellite structure and
manufacturing cost. Guided by the recent advances in solid-state physics research, a new type of satellite
vibration isolator is proposed by usingperiodic material that is hence called periodic isolator. The periodic
isolator possesses a unique dynamic property, i.e., frequency band gaps. External vibrations with frequencies
falling in the frequency band gaps of the periodic isolator are to be isolated. Using the elastodynamics and the
Bloch-Floquet theorem, the frequency band gaps of periodic isolators are determined. A parametric study is
conducted to provide guidelines for the design of periodic isolators. Based on these analytical results, a finite
element model of a micro-satellite with a set of designed periodic isolators is built to show the feasibility of
vibration isolation. The periodic isolator is found to be a multi-directional isolator that provides vibration
isolation in the three directions.
At Apex Institute, we endeavour to amalgamate the ancient values of uttermost dedication and responsibility that gave teaching a very pious and sacred status, with latest teaching methodologies so as to make the act of learning, a delectable experience. The arduous task is accomplished by a team of diligent academicians and entrepreneurs, who with the years of experience have mastered the techniques to transform even the most abstruse topics easy to comprehend.
Great emphasis is laid on the concepts and fundamentals with a smooth and systematic transition to the advanced levels of teaching. The interaction between students and teachers is always encouraged so as to provide a very healthy environment for growth and learning. During the process of training the students for IIT-JEE/Engg./Medical entrance examinations, great emphasis is laid on the fundamentals so as to excel in the CBSE examination also.
Illustrious faculty and excellent teaching techniques provide you will an infallible approach to success only at Apex Institute.
Our Mission
Generating excellence both in academic and competitive aspects thereby training the youth for most gruelling entrance level exams viz. IIT-JEE/Engg.& Medical entrance.
Our Vision
Generating excellence in academic, exploring creative areas of the dormant self, nurturing talent & aptitude & including perseverance among the students to keep themselves abreast of the latest developments in the field of competitive examinations.
Our Objectives
1. Striving for the best possible education to ambitious students aspiring to join corporate world as medical professionals.
2. Creating a comprehensive understanding of the subjects & help developing strategies to meet arduous competitions among the students to match, excel & ameliorate the competition oriented education.
Text Book: An Introduction to Mechanics by Kleppner and Kolenkow
Chapter 1: Vectors and Kinematics
-Explain the concept of vectors.
-Explain the concepts of position, velocity and acceleration for different kinds of motion.
References:
Halliday, Resnick and Walker
Berkley Physics Volume-1
Slides of my talk at IISc Bangalore on nanomechanics and finite element analysis for statics and dynamics of nanoscale structures such as carbon nanotube, graphene, ZnO nanotube and BN nano sheet.
Periodic material-based vibration isolation for satellitesIJERA Editor
The vibration environment of a satellite is very severe during launch. Isolating the satellitevibrations during
launch will significantly enhance reliability and lifespan, and reduce the weight of satellite structure and
manufacturing cost. Guided by the recent advances in solid-state physics research, a new type of satellite
vibration isolator is proposed by usingperiodic material that is hence called periodic isolator. The periodic
isolator possesses a unique dynamic property, i.e., frequency band gaps. External vibrations with frequencies
falling in the frequency band gaps of the periodic isolator are to be isolated. Using the elastodynamics and the
Bloch-Floquet theorem, the frequency band gaps of periodic isolators are determined. A parametric study is
conducted to provide guidelines for the design of periodic isolators. Based on these analytical results, a finite
element model of a micro-satellite with a set of designed periodic isolators is built to show the feasibility of
vibration isolation. The periodic isolator is found to be a multi-directional isolator that provides vibration
isolation in the three directions.
At Apex Institute, we endeavour to amalgamate the ancient values of uttermost dedication and responsibility that gave teaching a very pious and sacred status, with latest teaching methodologies so as to make the act of learning, a delectable experience. The arduous task is accomplished by a team of diligent academicians and entrepreneurs, who with the years of experience have mastered the techniques to transform even the most abstruse topics easy to comprehend.
Great emphasis is laid on the concepts and fundamentals with a smooth and systematic transition to the advanced levels of teaching. The interaction between students and teachers is always encouraged so as to provide a very healthy environment for growth and learning. During the process of training the students for IIT-JEE/Engg./Medical entrance examinations, great emphasis is laid on the fundamentals so as to excel in the CBSE examination also.
Illustrious faculty and excellent teaching techniques provide you will an infallible approach to success only at Apex Institute.
Our Mission
Generating excellence both in academic and competitive aspects thereby training the youth for most gruelling entrance level exams viz. IIT-JEE/Engg.& Medical entrance.
Our Vision
Generating excellence in academic, exploring creative areas of the dormant self, nurturing talent & aptitude & including perseverance among the students to keep themselves abreast of the latest developments in the field of competitive examinations.
Our Objectives
1. Striving for the best possible education to ambitious students aspiring to join corporate world as medical professionals.
2. Creating a comprehensive understanding of the subjects & help developing strategies to meet arduous competitions among the students to match, excel & ameliorate the competition oriented education.
Text Book: An Introduction to Mechanics by Kleppner and Kolenkow
Chapter 1: Vectors and Kinematics
-Explain the concept of vectors.
-Explain the concepts of position, velocity and acceleration for different kinds of motion.
References:
Halliday, Resnick and Walker
Berkley Physics Volume-1
Slides of my talk at IISc Bangalore on nanomechanics and finite element analysis for statics and dynamics of nanoscale structures such as carbon nanotube, graphene, ZnO nanotube and BN nano sheet.
Multiscale methods for next generation graphene based nanocomposites is proposed. This approach combines atomistic finite element method and classical continuum finite element method.
Feedback Control of Dynamic Systems 8th Edition Franklin Solutions ManualDakotaFredericks
Full download : https://alibabadownload.com/product/feedback-control-of-dynamic-systems-8th-edition-franklin-solutions-manual/ Feedback Control of Dynamic Systems 8th Edition Franklin Solutions Manual
Dynamic stiffness and eigenvalues of nonlocal nano beams - new methods for dynamic analysis of nano-scale structures. This lecture gives a review and proposed new techniques.
APEX INSTITUTE was conceptualized in May 2008, keeping in view the dreams of young students by the vision & toil of Er. Shahid Iqbal. We had a very humble beginning as an institute for IIT-JEE / Medical, with a vision to provide an ideal launch pad for serious JEE students . We actually started to make a difference in the way students think and approach problems. We started to develop ways to enhance students IQ. We started to leave an indelible mark on the students who have undergone APEX training. That is why APEX INSTITUTE is very well known of its quality of education
I am Mathew K. I am a Planetary Science Assignment Expert at eduassignmenthelp.com. I hold a Masters’s Degree in Planetary Science, The University of Chicago, USA. I have been helping students with their homework for the past 8 years. I solve assignments related to Planetary Sciences.
Visit eduassignmenthelp.com or email info@eduassignmenthelp.com.
You can also call on +1 678 648 4277 for any assistance with Planetary Science Assignments.
Multiscale methods for next generation graphene based nanocomposites is proposed. This approach combines atomistic finite element method and classical continuum finite element method.
Feedback Control of Dynamic Systems 8th Edition Franklin Solutions ManualDakotaFredericks
Full download : https://alibabadownload.com/product/feedback-control-of-dynamic-systems-8th-edition-franklin-solutions-manual/ Feedback Control of Dynamic Systems 8th Edition Franklin Solutions Manual
Dynamic stiffness and eigenvalues of nonlocal nano beams - new methods for dynamic analysis of nano-scale structures. This lecture gives a review and proposed new techniques.
APEX INSTITUTE was conceptualized in May 2008, keeping in view the dreams of young students by the vision & toil of Er. Shahid Iqbal. We had a very humble beginning as an institute for IIT-JEE / Medical, with a vision to provide an ideal launch pad for serious JEE students . We actually started to make a difference in the way students think and approach problems. We started to develop ways to enhance students IQ. We started to leave an indelible mark on the students who have undergone APEX training. That is why APEX INSTITUTE is very well known of its quality of education
I am Mathew K. I am a Planetary Science Assignment Expert at eduassignmenthelp.com. I hold a Masters’s Degree in Planetary Science, The University of Chicago, USA. I have been helping students with their homework for the past 8 years. I solve assignments related to Planetary Sciences.
Visit eduassignmenthelp.com or email info@eduassignmenthelp.com.
You can also call on +1 678 648 4277 for any assistance with Planetary Science Assignments.
Instalando Android SDK es la traducción del capitulo 1 del libro Prgramming Android. Cuyo objetivo principal es descargar las herramientas y configurarlas para empezar a programar en Android.
Die Präsentation wurde auf der code.talks 2014 gezeigt und stellt zwei Konzepte von NoSQL Datenbanken vor, dynamisches Schema und horizontale Skalierbarkeit.
How Carbon Nanotubes Collapse on Different Ag Surface?ijrap
The collapse and stability of carbon nanotubes (CNTs) on noble metal silver different surfaces were studied
using molecular mechanics and molecular dynamics simulations. From the results, it can be seen that the
CNTs can collapse spontaneously onto different silver surface [(1 0 0), (1 1 0), (1 1 1)] due to the van der
Waals force between them. Furthermore, the CNT collapsing on (1 0 0) and (1 1 1) surface are much easier
than that on (1 1 0) surface. Moreover, the results show that the collapsed CNTs exhibit as linked graphene
ribbons and have the largest area to contact with the Ag surface, which greatly enhances adhesion between
the CNTs and the Ag surface and keeps the system much more stable.
How Carbon Nanotubes Collapse on Different Ag Surface? ijrap
The collapse and stability of carbon nanotubes (CNTs) on noble metal silver different surfaces were studied
using molecular mechanics and molecular dynamics simulations. From the results, it can be seen that the
CNTs can collapse spontaneously onto different silver surface [(1 0 0), (1 1 0), (1 1 1)] due to the van der
Waals force between them. Furthermore, the CNT collapsing on (1 0 0) and (1 1 1) surface are much easier
than that on (1 1 0) surface. Moreover, the results show that the collapsed CNTs exhibit as linked graphene
ribbons and have the largest area to contact with the Ag surface, which greatly enhances adhesion between
the CNTs and the Ag surface and keeps the system much more stable.
Periodic material-based vibration isolation for satellitesIJERA Editor
The vibration environment of a satellite is very severe during launch. Isolating the satellitevibrations during
launch will significantly enhance reliability and lifespan, and reduce the weight of satellite structure and
manufacturing cost. Guided by the recent advances in solid-state physics research, a new type of satellite
vibration isolator is proposed by usingperiodic material that is hence called periodic isolator. The periodic
isolator possesses a unique dynamic property, i.e., frequency band gaps. External vibrations with frequencies
falling in the frequency band gaps of the periodic isolator are to be isolated. Using the elastodynamics and the
Bloch-Floquet theorem, the frequency band gaps of periodic isolators are determined. A parametric study is
conducted to provide guidelines for the design of periodic isolators. Based on these analytical results, a finite
element model of a micro-satellite with a set of designed periodic isolators is built to show the feasibility of
vibration isolation. The periodic isolator is found to be a multi-directional isolator that provides vibration
isolation in the three directions.
Research Inventy : International Journal of Engineering and Science is published by the group of young academic and industrial researchers with 12 Issues per year. It is an online as well as print version open access journal that provides rapid publication (monthly) of articles in all areas of the subject such as: civil, mechanical, chemical, electronic and computer engineering as well as production and information technology. The Journal welcomes the submission of manuscripts that meet the general criteria of significance and scientific excellence. Papers will be published by rapid process within 20 days after acceptance and peer review process takes only 7 days. All articles published in Research Inventy will be peer-reviewed.
Approximating offset curves using B ´ ezier curves with high accuracyIJECEIAES
In this paper, a new method for the approximation of offset curves is presented using the idea of the parallel derivative curves. The best uniform approximation of degree 3 with order 6 is used to construct a method to find the approximation of the offset curves for B ´ ezier curves. The proposed method is based on the best uniform approximation, and therefore; the proposed method for constructing the offset curves induces better outcomes than the existing methods.
Is ellipse really a section of cone. The question intrigued me for 20 odd years after leaving high school. Finally got the proof on a cremation ground. Only thereafter I came to know of Dandelin spheres. But this proof uses only bare basics within the scope of high school course of Analytical geometry.
Dear Students/Parents
We at 'Apex Institute' are committed to provide our students best quality education with ethics. Moving in this direction, we have decided that unlike other expensive and 5star facility type institutes who are huge investors and advertisers, we shall not invest huge amount of money in advertisements. It shall rather be invested on the betterment, enhancement of quality and resources at our center.
We are just looking forward to have 'word-of-mouth' publicity instead. Because, there is only a satisfied student and his/her parents can judge an institute's quality and it's faculty members coaching.
Those coaching institutes, who are investing highly on advertisements, are actually, wasting their money on it, in a sense. Rather, the money should be invested on highly experienced faculty members and on teaching gears.
We all at 'Apex' are taking this initiative to improve the quality of education along-with each student's development and growth.
Committed to excellence...
With best wishes.
S . Iqbal
( Motivator & Mentor)
Let's dive deeper into the world of ODC! Ricardo Alves (OutSystems) will join us to tell all about the new Data Fabric. After that, Sezen de Bruijn (OutSystems) will get into the details on how to best design a sturdy architecture within ODC.
Accelerate your Kubernetes clusters with Varnish CachingThijs Feryn
A presentation about the usage and availability of Varnish on Kubernetes. This talk explores the capabilities of Varnish caching and shows how to use the Varnish Helm chart to deploy it to Kubernetes.
This presentation was delivered at K8SUG Singapore. See https://feryn.eu/presentations/accelerate-your-kubernetes-clusters-with-varnish-caching-k8sug-singapore-28-2024 for more details.
Connector Corner: Automate dynamic content and events by pushing a buttonDianaGray10
Here is something new! In our next Connector Corner webinar, we will demonstrate how you can use a single workflow to:
Create a campaign using Mailchimp with merge tags/fields
Send an interactive Slack channel message (using buttons)
Have the message received by managers and peers along with a test email for review
But there’s more:
In a second workflow supporting the same use case, you’ll see:
Your campaign sent to target colleagues for approval
If the “Approve” button is clicked, a Jira/Zendesk ticket is created for the marketing design team
But—if the “Reject” button is pushed, colleagues will be alerted via Slack message
Join us to learn more about this new, human-in-the-loop capability, brought to you by Integration Service connectors.
And...
Speakers:
Akshay Agnihotri, Product Manager
Charlie Greenberg, Host
Essentials of Automations: Optimizing FME Workflows with ParametersSafe Software
Are you looking to streamline your workflows and boost your projects’ efficiency? Do you find yourself searching for ways to add flexibility and control over your FME workflows? If so, you’re in the right place.
Join us for an insightful dive into the world of FME parameters, a critical element in optimizing workflow efficiency. This webinar marks the beginning of our three-part “Essentials of Automation” series. This first webinar is designed to equip you with the knowledge and skills to utilize parameters effectively: enhancing the flexibility, maintainability, and user control of your FME projects.
Here’s what you’ll gain:
- Essentials of FME Parameters: Understand the pivotal role of parameters, including Reader/Writer, Transformer, User, and FME Flow categories. Discover how they are the key to unlocking automation and optimization within your workflows.
- Practical Applications in FME Form: Delve into key user parameter types including choice, connections, and file URLs. Allow users to control how a workflow runs, making your workflows more reusable. Learn to import values and deliver the best user experience for your workflows while enhancing accuracy.
- Optimization Strategies in FME Flow: Explore the creation and strategic deployment of parameters in FME Flow, including the use of deployment and geometry parameters, to maximize workflow efficiency.
- Pro Tips for Success: Gain insights on parameterizing connections and leveraging new features like Conditional Visibility for clarity and simplicity.
We’ll wrap up with a glimpse into future webinars, followed by a Q&A session to address your specific questions surrounding this topic.
Don’t miss this opportunity to elevate your FME expertise and drive your projects to new heights of efficiency.
Neuro-symbolic is not enough, we need neuro-*semantic*Frank van Harmelen
Neuro-symbolic (NeSy) AI is on the rise. However, simply machine learning on just any symbolic structure is not sufficient to really harvest the gains of NeSy. These will only be gained when the symbolic structures have an actual semantics. I give an operational definition of semantics as “predictable inference”.
All of this illustrated with link prediction over knowledge graphs, but the argument is general.
UiPath Test Automation using UiPath Test Suite series, part 3DianaGray10
Welcome to UiPath Test Automation using UiPath Test Suite series part 3. In this session, we will cover desktop automation along with UI automation.
Topics covered:
UI automation Introduction,
UI automation Sample
Desktop automation flow
Pradeep Chinnala, Senior Consultant Automation Developer @WonderBotz and UiPath MVP
Deepak Rai, Automation Practice Lead, Boundaryless Group and UiPath MVP
Transcript: Selling digital books in 2024: Insights from industry leaders - T...BookNet Canada
The publishing industry has been selling digital audiobooks and ebooks for over a decade and has found its groove. What’s changed? What has stayed the same? Where do we go from here? Join a group of leading sales peers from across the industry for a conversation about the lessons learned since the popularization of digital books, best practices, digital book supply chain management, and more.
Link to video recording: https://bnctechforum.ca/sessions/selling-digital-books-in-2024-insights-from-industry-leaders/
Presented by BookNet Canada on May 28, 2024, with support from the Department of Canadian Heritage.
PHP Frameworks: I want to break free (IPC Berlin 2024)Ralf Eggert
In this presentation, we examine the challenges and limitations of relying too heavily on PHP frameworks in web development. We discuss the history of PHP and its frameworks to understand how this dependence has evolved. The focus will be on providing concrete tips and strategies to reduce reliance on these frameworks, based on real-world examples and practical considerations. The goal is to equip developers with the skills and knowledge to create more flexible and future-proof web applications. We'll explore the importance of maintaining autonomy in a rapidly changing tech landscape and how to make informed decisions in PHP development.
This talk is aimed at encouraging a more independent approach to using PHP frameworks, moving towards a more flexible and future-proof approach to PHP development.
Slack (or Teams) Automation for Bonterra Impact Management (fka Social Soluti...Jeffrey Haguewood
Sidekick Solutions uses Bonterra Impact Management (fka Social Solutions Apricot) and automation solutions to integrate data for business workflows.
We believe integration and automation are essential to user experience and the promise of efficient work through technology. Automation is the critical ingredient to realizing that full vision. We develop integration products and services for Bonterra Case Management software to support the deployment of automations for a variety of use cases.
This video focuses on the notifications, alerts, and approval requests using Slack for Bonterra Impact Management. The solutions covered in this webinar can also be deployed for Microsoft Teams.
Interested in deploying notification automations for Bonterra Impact Management? Contact us at sales@sidekicksolutionsllc.com to discuss next steps.
DevOps and Testing slides at DASA ConnectKari Kakkonen
My and Rik Marselis slides at 30.5.2024 DASA Connect conference. We discuss about what is testing, then what is agile testing and finally what is Testing in DevOps. Finally we had lovely workshop with the participants trying to find out different ways to think about quality and testing in different parts of the DevOps infinity loop.
IJCER (www.ijceronline.com) International Journal of computational Engineering research
1. International Journal Of Computational Engineering Research (ijceronline.com) Vol. 2 Issue. 5
Analytical Study of Unit Cell and Molecular Structures of Single Walled
Carbon Nanotubes
1
Devi Dass, 2 Rakesh Prasher, 3 Rakesh Vaid*
1, 2, 3
Department of Physics and Electronics, University of Jammu, Jammu-180006, India
Abstract:
Recently it has been experimentally confirmed that the chirality of a nanotube controls the speed of its growth, and the armchair
nanotube should grow the fastest. Therefore, chirality is an important parameter in designing a carbon nanotube (CNT) and
needs to be investigated for the role it plays in the structure of a CNT. In this paper, we have analytically analyzed the unit cell
and molecular structures of various single walled carbon nanotubes (SWCNTs) at different values of chirality combinations.
The results suggest that total number of unit cells, carbon atoms and hexagons in each structure of SWCNTs are being changed
by changing its chirality. A simple and step by step approach has been followed in describing the analytical expressions of
overall unit cell structure, molecular structure, chiral angle and diameter of SWCNTs. The analytical formulations have been
verified by simulating different SWCNTs at various chirality values. The simulated results match very well with the
mathematical results thus validating, both the simulations as well as analytical expressions.
Keywords: chirality, unit cell structure, molecular structure, chiral angle, armchair SWCNT, zigzag SWCNT,
chiral SWCNT
1. Introduction
Carbon nanotubes (CNTs) are fourth allotropes of carbon after diamond, graphite and fullerene, with a cylindrical nanostructure
consisting of graphene sheet (hexagonal arrangement of carbon atoms) rolled into a seamless cylinder with diameter in the
nanometer range i. e. 10-9 m. These tubes were first discovered by Sumio Iijima in 1991 [1] and have been constructed with a
length-to-diameter ratio up to 132,000,000:1 [2] significantly larger than any other material. CNTs are members of the fullerene
structural family, which also includes the spherical buckyballs. Spherical fullerenes are also known as buckyballs, whereas
cylindrical ones are known as CNTs or buckytubes. The diameter of a CNT is of the order of a few nanometers (approx.
1/50,000th of the width of an human hair). The chemical bonding of CNTs is composed entirely of sp2 bonds similar to those of
graphite. These bonds, which are stronger than sp 3 bond found in alkanes, provide nanotubes with their unique strength.
Moreover, carbon nanotubes naturally align themselves into “ropes” held together by Van Der Waals forces [3]. CNTs can be
classified as single walled carbon nanotubes (SWCNTs) and multi walled carbon nanotubes (MWCNTs). SWCNTs consist of
single layer of graphite rolled into a cylinder whereas the MWCNTs consist of multi layers of graphite rolled into a cylinder
and the distance between two layers is 0.34nm [4 - 5]. SWCNTs with diameters of the order of a nanometer can be excellent
conductors [6 - 7]. SWCNTs are formed by rolling a graphene sheet into a cylinder. The way the graphene sheet is rolled is
represented by chiral vector or chirality (n, m). If n = m = l where l is an integer then nanotube formed is known as armchair, if
n = l & m = 0, then nanotube formed is known as zigzag and if n = 2l & m = l, then nanotube formed is known as chiral. It
means chirality (n, m) of the SWCNTs depends on the value of integer l e.g. when l = 4, we have (4, 4) armchair SWCNT, (4,
0) zigzag SWCNT and (8, 4) chiral SWCNT.
2. Mathematical Description of SWCNTs
In this section, we have discussed various single walled carbon nanotubes (SWCNTs) analytically so as to understand various
parameters associated with their operation. To proceed with the discussion on the geometry of SWCNT [8], let us first consider
the geometry of a two dimensional graphene sheet. Figure (1) shows such a sheet where the x- and y- axes are respectively
parallel to a so-called armchair direction and a zigzag direction of the sheet. The point O denotes the origin in the sheet. Each of
the hexagon corners represents the position of a carbon atom. The structure of SWCNT is specified by a vector called the chiral
vector Ch. The chiral vector corresponds to a section of the CNT perpendicular to the tube axis. In figure (1), the unrolled
hexagonal lattice of the CNT is shown, in which OB is the direction of the CNT axis, and OA corresponds to the chiral vector
Ch. By rolling the graphene sheet so that points O and A coincide (and points B and B’ coincide), a paper model of CNT can be
constructed. The vector OB defines another vector named translational vector T. The rectangle generated by the chiral vector Ch
and translational vector T, i.e. the rectangle OAB’B in figure (1), is called the overall unit cell for the SWCNT. When the
overall unit cell is repeated along the length, we get a SWCNT. The chiral vector of the SWCNT is defined as:
Ch = na1 + ma2 ≡ (n, m) (1)
Issn 2250-3005(online) September| 2012 Page 1447
2. International Journal Of Computational Engineering Research (ijceronline.com) Vol. 2 Issue. 5
Figure 1. Formation of various SWCNT using chirality (n, m) [8].
where n, m are integers (0≤ |m| ≤ n) and a1, a2 are the unit vectors of the graphene, a1 specifies the zigzag direction whereas a2
specifies the armchair direction. In figure (1), a1 and a2 can be expressed using the cartesian coordinates (x, y) as,
a1 = a (2)
a2 = a (3)
and the relations:
a1.a1 = a2.a2 = a2 (4)
a1.a2 = (5)
where a = 2.46Å is the lattice constant of the graphite. This constant is related to the carbon-carbon bond length ac-c by
a= ac-c (6)
For graphite, ac-c = 1.42 Å.
From equations (2) and (3), we observe that the lengths of a1, a2, i.e. , are both equal to ac-c = a. By using equations
(2) and (3) in equation (1), the chiral vector Ch can be expressed as
Ch = (n + m) + (n – m) (7)
In figure (1), it can be seen that the circumference length of the SWCNT is the length L of the chiral vector which can be
obtained from equation (7) as
L= =a (8)
The angle between the chiral vector Ch and the zigzag axis (or the unit vector a1) is called chiral angle θ and is defined as by
taking the dot product of Ch and a1, to yield an expression for cos θ:
cos θ = (9)
Or by using (2) and (7),
cos θ = (10)
Similarly, we have
sin θ = (11)
From expressions (10) and (11),
tan θ = (12)
Hence, the chiral angle is given by
θ= (13)
Rolling the sheet shown in figure (1), so that the end of the chiral vector Ch i.e. the lattice point A, coincides with the origin O
leads to the formation of an (n, m) SWCNT whose circumference is the length of the chiral vector, and whose diameter is given
by
d (SWCNT) (nm) = =
Issn 2250-3005(online) September| 2012 Page 1448
3. International Journal Of Computational Engineering Research (ijceronline.com) Vol. 2 Issue. 5
= 0.0783 (14)
If the chiral vector Ch lies on the zigzag axis i.e. θ = 0o and rolling along this axis, a zigzag SWCNT is generated. From
equation (13), we see that θ = 0o corresponds to m = 0 hence a zigzag SWCNT is an (l, 0) SWCNT. If the angle between chiral
vector Ch and the zigzag axis is 30o, it means the chiral vector lies on armchair axis and if the rolling chiral vector along this
axis, an armchair SWCNT is generated. From equation (13), we see that θ = 30o corresponds to n = m = l and hence an
armchair SWCNT is an (l, l) SWCNT. If the chiral vector lies between the zigzag and armchair axis i.e. 0 30o and rolling,
o
a chiral SWCNT is generated. From equation (13), we see that 0 30 corresponds to n ≠ m and m ≠ 0 and hence a chiral
SWCNT is like (2l, l) SWCNT.
The translational vector T may be expressed in terms of a1 and a2 as
T = t1a1 + t2a2 ≡ (t1, t2) (15)
where t1 and t2 are integers. The vector T is normal to the chiral vector Ch and thus parallel to the CNT axis. It represents the
translation required in the direction of the CNT axis to reach the nearest equivalent lattice point. We know that T is
perpendicular to Ch i.e. T.Ch = 0 or (t1a1 + t2a2) . (na1 + na2) = 0. Using equations (4) and (5), the expressions for t1 & t2 in
terms of n & m are obtained as
t1 = +A (2m + n) (16)
t2 = A (2n + m) (17)
The constant A is determined by the requirement that T specifies the translation to the nearest equivalent lattice point i.e. t1 and
t2 do not have a common divisor except unity. Thus,
A= (18)
where dR = gcd (2m + n, 2n + m) and gcd stands for greatest common divisor.
Therefore,
t1 = (19)
t2 = (20)
Hence, from equations (15), (19) & (20), the translational vector T is given by
T= a1 a2 (21)
Or using equations (2) & (3), we get
T= (m-n) + (n+m) (22)
The length of the overall SWCNT unit cell is equal to the magnitude of the translational vector T obtained as
L (SWCNT unit cell) = = (23)
The area of the graphene unit cell is given by
SG = = (24)
and the area of the overall SWCNT unit cell is given by
ST = = (25)
When the area of the overall SWCNT unit cell ST is divided by the area of the graphene unit cell SG, the total number of unit
cells in the overall SWCNT unit cell is obtained as a function of n and m as
N (SWCNT unit cell) = =
= (26)
As each unit cell consists of two carbon atoms, therefore, the total number of carbon atoms in the overall SWCNT unit cell can
be calculated as
NT (SWCNT unit cell) = 2 × N (SWCNT unit cell)
= (27)
3. Results and Discussion
In this section, we have discussed various simulation results such as overall unit cell structures and molecular structures for
various types of SWCNTs obtained using CNTBands [9] simulation tool and verified analytically.
Issn 2250-3005(online) September| 2012 Page 1449
4. International Journal Of Computational Engineering Research (ijceronline.com) Vol. 2 Issue. 5
3.1 Results of Armchair SWCNT
In general, an armchair SWCNT has chirality (n, m) = (l, l) where l is an integer. The values of l are chosen from 1 to 20, so,
we have (n, m) = (1, 1) to (20, 20), and all other parameters are fixed i.e. carbon-carbon spacing = 1.42Å = 0.142nm, tight
binding energy = 3eV, and length in 3D view = 50Å = 5nm. By using these parameters, the following results have been
obtained.
3.1.1 Overall unit cell structures of armchair SWCNT
The overall unit cell structures of armchair SWCNT for different values of chirality are shown in figure (2).
(n=m=1) (n=m=2) (n=m=3) (n=m=4) (n=m=5)
(n=m=6) (n=m=7) (n=m=8) (n=m=9) (n=m=10)
(n=m=11) (n=m=12) (n=m=13) (n=m=14) (n=m=15)
(n=m=16) (n=m=17) (n=m=18) (n=m=19) (n=m=20)
Figure 2. Overall unit cell structures of armchair SWCNT for different values of chirality upto n=m=20.
In figure (2), each green sphere denotes a carbon atom and white stick denote the bonding between two carbon atoms. A unit
cell is a smallest group of atoms and in figure (2), the smallest group consists of two carbon atoms. So, a unit cell consists of
two carbon atoms. It has been observed that the total number of unit cells in the overall unit cell structure of armchair SWCNT
is increased by 2 as the value of l is increased by 1 in its chirality (n = m = l). As each unit cell consists of two carbon atoms,
hence, with the increase in the value of integer l by 1 of the chirality (n = m = l) of armchair SWCNT, the total number of
carbon atoms in its overall unit cell structure is increased by 4. Also, analytically from equation (26), the total number of unit
cells in the overall armchair SWCNT unit cell structure is given by:
N (armchair SWCNT unit cell) = = = = 2l.
Thus, analytically, we can say that with the increase in the value of l by 1 in the chirality (n = m = l) of armchair SWCNT, the
total number of unit cells in its overall unit cell structure is increased by 2. Similarly, from equation (27), the total number of
carbon atoms in the overall armchair SWCNT unit cell structure is given by:
NT (armchair SWCNT unit cell) = = = = 4l.
Hence, we can say that with the increase in the value of l by 1 in the chirality (n = m = l) of armchair SWCNT, the total number
of carbon atoms in its overall unit cell structure is increased by 4. Therefore, the simulated total number of unit cells and
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carbon atoms in the overall unit cell structure of armchair SWCNT are verified analytically. Also, from equation (23) and
simulated results, the length of each armchair SWCNT unit cell is 0.246nm.
3.1.2 Molecular structures of armchair SWCNT
The molecular structures of armchair SWCNT for different values of chirality (n, m) are shown in figure (3).
(n=m=1) (n=m=2) (n=m=3) (n=m=4) (n=m=5)
(n=m=6) (n=m=7) (n=m=8) (n=m=9) (n=m=10)
(n=m=11) (n=m=12) (n=m=13) (n=m=14) (n=m=15)
(n=m=16) (n=m=17) (n=m=18) (n=m=19) (n=m=20)
Figure 3. The molecular structures of armchair SWCNT for different values of chirality upto n=m=20.
As per simulation results, the armchair SWCNT unit cell has repeated 5 times per nm length. If we choose the value of length
of the armchair SWCNT as 5nm, so, the armchair SWCNT unit cell is repeated 25 times along the length. Therefore, the total
number of unit cells in the molecular structure of armchair SWCNT is 25 times the total number of unit cells in its overall unit
cell structure i.e.
N (armchair SWCNT) = 25 N (armchair SWCNT unit cell) = 2 l 25 = 50l.
Hence, with the increase in the value of l by 1 in the chirality (n, m) = (l, l) of armchair SWCNT, the total number of unit cells
in its molecular structure is increased by 50. As each unit cell consists of two carbon atoms, the total number of carbon atoms in
the molecular structure of armchair SWCNT is:
NT (armchair SWCNT) = 2 N (armchair SWCNT) = 2 50l = 100 l.
Hence, with the increase in the value of l by 1 in the chirality (n, m) = (l, l) of armchair SWCNT, the total number of carbon
atoms in its molecular structure is increased by 100.
The number of hexagons in each ring of armchair molecular structure is l, where l (>1 because hexagons not found in (1, 1)
armchair SWCNT) is an integer and the total hexagonal rings in armchair molecular structure = 2 [(Total number of repeated
armchair SWCNT unit cell along the length) – 1] = 2 [25 – 1] = 2 24 = 48. Hence, the total number of hexagons in the
molecular structure of armchair SWCNT is:
NTHEX (armchair SWCNT) = the number of hexagons in each ring of armchair molecular structure the total hexagonal rings in
armchair molecular structure = l 48 = 48 l.
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Hence, with the increase in the value of l by 1 in the chirality (n, m) = (l, l) of armchair SWCNT, the total number of hexagons
in its molecular structure is increased by 48. Also, from equation (13) and simulated results, the chiral angle for armchair
SWCNT is 30o.
3.2 Results of Zigzag SWCNT
In general, a zigzag SWCNT has chirality (n, m) = (l, 0) where l is an integer. The values of l are chosen from 1 to 20, so that
(n, m) = (1, 0) to (20, 0), and all other parameters are fixed i.e. carbon-carbon spacing = 1.42Å = 0.142nm, tight binding energy
= 3eV, and length in 3D view = 50Å = 5nm. By using these parameters, the following results have been obtained.
3.2.1 Overall unit cell structures of zigzag SWCNT
The overall unit cell structures of zigzag SWCNT for different values of chirality (n, m) are shown in figure (4). It has been
observed that the shape of each zigzag SWCNT unit cell is different than the shape of armchair SWCNT unit cell but the total
number of unit cells and the carbon atoms in each zigzag SWCNT unit cell is similar to the armchair SWCNT unit cell. Also,
analytically from equation (26), the total number of unit cells in the overall zigzag SWCNT unit cell structure is given by:
N (zigzag SWCNT unit cell) = = = = 2l.
Hence, analytically, we can say that with the increase in the value of l by 1 in the chirality (n, m) = (l, 0) of zigzag SWCNT, the
total number of unit cells in its overall unit cell structure is increased by 2. Similarly, from equation (27), the total number of
carbon atoms in the overall zigzag SWCNT unit cell structure is given by:
NT (zigzag SWCNT unit cell) = 2 N (zigzag SWCNT unit cell) = = = = 4l.
Hence, analytically, we can say that with the increase in the value of l by 1 in the chirality (n, m) = (l, 0) of zigzag SWCNT, the
total number of carbon atoms in its overall unit cell structure is increased by 4. Hence, simulated number of unit cells and
carbon atoms in the overall unit cell structure of zigzag SWCNT remains the same as verified analytically. Also, from equation
(23) and simulated results, the length of each zigzag SWCNT unit cell is 0.426nm.
(n=1, m=0) (n=2, m=0) (n=3, m=0) (n=4, m=0) (n=5, m=0)
(n=6, m=0) (n=7, m=0) (n=8, m=0) (n=9, m=0) (n=10, m=0)
(n=11, m=0) (n=12, m=0) (n=13, m=0) (n=14, m=0) (n=15, m=0)
(n=16, m=0) (n=17, m=0) (n=18, m=0) (n=19, m=0) (n=20, m=0)
Figure 4. Overall unit cell structures of zigzag SWCNT for different values of chirality upto n=20, m=0.
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3.2.2 Molecular structures of zigzag SWCNT
The molecular structures of zigzag SWCNT for different values of chirality (n, m) are shown in figure (5). As per simulation
results, zigzag SWCNT unit cell has been repeated 3 times for 1nm length, 5 times for 2nm length, 8 times for 3nm length, 10
times for 4nm length and 13 times for 5nm length. If we choose length of zigzag SWCNT as 5nm, so, the zigzag SWCNT unit
cell is repeated 13 times along the length. Therefore, the total number of unit cells in the molecular structure of zigzag SWCNT
is 13 times the total number of unit cells in its overall unit cell structures i.e.
N (zigzag SWCNT) = 13 N (zigzag SWCNT unit cell) = 2l 13 = 26l.
Hence, with the increase in the value of l by 1 in the chirality (n, m) = (l, 0) of zigzag SWCNT, the total number of unit cells in
its molecular structure is increased by 26. As each unit cell consists of two carbon atoms, the total number of carbon atoms in
the molecular structure of zigzag SWCNT is:
NT (zigzag SWCNT) = 2 N (zigzag SWCNT) = 2 26l = 52 l.
Hence, with the increase in the value of l by 1 in the chirality (n, m) = (l, 0) of zigzag SWCNT, the total number of unit cells in
its molecular structure is increased by 52.
The number of hexagons in each ring of zigzag molecular structure is l where l is an integer and the total hexagonal rings in
zigzag molecular structure = 2 [(Total number of repeated zigzag SWCNT unit cell along the length) – 1] = 2 [13 – 1] = 2 12
= 24.
Hence, the total number of hexagons in the molecular structure of zigzag SWCNT is:
NT HEX (zigzag SWCNT) = l 24 = 24 l.
Hence, with the increase in the value of l by 1 in the chirality (n, m) = (l, 0) of zigzag SWCNT, the total number of hexagons in
its molecular structure is increased by 24. Also, we can say that the total number of unit cells, carbon atoms, and hexagons in
each molecular structure of zigzag SWCNT is approximately half of the total number of unit cells, carbon atoms and hexagon
in each molecular structure of armchair SWCNT. Also, from equation (13) and simulated results, the chiral angle for zigzag
SWCNT is 0o.
(n=1, m=0) (n=2, m=0) (n=3, m=0) (n=4, m=0) (n=5, m=0)
(n=6, m=0) (n=7, m=0) (n=8, m=0) (n=9, m=0) (n=10, m=0)
(n=11, m=0) (n=12, m=0) (n=13, m=0) (n=14, m=0) (n=15, m=0)
(n=16, m=0) (n=17, m=0) (n=18, m=0) (n=19, m=0) (n=20, m=0)
Figure 5. The molecular structures of zigzag SWCNT for different values of chirality upto n=20, m=0.
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3.3 Results of Chiral SWCNT
In general, a chiral SWCNT has chirality (n, m) = (2l, l) where l is an integer. The values of l are chosen from 1 to 20, so that
(n, m) = (2, 1) to (20, 10), and keeping all other parameters are fixed i.e., carbon-carbon spacing = 1.42Å = 0.142nm, tight
binding energy = 3eV, and length in 3D view = 50Å = 5nm. By using these parameters, the following results have been
obtained.
3.3.1 Overall unit cell structures of chiral SWCNT
The overall unit cell structures of chiral SWCNT for different values of chirality (n, m) are shown in figure (6).
(n=2, m=1) (n=4, m=2) (n=6, m=3) (n=8, m=4) (n=10, m=5)
(n=12, m=6) (n=14, m=7) (n=16, m=8) (n=18, m=9) (n=20, m=10)
(n=22, m=11) (n=24, m=12) (n=26, m=13) (n=28, m=14) (n=30, m=15)
(n=32, m=16) (n=34, m=17) (n=36, m=18) (n=38, m=19) (n=40, m=20)
Figure 6. Overall unit cell structures of chiral SWCNT for different values of chirality upto n=40, m=20.
As per simulation results, it has been observed that the total number of unit cells in the overall unit cell structure of chiral
SWCNT is increased by 14 as the value of integer l is increased by 1 in its chirality (n, m) = (2l, l). As each unit cell consists of
two carbon atoms, hence, with the increase in the value of integer l by 1, the total numbers of carbon atoms in the overall unit
cell structure of chiral SWCNT is increased by 28. Also, analytically from equation (26), the total number of unit cells in the
overall chiral SWCNT unit cell structure is given by:
N (chiral SWCNT unit cell) = = = = 14l.
Hence, analytically, we can say that with the increase in the value of l by 1 in the chirality (n, m) = (2l, l) of chiral SWCNT, the
total number of unit cells in its overall unit cell structure is increased by 14. Similarly, from equation (27), the total number of
carbon atoms in each zigzag SWCNT unit cell structure is given by:
NT (chiral SWCNT unit cell) = 2 N (chiral SWCNT unit cell) = = = = 28l.
Hence, analytically also, we can say that with the increase in the value of l by 1 in the chirality (n, m) = (2l, l) of chiral
SWCNT, the total number of carbon atoms in its overall unit cell structure is increased by 28.
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Also, as per simulation results, the total number of hexagons in each chiral SWCNT unit cell structure is given by:
NTHEX (chiral SWCNT unit cell) = 4m + 3n n, m 2.
Hence, with the increase in the value of l by 1 in the chirality (n, m) = (2l, l) of chiral SWCNT, the total number of hexagons in
its overall unit cell structure is increased by 10. The hexagons are not found in armchair and zigzag SWCNT unit cell
structures. Also, from equation (23) and simulated results, the length of each chiral SWCNT unit cell is 1.127 nm. Also, we can
say that L (armchair SWCNT unit cell) < L (zigzag SWCNT unit cell) < L (chiral SWCNT unit cell).
3.3.2 Molecular structures of chiral SWCNT
The molecular structures of chiral SWCNT for different values of chirality (n, m) are shown in figure (7).
(n=2, m=1) (n=4, m=2) (n=6, m=3) (n=8, m=4) (n=10, m=5)
(n=12, m=6) (n=14, m=7) (n=16, m=8) (n=18, m=9) (n=20, m=10)
(n=22, m=11) (n=24, m=12) (n=26, m=13) (n=28, m=14) (n=30, m=15)
(n=32, m=16) (n=34, m=17) (n=36, m=18) (n=38, m=19) (n=40, m=20)
Figure 7. The molecular structures of chiral SWCNT for different values of chirality upto n=40, m=20.
As per simulation results, chiral SWCNT unit cell has been repeated 1 times for 1nm and 2nm length, 2 times for 3nm, 4nm
and 5nm length. If we choose length of chiral SWCNT as 5nm, so, the chiral SWCNT unit cell is repeated 2 times along the
length. Therefore, the total number of unit cells in the molecular structure of chiral SWCNT is 2 times the total number of unit
cells in its overall unit cell structures i.e.
N (chiral SWCNT) = 2 N (chiral SWCNT unit cell) = 2 14l = 28l.
Hence, we can say that with the increase in the value of l by 1 in the chirality (n, m) = (2l, l) of chiral SWCNT, the total
number of unit cells in its molecular structure is increased by 28.
As each unit cell consists of two carbon atoms, the total number of carbon atoms in the molecular structure of chiral SWCNT
is: NT (chiral SWCNT) = 2 N (chiral SWCNT) = 2 28l = 56 l.
Hence, we can say that with the increase in the value of l by 1 in the chirality (n, m) = (2l, l) of chiral SWCNT, the total
numbers of carbon atoms in its molecular structure is increased by 56.
As we know that, chiral SWCNT unit cell has been repeated 2 times along the 5nm length. Hence, the total number of hexagons
in the molecular structure of chiral SWCNT can be calculated as:
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NTHEX (chiral SWCNT) = 8 (n + m) n, m 2.
Hence, with the increase in the value of l by 1 in the chirality (n, m) = (2l, l) of chiral SWCNT, the total number of hexagons in
its molecular structure is increased by 24. Also, from equation (13) and simulated results, the chiral angle for chiral SWCNT
lies between 0o and 30o.
A comparison of the total number of unit cells, carbon atoms and hexagons in each overall unit cell structure and molecular
structure for all types of SWCNTs with l from 1, 2, 3, 4, 5,----, 20 has been shown in Table 1.
Table 1. Total no. of unit cells, carbon atoms and hexagons in each overall unit cell and molecular structure of three
types of SWCNTs for l = 1 to 20 i.e by varying the chirality of SWCNTs.
l Armchair SWCNT (n = m = l) Zigzag SWCNT (n = l, m = 0) Chiral SWCNT (n = 2l, m = l)
Overall unit Molecular structure Overall unit Molecular structure Overall unit cell Molecular structure
cell structure cell structure structure
Total Total Total Total Total Total Total Total Total Total Total Total Total Total Total Total
no. no. of no. no. of no. no. no. of no. no. of no. no. no. of no. no. of no. of no. of
of carbon of carbon of of carbon of carbon of of carbon of unit carbon hexa-
unit atoms unit atoms hexa unit atoms unit atoms hexa unit atoms hexa cells atoms gons
cells cells -gons cells cells -gons cells -gons
1 2 4 50 100 n.a 2 4 26 52 n.a 14 28 n.a 28 56 n.a
2 4 8 100 200 96 4 8 52 104 48 28 56 20 56 112 48
3 6 12 150 300 144 6 12 78 156 72 42 84 30 84 168 72
4 8 16 200 400 192 8 16 104 208 96 56 112 40 112 224 96
5 10 20 250 500 240 10 20 130 260 120 70 140 50 140 280 120
6 12 24 300 600 288 12 24 156 312 144 84 168 60 168 336 144
7 14 28 350 700 336 14 28 182 364 168 98 196 70 196 392 168
8 16 32 400 800 384 16 32 208 416 192 112 224 80 224 448 192
9 18 36 450 900 432 18 36 234 468 216 126 252 90 252 504 216
10 20 40 500 1000 480 20 40 260 520 240 140 280 100 280 560 240
11 22 44 550 1100 528 22 44 286 572 264 154 308 110 308 616 264
12 24 48 600 1200 576 24 48 312 624 288 168 336 120 336 672 288
13 26 52 650 1300 624 26 52 338 676 312 182 364 130 364 728 312
14 28 56 700 1400 672 28 56 364 728 336 196 392 140 392 784 336
15 30 60 750 1500 720 30 60 390 780 360 210 420 150 420 840 360
16 32 64 800 1600 768 32 64 416 832 384 224 448 160 448 896 384
17 34 68 850 1700 816 34 68 442 884 408 238 476 170 476 952 408
18 36 72 900 1800 864 36 72 468 936 432 252 504 180 504 1008 432
19 38 76 950 1900 912 38 76 494 988 456 266 532 190 532 1064 456
20 40 80 1000 2000 960 40 80 520 1040 480 280 560 200 560 1120 480
To explain the above mentioned values, we have presented the following examples:
Example 1: How many number of unit cells and carbon atoms in the overall unit cell structure of armchair SWCNT for
chirality n = m = 7. Also, calculate the total number of unit cells, carbon atoms and hexagons in the molecular structure of 5nm
long armchair SWCNT for the same chirality.
Solution: An armchair SWCNT has chirality (n = m = l). Here l = 7.
Therefore, the total number of unit cells in the overall unit cell structure of armchair SWCNT is 2l = 2 × 7 = 14.
Total number of carbon atoms in the overall unit cell structure of armchair SWCNT is 4l = 4 × 7 = 28.
Total number of unit cells in the molecular structure of 5nm long armchair SWCNT is 50l = 50 × 7 = 350.
Total number of carbon atoms in the molecular structure of 5nm long armchair SWCNT is 100l = 100 × 7 = 700.
Total number of hexagons in the molecular structure of 5nm long armchair SWCNT is 48l = 48 × 7 = 336.
Example 2: How many number of unit cells and carbon atoms in the overall unit cell structure of zigzag SWCNT for chirality
n = 7, m = 0. Also, calculate the total number of unit cells, carbon atoms and hexagons in the molecular structure of 5nm long
zigzag SWCNT for the same chirality.
Solution: A zigzag SWCNT has chirality (n = l, m = 0). Here l = 7.
Therefore, the total number of unit cells in the overall unit cell structure of zigzag SWCNT is 2l = 2 × 7 = 14.
Total number of carbon atoms in the overall unit cell structure of zigzag SWCNT is 4l = 4 × 7 = 28.
Total number of unit cells in the molecular structure of 5nm long zigzag SWCNT is 26l = 26 × 7 = 182.
Total number of carbon atoms in the molecular structure of 5nm long zigzag SWCNT is 52l = 52 × 7 = 364.
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Total number of hexagons in the molecular structure of 5nm long zigzag SWCNT is 24l = 24 × 7 = 168.
Example 3: How many number of unit cells, carbon atoms and hexagons in the overall unit cell structure and molecular
structure of 5nm long chiral SWCNT for chirality n = 14, m = 7.
Solution: A chiral SWCNT has chirality (n = 2l, m = l). Here l = 7.
Therefore, the total number of unit cells in the overall unit cell structure of chiral SWCNT is 14l = 14 × 7 = 98.
Total number of carbon atoms in the overall unit cell structure of chiral SWCNT is 28l = 28 × 7 = 196.
Total number of hexagons in the overall unit cell structure of 5nm long chiral SWCNT is 70.
Total number of unit cells in the molecular structure of 5nm long chiral SWCNT is 28l = 28 × 7 = 196.
Total number of carbon atoms in the molecular structure of 5nm long chiral SWCNT is 56l = 56 × 7 = 392.
Total number of hexagons in the molecular structure of 5nm long chiral SWCNT is 168.
4. Conclusions
Based on the analytical formulations and simulation results obtained (see Table 1) using different values of chirality (n, m) in
SWCNTs, the following conclusions have been drawn:
For Armchair SWCNT:
With the increase in the value of l by 1 i.e. with the increase in the chirality (n, m) = (l, l) of armchair SWCNT by 1,
(i) Total number of unit cells in its overall unit cell structure is increased by 2.
(ii) Total number of carbon atoms in its overall unit cell structure is increased by 4.
(iii) Total number of unit cells in its molecular structure is increased by 50.
(iv) Total number of carbon atoms in its molecular structure is increased by 100 and
(v) Total number of hexagons in its molecular structure is increased by 48.
For Zigzag SWCNT:
With the increase in the value of l by 1 in the chirality (n, m) = (l, 0) of zigzag SWCNT,
(i) Total number of unit cells and the carbon atoms in its overall unit cell structure is similar than overall armchair unit cell
structures.
(ii) Total number of unit cells in its molecular structure is increased by 26.
(iii) Total number of carbon atoms in its molecular structure is increased by 52 and
(iv) Total number of hexagons in its molecular structure is increased by 24 i.e. approximately half than the molecular structure
armchair SWCNT.
For Chiral SWCNT:
With the increase in the value of l by 1 in the chirality (n, m) = (2l, l) of chiral SWCNT,
(i) Total number of unit cells in its overall unit cell structure is increased by 14.
(ii) Total number of carbon atoms in its overall unit cell structure is increased by 28.
(iii) Total number of hexagons in the overall unit cell structure is increased by 10.
(iv) Total number of unit cells in its molecular structure is increased by 28.
(v) Total number of carbon atoms in its molecular structure is increased by 56 and
(vi) Total number of hexagons in its molecular structure is increased by 24.
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*
Corresponding Author: Dr Rakesh Vaid Email: rakeshvaid@ieee.org
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