Showing posts with label carbon nanotubes. Show all posts
Showing posts with label carbon nanotubes. Show all posts

Thursday, February 2, 2023

Creating arbitrarily long graphene and carbon nanotubes. 2nd UPDATE: 2/24/2023: additional proposals for lengthened graphene-nanotube hybrids.

 Copyright 2023 Robert Clark

(patents pending)

(Appended at the bottom below are additional suggestions for combining graphene/carbon nanotubes.)

 Carbon nanotubes were created in the early 1990's. Experiments on them revealed extraordinary strength in the range of 1,000 times higher tensile strength per weight than standard grade steel plate and 100 times higher tensile strength per weight than the strongest steel wires available. 

 Graphene which can be regarded as carbon nanotubes flattened out were discovered about a decade later. Experiments confirmed they had comparable strength to carbon nanotubes.

 The only problem towards making them common industrial materials is that they have only been available in small sizes, at microns to a few millimeters in size.

 This is a proposal for constructing larger size graphene and carbon nanotubes. 

I.)Creating Large Graphene Sheets.

Recent research has produced hybrids of graphene and carbon nanotubes:

James’ bond: A graphene/nanotube hybrid

Rice University’s James Tour Group creates single-surface material for energy storage, electronics

Graphic

Seven-atom rings (in red) at the transition from graphene to nanotube make this new hybrid material a seamless conductor. The hybrid may be the best electrode interface material possible for many energy storage and electronics applications. Image by Yang Yang/Yakobson Group

Graphic

Nanotubes are grown from graphene to create nanoscale odako, so named for the giant Japanese kites they resemble. Image courtesy of the Tour Group


https://news2.rice.edu/2012/11/27/james-bond-a-graphenenanotube-hybrid-2/


 The researchers were able to attach carbon nanotubes to graphene sheets. 

 

Several teams have been able to create such hybrids, [1], [2], [3], [4], [5]. Usually, these are formed by placing nanotubes onto graphene. However, one team was able to place graphene onto nanotube surfaces, [6].


 Repeating such hybrids into multiple layers, the strength and electrical properties of graphene and carbon nanotubes can be extended into 3-dimensions, [7], [8], [9], [10]:


Hybrid Structures of Graphene and Nanotubes Exhibit Unique Mechanical Properties

Carbon nanotube pillars between sheets of graphene may create hybrid structures with a unique balance of strength, toughness and ductility throughout all three dimensions, according to Rice University scientists. Five, seven or eight-atom rings at the junctions can force the graphene to wrinkle. Illustration by Shuo Zhao and Lei Tao
https://www.azonano.com/news.aspx?newsID=33709


 However, other research had shown it is possible to "unzip" carbon nanotubes to turn them into graphene sheets:


Unzipping Carbon Nanotubes: A Peeling Method for the Formation of Graphene Nanoribbons†

First published: 19 August 2009
 Graphical Abstract

Zipper examined: Elegant unzipping procedures result in the clean opening of multiwalled carbon nanotubes, leading to graphene nanoribbons (see scheme). Since graphene exhibits outstanding electronic properties, this method may be important in the development of modern nanoelectronic applications.

Description unavailable

https://onlinelibrary.wiley.com/doi/full/10.1002/anie.200902534?saml_referrer

 Several different methods have been found for accomplishing the unzipping, [11], [12], [13]. However, for my purposes the unzipping has to be targeted, as well as being able to cut the graphene at a targeted location in the graphene/nanotube hybrid. I therefore suggest using electron beams or x-ray beams to cut the graphene/carbon nanotubes at the specified locations:


 The idea would be to slice the graphene-nanotube along the lines shown then open up the material flat, to get a larger single sheet of graphene. Then the process would be repeated to attach further nanotubes, slice them open as well and open them up to get a larger sheet of graphene to make a graphene sheet arbitrarily large.

II.)Creating long nanotubes.

That's for creating arbitrarily large graphene. How about for arbitrarily long nanotubes? First the large graphene sheets would be created. Then methods for rolling up the graphene into carbon nanotubes would be used. Theoretical simulations had shown this possible, [14]:

Graphene Nanoribbons Zip Up
February 23, 2012• Physics 5, s29
Nanoscale planar materials such as graphene could be twisted to fabricate tubular objects.
O. Kit, Phys. Rev. B (2012)
https://physics.aps.org/articles/v5/s29

Figure caption
O. Kit, Phys. Rev. B (2012)


   And this has been experimentally confirmed:

 2013 Oct 4; 4: 2548.
Published online 2013 Oct 4. doi: 10.1038/ncomms3548
Growth of carbon nanotubes via twisted graphene nanoribbons



REFERENCES.

1.)Graphene as an atomically thin interface for growth of vertically aligned carbon nanotubes.
Rahul Rao, Gugang Chen, Leela Mohana Reddy Arava, Kaushik Kalaga, Masahiro Ishigami, Tony F. Heinz, Pulickel M. Ajayan & Avetik R. Harutyunyan 
Scientific Reports volume 3, Article number: 1891 (2013)
https://www.nature.com/articles/srep01891

2.)Growing Carbon Nanotubes from Both Sides of Graphene.
Jinlong Jiang*‡§, Yilun Li‡, Caitian Gao‡#, Nam Dong Kim‡, Xiujun Fan‡, Gunuk Wang‡, Zhiwei Peng‡, Robert H. Hauge‡⊥, and James M. Tour*‡⊥||
ACS Appl. Mater. Interfaces 2016, 8, 11, 7356–7362
Publication Date:February 23, 2016
https://doi.org/10.1021/acsami.5b12254


3.)A Three-Dimensional Carbon Nanotube/Graphene Sandwich and Its Application as Electrode in Supercapacitors.
Zhuangjun Fan, Jun Yan, Linjie Zhi, Qiang Zhang, Tong Wei, Jing Feng, Milin Zhang, Weizhong Qian, Fei Wei
First published: 20 August 2010
https://doi.org/10.1002/adma.201001029

4.)Article
Open Access
Published: 11 March 2019
High-Electrical-Conductivity Multilayer Graphene Formed by Layer Exchange with Controlled Thickness and Interlayer.
Hiromasa Murata, Yoshiki Nakajima, Noriyuki Saitoh, Noriko Yoshizawa, Takashi Suemasu & Kaoru Toko 
Scientific Reports volume 9, Article number: 4068 (2019)
https://www.nature.com/articles/s41598-019-40547-0
5.)A seamless three-dimensional carbon nanotube graphene hybrid material
Yu Zhu, Lei Li, Chenguang Zhang, Gilberto Casillas, Zhengzong Sun, Zheng Yan, Gedeng Ruan, Zhiwei Peng, Abdul-Rahman O. Raji, Carter Kittrell, Robert H. Hauge & James M. Tour 
Nature Communications volume 3, Article number: 1225 (2012)

6.)Open Access
Published: 05 August 2013
Self-Assembly of Graphene on Carbon Nanotube Surfaces.
Kaiyuan Li, Gyula Eres, Jane Howe, Yen-Jun Chuang, Xufan Li, Zhanjun Gu, Litong Zhang, Sishen Xie & Zhengwei Pan 
Scientific Reports volume 3, Article number: 2353 (2013)

7.)AUGUST 2, 2018
Nanotube 'rebar' makes graphene twice as tough
by Mike Williams, Rice University
https://phys.org/news/2018-08-nanotube-rebar-graphene-tough.html
8.)Rebar Graphene
Zheng Yan†, Zhiwei Peng†, Gilberto Casillas∥, Jian Lin‡§, Changsheng Xiang†, Haiqing Zhou†, Yang Yang†‡, Gedeng Ruan†, Abdul-Rahman O. Raji†, Errol L. G. Samuel†, Robert H. Hauge†‡⊥, Miguel Jose Yacaman∥, and James M. Tour†‡§*
ACS Nano 2014, 8, 5, 5061–5068
Publication Date:April 2, 2014
https://doi.org/10.1021/nn501132n

9.)Pillared graphene gains strength
MIKE WILLIAMS – SEPTEMBER 14, 2015
POSTED IN: CURRENT NEWS
https://news2.rice.edu/2015/09/14/pillared-graphene-gains-strength/

10.)Graphene and Carbon Nanotubes: Two Great Materials Even Better Together Researchers use carbon nanotubes to create a reinforced version of graphene.
DEXTER JOHNSON
09 APR 2014
https://spectrum.ieee.org/graphene-and-carbon-nanotubes-two-great-materials-even-better-together


11.)Published: 24 April 2009
Graphene nanoribbons
Unzipping nanotubes
Gavin Armstrong 
Nature Chemistry (2009)
Two methods for producing graphene nanoribbons by unzipping carbon nanotubes have been developed.
https://www.nature.com/articles/nchem.236

12.)Published: 16 April 2009
Longitudinal unzipping of carbon nanotubes to form graphene nanoribbons
Dmitry V. Kosynkin, Amanda L. Higginbotham, Alexander Sinitskii, Jay R. Lomeda, Ayrat Dimiev, B. Katherine Price & James M. Tour 
Nature volume 458, pages872–876 (2009)
https://www.nature.com/articles/nature07872

13.)Unzipping of Single-Walled Carbon Nanotube for the Development of Electrocatalytically Active Hybrid Catalyst of Graphitic Carbon and Pd Nanoparticles.
Siniya Mondal, Sourov Ghosh, and C. Retna Raj
ACS Omega 2018, 3, 1, 622–630
Publication Date:January 19, 2018
https://doi.org/10.1021/acsomega.7b01913

14.)Twisting graphene nanoribbons into carbon nanotubes
O. O. Kit, T. Tallinen, L. Mahadevan, J. Timonen, and P. Koskinen
Phys. Rev. B 85, 085428 – Published 23 February 2012
https://journals.aps.org/prb/abstract/10.1103/PhysRevB.85.085428

UPDATE: 2/14/2023: Squashed together carbon nanotubes and graphene sheets.

(patents pending)  
 A recent report demonstrated producing graphene sheets from squashing carbon nanotubes under diamond anvils:

EDITORIAL FEATURE
New Research Narrows the Gap for Graphene Nanoribbon Applications
Cvetelin Vasilev, Ph.D.
https://www.azonano.com/article.aspx?ArticleID=5868

Article
Published: 06 September 2021
Sub-10-nm graphene nanoribbons with atomically smooth edges from squashed carbon nanotubes.
Changxin Chen, Yu Lin, Wu Zhou, Ming Gong, Zhuoyang He, Fangyuan Shi, Xinyue Li, Justin Zachary Wu, Kai Tak Lam, Jian Nong Wang, Fan Yang, Qiaoshi Zeng, Jing Guo, Wenpei Gao, Jian-Min Zuo, Jie Liu, Guosong Hong, Alexander L. Antaris, Meng-Chang Lin, Wendy L. Mao & Hongjie Dai 
Nature Electronics volume 4, pages 653–663 (2021)
https://www.nature.com/articles/s41928-021-00633-6 (behind paywall)
Free PDF: http://sscms.hpstar.ac.cn/hpstar/upload/files/2021/9/76740ddde9b92399.pdf 


 

 Then the proposal is to use graphene sheets and/or carbon nanotubes laid one on top of another but with only for a short overlap distance compared to their lengths. The test is to see if the high pressure compression can induce the carbon-carbon bonds of graphene/nanotubes between the layers of the graphene/nanotubes. Previous work with graphene and nanotubes have been able to induce much weaker van der Waals bonds between the carbon atoms. These do not have the same strength as the carbon-carbon covalent bonds that prevail in graphene and carbon nanotubes.


 The purpose of the short overlap distance compared to their lengths is that likely there will be a combination of the stronger carbon-carbon bonds and van der Waals bonds between the layers. You might then need several layers to make the equivalent cross-sectional strength of a single graphene/nanotube layer. However, by making this portion of the composite small compared to the rest of the graphene/nanotubes the overall strength to weight ratio will be close to that of the pure graphene or carbon nanotubes.


2nd UPDATE, 2/24/2023: Cyclic graphene growing nanotubes growing graphene.

(patent pending)

 Above was first described methods of growing carbon nanotubes on graphene, as references, [1], [2], [3], [4], [5]. However, reference [6] described growing graphene on nanotubes:

Open Access
Published: 05 August 2013
Self-Assembly of Graphene on Carbon Nanotube Surfaces.
Kaiyuan Li, Gyula Eres, Jane Howe, Yen-Jun Chuang, Xufan Li, Zhanjun Gu, Litong Zhang, Sishen Xie & Zhengwei Pan 
Scientific Reports volume 3, Article number: 2353 (2013)

  Then the proposal is to cycle repetitively first of growing nanotubes onto graphene and then growing graphene onto nanotubes to produce arbitrarily large graphene-nanotube hybrids.
 


  

Saturday, January 25, 2020

Introducing the mechanical rocket motor.I:rotational carbon nanotube propulsion.

Copyright 2020 Robert Clark
(patents pending)

 SpinLaunch has been funded to launch rockets to space electromagnetically from the ground:

Stealth space startup SpinLaunch snares another $35 million from investors.
By Mike Wall
The company's total investment haul is now $80 million.
https://www.space.com/spinlaunch-launch-startup-investment-funding.html

 Though some launch proposals for slinging rockets to space have proposed nearly getting to the full orbital velocity of 7,400 m/s, this proposal seems more modest in proposing getting in the range of 1,500 m/s. The rest of orbital velocity would be provided by onboard rockets.

 However, it may be possible to get the entire propulsion for the flight to orbit by mechanical means. That is, rather then using chemical energy, by using stored mechanical energy. Because of their ultra high strength at lightweight, carbon nanotubes have the capability of serving as the propellant for such an orbital rocket. Below are some earlier discussions on the topic.

 There are several methods discussed of using the nanotubes as the propellant. It is notable they each  would allow SSTO vehicles.

 Also, notable that at a 10,000 m/s rotational rim velocity of a carbon nanotube flywheel, it would provide energy density at 100 times that of lithium batteries.

 So far however, carbon nanotubes only have been made at most at about centimeter lengths. However, this would be no impediment to the propulsion application since you could use very many of the flywheels at the microscale, which when they fly off at off in unison would provide sufficient thrust for a large scale rocket.

 And for the energy storage application very many of the carbon nanotube flywheels could be arranged in arrays to act as large-scale batteries.



*************************************************
From: "Robert Clark" <rgrego...@****.com>
Newsgroups: sci.astro,sci.physics,sci.energy,sci.materials,sci.space.policy
Subject: The Mechanical Rocket Motor. I
Date: 8 Sep 2006 17:54:39 -0700

This page gives the energy storage capacity for a flywheel given the
tensile strength of the material and its density:
 The energy storage per weight is best when the mass is concentrated as
a thin hoop of rotating material, though the energy stored per volume
is less in this configuration.
 If you want to maximize the energy stored per weight criterion, then:
 (energy stored)/mass = (1/2)*(tensile strength)/density .
 For the thin hoop configuration this is also equal to
(1/2)*(velocity)^2. So
 velocity = sqrt(tensile strength/density).
  The tensile strength of multiwalled carbon nanotubes has been
measured to be 150 GPa:
Direct mechanical measurement of the tensile strength and elastic
modulus of multiwalled carbon nanotubes.
B.G. Demczyk et al.
Materials Science and Engineering A334 (2002), 174, 173-178.
http://www.glue.umd.edu/~cumings/PDF%20Publications/16.MSE%20A334demczyk.pdf
 This was for micro-scale samples. It is not known if this strength
will still hold for macro-scale nanotubes, but it has been confirmed at
the micro-scale.
 The density of carbon nanotubes is in the range of 1300 kg/m^3. Then
the possible speed of the hoop could be:
 velocity = sqrt(150 GPa/1300 kg/m^3) = 10,740 m/s.
 This is a tremendously high speed. This raises the possibility they
could be used for rocket propulsion. What you would want to do is
convert this rotational velocity to linear velocity to be able to
impart momentum to the rocket.
 However, you also want the material to all exit in a single direction
to impart the momentum of the rocket in the opposite direction. But if
you induced the hoop to fly apart the materials would fly off in all
directions in the plane of rotation.
 So another possibility would have the nanotube material rotate around
as a thin rod attached at one end. Then if we broke the connection at
this end the rod could be made to fly off in the desired direction by
breaking the connection at the right time in its rotation. However the
rod will not attain the full velocity of its rotational speed at the
free end. The reason is the rod will still retain some rotation because
of conservation of angular momentum. So some of the energy will go into
rotation and some will go into linear translational motion.
 This report by Jerome Pearson calculates the velocity possible at the
tip of a thin uniform rod according to its tensile strength and
density:
 The speed calculated is U = sqrt(2σ/ρ) , σ the tensile strength and
ρ the density. Pearson refers to this as the materials characteristic
velocity. For the carbon nanotube material it would be U = sqrt(2*150
GPa/1300 kg/m^3) = 15,200 m/s.
 However, as I said this would not be the linear speed of the rod
flying off because some of the energy will be retained as rotational
motion. The linear speed of the rod when it flies off should instead be
the speed of the center of mass, which is at the midpoint for the
uniform rod, because of conservation of linear momentum.
 The speed of this midpoint half-way along the rod will be half the tip
speed or 7600 m/s, giving an ISP of 760 s. This compares to the best
liquid hydrogen/liquid oxygen chemical rockets of 450 s. The carbon
nanotubes would also take up much less space since they are denser than
liquid hydrogen. However, the volume would not be found simply from the
density of the carbon nanotubes. This is because you would need space
for the rods to rotate freely before they are released. So the
effective density would be less than 1300 kg/m^3, but still better than
that of liquid hydrogen. You also would not have the volume of the
liquid oxygen to carry.
 You could probably also design the rod in a tapered configuration to
maximize the linear translational velocity. Pearson in his report
calculates the degree of tapering to attain the maximum tip velocity.
The intent of his report was to propose a method of propulsion in the
form of a large 'sling' that could propel mass from an asteroid as a
means to retrieve the asteroid. But the calculations still work for a
tapered rod at the micro-scale.
 This page describes the idea in the form of a launching method for
payloads from Earth:
 To use this idea instead to calculate the speed the tapered rod would
fly off if released, you need to calculate the position of the center
of mass. Using this you can find the speed for the center of mass from
the proportion of its distance from the fixed end to the tip. From
conservation of linear momentum this will be the speed the tapered rod
will receive when released. The center of mass calculation for the
center of mass is rather complicated but I wind up with a speed for the
released rod of v =(characteristic velocity)/sqrt(π) = 8570 m/s, an
ISP of about 860 s. I would like to receive some confirmation on this
calculation though.
 This tapered rod does give a better ISP but you would have the problem
of binding the nanotubes together to result in the right taper. It is
not known whether nanotubes bound together will retain the same
strength of individual nanotubes.
 One possibility would be to use the single atomic layer graphene
recently produced. This has been made in micron-scale sizes which is
sufficient for the purpose. You could cut this in the shape to have the
right taper. I've been informed by one of the scientists who produced
it that it should have the same strength as individual nanotubes.
 This speed though is still less than the speed of the thin rotating
nanotube hoop at 10,400 m/s. One possibility to convert this rotational
motion fully into linear motion in a single direction might be to have
a fixed low friction flat slab with one end very close to and
tangential to the rotating hoop. You cut the hoop at the point closest
to the slab. This point will fly off in a tangential direction then
will move linearly along the surface of the slab. But we want the rest
of the hoop to also move linearly along the surface of the slab. To
insure this you might have the hoop be rotating inside another hoop
kept fixed of a slightly larger diameter.
 This though would increase the weight of the material that has to be
carried along, thus effectively reducing the ISP. However, if this
material is also made of strong nanotube material you might be able to
get a higher velocity of the rotating hoop thereby cancelling out the
effect of the increased weight that has to be carried.
 Both the tangential slab and the containing hoop would have to be made
of very low friction material at the velocities to be used. Carbon
nanotubes remarkably have been found to have very low friction:
Low-Friction Nanoscale Linear Bearing Realized from Multiwall Carbon
Nanotubes.
Science 28 July 2000: Vol. 289. no. 5479, pp. 602 - 604.
http://www.sciencemag.org/cgi/content/abstract/289/5479/602
 Then the rotating hoop, the containing hoop and the fixed slab could
all be made of nanotube material or perhaps of single atomic layer
graphene.

   Bob Clark
*************************************************
From: "Robert Clark" <rgrego...@****.com>
Newsgroups: sci.astro,sci.physics,sci.energy,sci.materials,sci.space.policy
Subject: Re: The Mechanical Rocket Motor. I
Date: 9 Sep 2006 16:10:01 -0700
The spinning of rotors at the micro-scale and the nano-scale has
already been accomplished so this is within the range of what is
currently possible:
Nanomotors realise visionary's dream.
Thursday, 30 October, 2003
"Researchers at Berkeley at the University of California created the
world's smallest electrical device earlier this year - one hundred
million of which could fit on the end of a pin."
http://www.scienceagogo.com/news/20030627221223data_trunc_sys.shtml
Using Nanotubes and Etched Silicon, UC Berkeley Physicists Build
World's Smallest Motor.
Berkeley, CA. July 23rd, 2003.
http://www.nanotech-now.com/ucb-release-07232003.htm
 The spinning motion of the rotor is initiated by electrostatic charge.
You would have to have quadrillions to quintillions of them though at
the nanoscale if they were to amount to thousands of kilos of reaction
mass.
 An automated process would be needed for making the rotors, such as
for example used for integrated circuits.
 Another problem is that the spin of the rotors would have to be
maintained in vacuum. So additional mass for the vacuum chamber would
have to be carried along.

  Bob Clark
*************************************************

Monday, July 30, 2018

Beamed propulsion doable now, and with it space solar power, Page 2: carbon nanotube beam production.

Copyright 2018 Robert Clark
(patents pending)

 In the blog post, Beamed propulsion doable now, and with it space solar power, I discussed microLED's whose extremely high light output can be used for orbital beamed propulsion, space solar power, or laser missile defense. I wondered though if their output could be made even larger by making the light emitters at the nanoscale rather than the microscale.

 Of course for anything at the nanoscale the first thing to comes to mind are the carbon nanotubes because they have so many extraordinary properties. We'll discuss some possible ways to generate the high intensity light via carbon nanotubes. Some of them may also work with nanowires of other types. For each, we'll follow the example of the microLED's of using nanoscale parabolic mirrors to collimate the light thereby forming a more intense beam.

Glow Discharge Light.
One way nanotubes can create light is though electrical breakdown producing an ionization plasma. In general, high voltage passed througn thin wires or though a sharp point electrode can generate a plasma, known as a corona discharge:

Corona discharge.
When the potential gradient (electric field) is large enough at a point in the fluid, the fluid at that point ionizes and it becomes conductive. If a charged object has a sharp point, the electric field strength around that point will be much higher than elsewhere. Air near the electrode can become ionized (partially conductive), while regions more distant do not. When the air near the point becomes conductive, it has the effect of increasing the apparent size of the conductor. Since the new conductive region is less sharp, the ionization may not extend past this local region. Outside this region of ionization and conductivity, the charged particles slowly find their way to an oppositely charged object and are neutralized.

 Or electric arc discharge:

Electric arc.
An electric arc between two nails
An electric arc, or arc discharge, is an electrical breakdown of a gas that produces an ongoing electrical discharge. The current through a normally nonconductive medium such as air produces a plasma; the plasma may produce visible light. An arc discharge is characterized by a lower voltage than a glow discharge and relies on thermionic emission of electrons from the electrodes supporting the arc. An archaic term is voltaic arc, as used in the phrase "voltaic arc lamp".

 The thinner the wires or sharper the point electrodes the more intense the electrical field and the more intense will be the light generated in accordance with Paschen's Law. Because the nanotubes are so thin but at the same time can carry high electrical power, intense plasma generated light can be produced.

Fluorescent Light.
 Fluorescent lamps work by sending an electric current through mercury vapor. This induces UV light to be emitted. The UV interacts with a phosphor on the inner surface of the lamp to emit visible light. The fluorescent lamps could be made at the nanoscale using nanotubes or nanowires. Note that it might even be sufficient to make a UV beam in which case a phosphor would not be needed to make a visible light beam.

Cathode Ray Tube.
 Cathode ray tubes also called vacuum tubes were the primary method of operation for TV's prior to the advent of flat-screen TV's. They work by generating an electron beam and directing it a phosphor covered screen to generated light. Carbon nanotubes are known as efficient electron emitters via application of electric current so can be used to make a CRT at the nanoscale.

Neon Lights.
 Neon lights also work by sending electric current through an inert gas such as neon or xenon. Unlike the fluorescent and CRT cases though it produces directly visible light rather than needing a phosphor.


  Bob Clark






Monday, February 15, 2016

Carbon nanotubes for "ionic wind" craft or "ionocraft".

Copyright 2016 Robert Clark
(Patents Pending) 
 
 Nanotechnology makes possible an "ion drive" for air vehicles analogous to the famous ion drive of NASA's deep space probes:

Carbon nanotubes for "Ionic Wind" Craft or "Ionocraft".
Clark R*
Department of Mathematics, Widener University, USA
Review Article
Volume 1 Issue 2 / Received Date: September 26, 2016 / Published Date: October 20, 2016
Abstract
  Peter Thiel of the Founders Fund once famously said, "We wanted flying cars, and we got 140 characters."But nanotechnology now does make possible the long desired flying cars. It's a different propulsion method though than propellers or jets however. It's propulsion by electric fields known as electrohydrodynamic propulsion (EHD). It works by ionizing air then using electric fields to propel the charged air molecules rearward, thus producing thrust. It's quite analogous to the famous space ion drive of NASA. EHD has been known at least since the sixties. Its problem is, as with ion drive, the thrust is so low. So far the EHD craft have not been able to lift both themselves and their power supplies. The ones made so far leave the power supply on the ground and connect to the craft through power cables. But the equations of EHD suggest the thrust for the power required gets larger for thinner ionizing wires. In fact if the wires are at the nanoscale then this important thrust-to-power ratio can be a hundred times higher than for the craft constructed so far. This would be enough to lift the craft and the power supply. This research is to prove what the mathematics suggests. Note that if it works then all propeller and rotor driven craft become obsolete. Also, intermediate range automobile travel would be taken over by the EHD craft, so a large proportion of carbon-emissions would be eliminated, replaced by this zero-emission travel method. In regards to space propulsion, since EHD is so similar to ion drive, using components at the nanoscale may also work to improve the thrust of ion drive. This would be important to shortening the flight times of spacecraft using such drives. This is important not just for robotic spacecraft but also satellites that use such ion drives to reach their final GEO destinations. As it is now, the ion drives used have such low thrust it takes months for such satellites to reach GEO, resulting in millions of dollars of lost revenue to the satellite companies. Being able to increase the thrust of these drives would reduce the flight time, and therefore reduce this lost revenue.
Keywords: Electrohydrodynamic propulsion; Carbon nanotubes; Nanowires; Ionic wind; Ionocraft; Plasma drive
 
     Bob Clark

Wednesday, February 3, 2016

From nanoscale to macroscale: applications of nanotechnology to production of bulk ultra-strong materials.

Copyright 2016 Robert Clark
(patents pending)


_________________________________________________

Note: this is the technical background to an announced crowdfunding campaign now live, as of February 5, 2016:


_________________________________________________


 For the twenty years since their discovery, the "Holy Grail" of nanotube research has been to produce them in arbitrarily long lengths. They initially were only produced at micron-scale lengths. After intense research, so far they have still only been made in millimeter to centimeter lengths.
 Still, in the micron-scale samples tested, their tensile strength has been measured to be a maximum of 150 gigapascals (GPa) at a density of only 1.6 g/cm3, 200 times stronger than steel at only 1/5th the weight, for an improvement of 1,000 times in strength-to-weight ratio.

 The big question is can we make or combine the nanotubes to macroscale sizes while maintaining the strength of the individual nanotubes? Individual carbon nanotubes and the 2-dimensional form monolayer graphene have been measured at micron-scale lengths to have tensile strengths in the range of 100 to 150 GPa, [1], [2], [3]. Carbon nanotubes have been combined, intermingled into bundles and threads for awhile now. These always have significantly lower strength than the individual nanotubes, [4]. However, this is because there were many single nanotubes connected together by weaker van der Waals forces rather than the stronger carbon-carbon molecular bonds that prevail in individual nanotubes. In these cases, with separate nanotubes weakly connected end-to-end, they can just peal apart under tensile load. This is explained here, [5].

  However, some tests of aligned, arrays of nanotubes at millimeter length scales also showed significantly lower strength than individual micro-scale nanotubes, [6], [7], [8]. This may be because of the predicted effect of longer nanotubes having more defects and therefore becoming weaker. If this is the case, then rather than pursuing arbitrarily long nanotubes it may be better to pursue methods of bonding the micro-scale nanotubes at their ends so that their ultra high strength is maintained.  Some possibilities will be suggested in the following pages.

 Joining nanotubes to arbitrary lengths.
 Tying ropes together has been known to create longer ropes whose strength can be 80% to 90% as strong as the component ropes, [9], [10]. Quite key then is that the capability exists to manipulate individual nanotubes at the nanoscale:

The stress test: One experiment repeatedly bent a nanotube through contortions to see if it would break. All these modifications were performed by the NanoManipulator, with the user guiding the AFM tip by moving the Phantom force-feedback pen. [11], [12], [13]

  See also, [14], [15], [16]. Then the suggestion is to tie the nanotubes together using some of the knots known to maintain near the strength of the original ropes. (patent pending.)

 To prevent slipping of the nanotubes under high tensile load we might use them with “nanobuds” along their lengths, [17].



 Also, since the nanotubes are quite thin they might be expected to cut into each other when knotted thus weakening the strength of the knot. One possibility might be to fill the portion of nanotube that is to be knotted with water or other fluid to make the nanotube more spongy there, [18].

This method of tying nanotubes together to produce greater lengths has already been proven to work to preserve at least one characteristic of nanotubes, high conductivity:


Energy
Nanotube Cables Hit a Milestone: As Good as Copper.
Researchers achieve a goal they've been after since the 1980s—the advance could make cars and airplanes lighter, and renewable energy more practical.
Monday, September 19, 2011 By Katherine Bourzac



 The article describes research by scientists at Rice University who created lightweight electrical cables by mechanically tying together nanotubes.

 An alternative method for linking the nanotubes together would be to connect them with nanotube rings:

Ring Closure of Carbon Nanotubes.
Science, Vol. 293, No. 5533, p. 1299-1301, 17 August 2001
Lightly etched single-walled carbon nanotubes are chemically reacted to form rings. The rings appear to be fully closed as opposed to open coils, as ring-opening reactions did not change the structure of the observed rings. The average diameter of the rings was 540 nanometers with a narrow size distribution. [19]



 These are closed rings formed from one or more nanotubes. They are about 540 nm across so several of the aligned nanotubes would have to be fitted into the rings. One question would be how to tighten the rings around the nanotubes once they were fitted into the rings. One possibility might be to apply heating to the rings so that they lengthen then insert the nanotubes inside. Then as the rings cooled they would shrink back to their normal size forming a tight stricture around the nanotubes. As before with the knotting we may have to fill the rings with a fluid so that they are spongy and don’t cut into the nanotubes.

  Another method for fitting the carbon nanotubes into the rings would be by using ring-shaped nanotubes of materials that are piezoelectric. Carbon nanotubes are not piezoelectric but nanotubes of many different types of materials have been made, such as boron nitride nanotubes and zinc oxide nanotubes. Nanotubes of both these types are piezoelectric, and they can also be made in the form of nanorings, [20], [21]. Then we could apply electric current to these nanorings to get them to expand, insert the carbon nanotubes, then remove the current to get the nanorings to shrink back to their regular size.

  Note that using the rings as a means of binding the ropes together means you are using frictional effects to get the nanotubes to hold together. Then is this any better than the van der Waals forces holding just intermingled nanotubes together? I believe it can be as long as you make the rings stricture tight enough. But if it is made too tight, this would cut into the nanotube ropes reducing their strength. Then the optimal degree of tightening would have to be found to maintain the greatest strength.
 Interestingly, the method of knotting the nanotubes together or binding them by rings might also be applied to the intermingled bundles, that is, to the case where the nanotubes are of different lengths held together by van der Waals forces. You would note the shortest length of the nanotubes composing a bundle and tie knots around the bundle or bind it with rings at short enough intervals to insure that every nanotube is held tightly with a tie or knot at least once all along the length of the bundle.

  Another question that would need to be answered is how binding together a group of equally long nanotubes effects the strength of the nanotubes when the binding is only going around the outer nanotubes. That is, suppose you created a string made from single nanotubes bound end-to-end and measured the string’s strength.

 Then you composed a string by using aligned nanotube arrays that all contained the same number of nanotubes, say 100, and bound these ropes end-to-end with the rings. Would the string composed of the aligned ropes be able to hold 100 times as much as the string composed of individual nanotubes? This is asking a somewhat different question than how knotting weakens the nanotubes. It's asking how strong a composed string will be when a binding can only go around the outer nanotubes composing the string.

  Yet another mechanical method for joining the ends together might be to use some nanotubes bent into shapes as clamps. Since nanotubes have such high stiffness they should as clamps be able to hold the ends of aligned arrays of nanotubes together. Again so the clamps don’t cut into the nanotubes you might want to have the clamping nanotubes and/or the nanotubes that are being tied to be fluid filled.
 A different method of joining individual nanotubes or aligned nanotube arrays end-to-end is suggested by the recent research that created diamond-nanotube composites, [22], [23]. To form the strongest bonds for our purposes, I suggest that the method of creating the strongest nanotubes be used first to create the nanotubes, the arc-discharge method by which the 150 GPa tensile strength nanotubes were made, as in [1]. Then the ends of separate nanotubes or nanotube arrays should be placed on the same diamond seed particle and the high strength microwave CVD method of [4] be used to grow diamond around the ends of both, encasing the tips of each of them inside the diamond thus grown. In order to keep the weight low, you only use a small seed particle and you only grow the diamond large enough to maintain the strong bonds that prevail in individual nanotubes.


 Another highly promising method for joining the nanotube ends arises from the surprising effects found by irradiating nanotubes by electron beam:

Reinforcement of single-walled carbon nanotube bundles by intertube bridging.
Nature Materials, 3, p. 153 – 157, March 2004
During their production, single-walled carbon nanotubes form bundles. Owing to the weak van der Waals interaction that holds them together in the bundle, the tubes can easily slide on each other, resulting in a shear modulus comparable to that of graphite. This low shear modulus is also a major obstacle in the fabrication of macroscopic fibres composed of carbon nanotubes. Here, we have introduced stable links between neighbouring carbon nanotubes within bundles, using moderate electron-beam irradiation inside a transmission electron microscope. [24]

NEWS & VIEWS
Strong bundles.
Nature Materials, 3, 135-136, March 2004.
The mechanical properties of nanotube bundles are limited by the sliding of individual nanotubes across each other.
Introducing crosslinks between the nanotubes by electron irradiation prevents sliding, and leads to dramatic improvements in strength. [25]

 The researchers noted as had others that intermingled bundles of nanotubes were relatively weak compared to the strength of individual tubes, in this case their measurements being of bending strength. However, after electron beam irradiation the bundles achieved almost 70% of the bending modulus strength of individual nanotubes. A similar effect was seen in  [26], [27], [28]. The irradiation produced interconnections between the nanotubes that prevented slipping. Then quite likely this can also be used to combine nanotubes at their ends.

  Electron beam irradiation has also been used to attach nanotubes to sensors in scanning electron microscopes for strength testing. One method used was to direct a small amount of hydrocarbons by focused e-beam to weld the nanotubes to the SEM sensor tip. Then this may also work to weld nanotube ends together, [29]. Note that e-beam irradiation can also be used in concert with the tying or ring binding methods to insure no slipping of the nanotubes.

 Additionally laser irradiation has been used to connect double-walled nanotubes strands together, [30]. This resulted in longer nanotube strands as strong as the original ones. However, the starting strength of these was low at 335.6 MPa. It needs to be tested if this method can maintain the strength of the original nanotubes at the highest measured strengths of 150 GPa.

 Note that these e-beam or laser irradiation methods may also work to produce graphene sheets of large size as well. Currently the 2-dimensional graphene has only been produced in micron-scale sizes, though its strength has been shown to be comparable to that of the highest measured strengths of the nanotubes at 130 GPa, [3]. However, irradiating overlapping graphene sheets on their edges may also allow these to be bonded together.

Friction-stir welding of nanotube arrays.
Another method for joining the aligned arrays of nanotubes might be the method friction-stir welding. This method is used to weld metals while maintaining relatively low temperatures. This reduces the damage to the metals and helps to maintain strength. Since this uses relatively low temperatures it may also work to combine the ends of the aligned arrays of nanotubes.

 The Space Elevator.
 Such high strengths in the 100 to 150 GPa range if they can be maintained in the bonded nanotubes are within the range to make the “space elevator” possible.
 However, even at such high strengths it is expected the space elevator ribbon would require tapering. Then you would need a means of connecting nanotubes ropes to each other of ever increasing diameter. One possibility for accomplishing this might be by using the “y-shaped” nanotubes, [31]. These are nanotubes that branch off into a Y-shape. If each branch is as strong as the base column then we could attach a base column of one to a branch of another, thereby creating larger and larger diameters.

  Using “y-shaped” nanotubes might also be a way to maintain the high strength across connections in general, assuming each branch is as strong as the base, if multiple branches of one are attached to multiple branches of another. To continue this indefinitely, you would need the y-branches to be on both ends of each nanotube.



  If in general, the connections weakened the strength by some factor we would just use enough branches so that the total strength would be the same as the individual nanotubes. Then if the branches are quite short compared to the base column, the total mass would be just a small fraction larger than that of just the base columns alone, so the strength to weight ratio would be about the same.

 In regards to the space elevator, NASA and the SpaceWard Foundation had sponsored a competition with a $1 million prize for a team that can produce a cable material at about double the strength to weight ratio of the strongest commonly used materials now:

Tether Strength Competition.
By the numbers:
Tether Length: 2 m (closed loop)
Tether Weight: 2 g
Breaking Force: 1 ton, 1.5 ton (approx)
Prize Purse: $900k, $1.1M
Best performance to date: 0.72 Ton
Number of Teams: None Yet
Competition Date: February-March, 2009. [32]

 I believe both a carbon nanotube cable joined by one the methods described above and a cable made of the new synthetic diamond could each win this competition.


  Bob Clark


REFERENCES
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2.) Measurements of near-ultimate strength for multiwalled carbon nanotubes and irradiation-induced crosslinking improvements.
Bei Peng, Mark Locascio, Peter Zapol, Shuyou Li, Steven L. Mielke, George C. Schatz &  Horacio D. Espinosa
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3.) Measurement of the Elastic Properties and Intrinsic Strength of Monolayer Graphene.
Changgu Lee, Xiaoding Wei, Jeffrey W. Kysar, James Hone
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4.) Direct Synthesis of Long Single-Walled Carbon Nanotube Strands.
H.W. Zhu,  . L. Xu, D. H. Wu, B. Q. Wei, R. Vajtai, P.M. Ajayan
Science, Vol 296, Issue 5569, 884-886 , 3 May 2002

5.) Pulling nanotubes makes thread.
October 30/November 6, 2002

6.) Tensile tests of ropes of very long aligned multiwall carbon nanotubes.
Z. W. Pan, S. S. Xie, L. Lu, B. H. Chang, L. F. Sun, W. Y. Zhou, G. Wang, and D. L. Zhang
Appl. Phys. Lett. 74, 3152 (1999) 24 May 1999.

7.) Tensile strength of single-walled carbon nanotubes directly measured from their macroscopic ropes.
F. Li, H. M. Cheng, S. Bai, G. Su, M. S. Dresselhaus
Applied Physics Letters, 77, p. 3161 (2000)

8.) Strong Carbon-Nanotube Fibers Spun from Long Carbon-Nanotube Arrays.
Xiefei Zhang, Qingwen Li, Yi Tu, Yuan Li, James Y. Coulter, Lianxi Zheng, Yonghao Zhao, Qianxi Jia, Dean E. Peterson, and Yuntian Zhu
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9.) The Study of Knot Performance

10.) Knot Break Strength vs Rope Break Strength.

11.) Carbon nanotubes.

12.) Bending and buckling of carbon nanotubes under large strain.
M. R. Falvo, G.J. Clary, R.M. Taylor II, V. Chi, F.P. Brooks Jr., S. Washburn and R. Superfine
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13.) Nanomanipulation experiments exploring frictional and mechanical properties of carbon nanotubes.
M. R. Falvo, G. Clary, A. Helser, S. Paulson, R. M. Taylor II, V. Chi, F. P. Brooks Jr, S. Washburn, R. Superfine Microscopy and Microanalysis, 4, p. 504-512. (1998)

14.) Nanotube Nanotweezers.
Science, Vol. 286, No. 5447, p. 2148-2150, 10 December 1999

15.) Fabrication and actuation of customized nanotweezers with a 25 nm gap.
Nanotechnology, 12, p. 331-335, 2001

16.) Three-dimensional manipulation of carbon nanotubes under a scanning electron microscope.
Nanotechnology, 10, p. 244-252, 1999

17.) New Nanomaterial, 'NanoBuds,' Combines Fullerenes and Nanotubes.
March 30th, 2007 By Laura Mgrdichian in Nanotechnology / Materials

18.) Water-filled single-wall carbon nanotubes as molecular nanovalves.
Yutaka Maniwa, Kazuyuki Matsuda, Haruka Kyakuno, Syunsuke Ogasawara, Toshihide Hibi, Hiroaki Kadowaki, Shinzo Suzuki, Yohji Achiba & Hiromichi Kataura.
Nature Materials 6, 135 - 141 (2007)

19.) Ring Closure of Carbon Nanotubes.
Masahito Sano,  Ayumi Kamino,  Junko Okamura,  Seiji Shinkai
Science, Vol. 293, No. 5533, p. 1299-1301, 17 August 2001

20.) A facile sulfur vapor assisted reaction method to grow boron nitride nanorings at relative low temperature.
XIAOPENG HAO ; YONGZHONG WU ; JIE ZHAN ; JIAXIANG YANG ; XIANGANG XU ; MINHUA JIANG
The Journal of Physical Chemistry. B, 2005, vol. 109, no. 41, pp. 19188-19190.

21.) Nanorings: Seamless Circular Nanostructures Could be Sensors, Resonators and Transducers for Nanoelectronic and Biotechnology Applications.
February 26, 2004

22.) Synthesis of a Self-Assembled Hybrid of Ultrananocrystalline Diamond and Carbon Nanotubes.
X. Xiao, J. W. Elam , S. Trasobares , O. Auciello, J. A. Carlisle
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Nagraj Shankar, Nick G. Glumac, Min-Feng Yu, S.P. Vanka
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24.) Reinforcement of single-walled carbon nanotube bundles by intertube bridging.
A.Kis, G. Csányi, J.-P. Salvetat, Thien-Nga Lee, E. Couteau, A. J. Kulik, W. Benoit, J. Brugger & L. Forró
Nature Materials, 3, p. 153 - 157 (2004)

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P.M. Ajayan, F. Banhart
Nature Materials, vol. 3, p. 135-136, March 2004.

26.) Modeling of carbon nanotube clamping in tensile tests.
Chunyu Li, Rodney S. Ruoff, Tsu-Wei Chou .
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27.) Measured properties of carbon nanotubes match theoretical predictions.
August 14, 2008

28.) Electron beam welds nanotubes.
By Ted Smalley Bowen, Technology Research News
August 1/8, 2001.

29.) Tensile Test of Carbon Nanotube using Manipulator in Scanning Electron Microscope.
Seung Hoon Nahm
April 3-4, 2006

The 3rd Korea-U.S. NanoForum.


30.) Connection of macro-sized double-walled carbon nanotube strands by current-assisted laser irradiation.
Tao Gong, Yong Zhang, Wenjin Liu, Jinquan Wei, Kunlin Wang, Dehai Wu, and Minlin Zhong
Journal of Laser Applications -- May 2008 -- Volume 20, Issue 2, pp. 122-126.

31.) Controlled fabrication of hierarchically branched nanopores, nanotubes, and nanowires.
Guowen Meng, Yung Joon Jung, Anyuan Cao, Robert Vajtai,, and Pulickel M. Ajayan
PNAS  May 17, 2005  vol. 102, no. 20,  p. 7074-7078.

32.) Tether Strength Competition.


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