Showing posts with label Carbon Nanotube. Show all posts
Showing posts with label Carbon Nanotube. Show all posts

Monday, July 20, 2020

New material for lithium-ion storage - Graphdiyne

Researchers has devised new two-dimensional carbon based materials – called Graphydiyne.  

Carbon is the anode material in lithium-ion batteries. Its layered structure allows lithium ions to travel in and out of the spaces between layers during battery cycling. Carbon has a highly conductive two-dimensional hexagonal crystal lattice, and they form a stable, porous network for efficient electrolyte penetration. However, the fine-tuning of the structural and electrochemical properties is difficult as these carbon materials are mostly prepared from polymeric carbon matter in a top-down synthesis.

Graphdiyne being a hybrid two-dimensional network made of hexagonal carbon rings bridged by two acetylene units, has been used as a nanoweb membrane for the separation of isotopes. However, its distinct electronic properties and web-like structure also make graphdiyne suitable for electrochemical applications. Changshui Huang from the Chinese Academy of Sciences, Beijing, and colleagues have investigated the lithium-storage capabilities and electrochemical properties of tailor-made, electronically adjusted graphdiyne derivatives.

The scientists synthesized the graphdiyne derivatives in a bottom-up approach by adding precursors on a copper foil, which self-organized to form ordered layered nanostructures with distinct electrochemical and morphological properties.

Among these functional groups, those exerting electron-withdrawing effects reduced the band gap of graphdiyne and increased its conductivity, the authors reported. The cyano group was especially effective and, when used as an anodic material, the cyano-modified graphdiyne demonstrated excellent lithium-storage capacity and was stable for thousands of cycles, as the authors reported.

The authors conclude that modified graphdiyne can be prepared by a bottom-up strategy, which is also best suited to build functional two-dimensional carbon material architectures for batteries, capacitors, and other electrocatalytic devices.

 


Sunday, May 10, 2020

Storage solution using silicon in battery with the aid of nanotechnology


Silicon along with carbon nanotubes has been used to develop a nanostructure to make an effective design for battery anodes. CNT is used to strengthen the material and modify the way the silicon interacts with lithium, which has been extensively used in electrical cars and other devices.


Scientists at the U.S. Department of Energy's Pacific Northwest National Laboratory have used a novel way to use silicon. Silicon, used in computer chips is attractive as it can hold 10 times the electrical charge per gram compared to graphite. The trouble is, silicon expands greatly when it encounters lithium, and it is too weak to withstand the pressure of electrode manufacturing.


To tackle these issues, a unique nanostructure that prevents silicon's expansion when it is mixed with carbon. Scientist work, which was recently published in the journal Nature Communications, could inform new electrode material designs for other types of batteries and eventually help increase the energy capacity of the lithium-ion batteries in electric cars, electronic devices, and other equipment.


How they do it!!


A conductive and stable form of carbon, graphite is well suited to packing lithium ions into a battery's anode as it charges. Silicon can take on more lithium than graphite, but it tends to expand about 300 percent in volume, causing the anode to break apart. The researchers created a porous form of silicon by aggregating small silicon particles into microspheres about 8 micrometers in diameter.


The electrode with porous silicon structure exhibits a change in thickness of less than 20 percent while accommodating twice the charge of a typical graphite anode. However, unlike previous versions of porous silicon, the microspheres also exhibited extraordinary mechanical strength, thanks to carbon nanotubes that make the spheres resemble balls of yarn.


The researchers created the structure sequentially, starting by coating the carbon nanotubes with silicon oxide. Next, the nanotubes were put into an emulsion of oil and water. Then they were heated to boiling. The coated carbon nanotubes condense into spheres when the water evaporates. Then aluminum and higher heat is used to convert the silicon oxide into silicon, followed by immersion in water and acid to remove by-products. What emerges from the process is a powder composed of the tiny silicon particles on the surface of carbon nanotubes.

Sunday, April 6, 2014

Discovery of EIGHTH colour in the rainbow using Carbon nano tube


Scientists have recently “observed” an invisible eighth colour in the rainbow, a discovery that could have wide-ranging implications in the field of military camouflage and modern surveillance.

The invention of the new basic colour in the spectrum of light was made by physicists at the Randall Monroe University in West Virginia, who were investigating packets of photons that are fired through a cloud of ultracold sodium atoms, colliding with the light and slowing it down. This light was then passed through a series of carbon nanotubes in which the incident angle was enough to bounce the photons back on themselves.

The eighth colour can be thought of as the first addition to the traditional spectrum since Isaac Newton first successfully split white light using a triangular prism in 1671.

There is a possibility that this new colour could be the pioneer in the invention of a invisible cover. While current designs rely on physically bending light around an object or shielding it from a small portion of the spectrum, scientists suggest that simply bathing the target in this previously unseen colour could have dramatic results. 
 
The relative simplicity of the new technology could also have impact on the consumer market, as researchers claim, accessing the colour would not be expensive.

Tuesday, November 1, 2011

Nanotubes for Microscopic Mechanics

In the latest issue of Elsevier's Materials Today, researchers from Spain and Belgium reported on the innovative use of carbon nanotubes to create mechanical components for use in a new generation of micro-machines. While the electronics industry has excelled in miniaturizing components, with individual elements approaching the nanoscale (or a billionth of a meter), reducing the size of mechanical systems has proved much more challenging.

One of the difficulties of shrinking mechanical devices is that the conventional techniques used to produce individual components are not useful when it comes to creating intricate shapes on the microscale. One promising technique is electrical discharge machining (EDM), which uses a spark of electricity to blast away the unwanted material to create complex shapes. However, this method requires that the target material is electrically conductive, limiting the use of EDM on hard, ceramic materials.

But now, by implanting carbon nanotubes in silicon nitride, the ceramic of choice, Manuel Belmonte and colleagues have been able to increase the electrical conductivity of the material by 13 orders of magnitude and have used EDM to produce a microgear without compromising the production time or integrity of the apparatus.

 Carbon nanotubes rose to prominence in the early 1990s when their range of remarkable properties became apparent. These include phenomenal strength and electrical properties that can be tailored to suit. Each tube is made from a rolled up sheet of carbon atoms in a honeycomb-like structure. Unrolled, this sheet is also known as graphene, the innovative material which was the subject of the 2010 Nobel Prize in Physics. Implanted inside a ceramic, these nanotubes form a conductive network that greatly reduces electrical resistance.

 The electrical conductivity of the composite material is much higher, while the mechanical properties of the ceramic are preserved and wear resistance is significantly improved. As the corresponding author, Dr Manuel Belmonte clarifies this breakthrough will allow the manufacture of intricate 3D components, widening the potential use of advanced ceramics and other insulating materials. The team hopes that such nanocomposite materials will find use in emerging applications, such as, microturbines, microreactors, and bioimplants.

Tuesday, February 1, 2011

Touchscreens: Made of Carbon Nanotubes

Touchscreens are not a new thing in this rapidly paced technological world. But what it lacks is its viability as far as the price is concerned. In the upcoming Nano Tech Fair 2011 which is scheduled to take place February 16-18, researchers at Fraunhofer are presenting touchscreens that contain carbon nanotubes.

The versatile nature of touchscreen make it a celebrity in the modern technology. Just touching it slightly with the tips of the fingers is enough. One can effortlessly write, navigate, open menu windows or rotate images on touchscreens. Within fractions of a second one touch is translated into control commands that a computer understands. At first glance, this technology borders on the miraculous, but in real life this mystery just is a wafer-thin electrode under the glass surface of the display made of indium-tin-oxide (ITO). This material is nothing short of ideal for use in touchscreens because it is excellent at conducting slight currents and lets the colours of the display pass through unhampered. But, the problem is: indium is not abundant in nature.

Therefore, private industry is very interested in alternatives to ITO that are similarly efficient. The researchers at Fraunhofer have succeeded at coming up with a new material for electrodes that is on the same level as ITO and on top of it is much cheaper. Its main components are carbon nanotubes and low-cost polymers. This new electrode foil is composed of two layers. One is the carrier, a thin foil made of inexpensive polyethylenterephthalate (PET) used for making plastic bottles. Then a mixture of carbon-nanotubes and electrically conducting polymers is added that is applied to the PET as a solution and forms a thin film when it dries.

In comparison to ITO, these combinations of plastics have not been particularly durable because humidity, pressure or UV light put a strain on the polymers. The layers became brittle and broke down. Only carbon nanotubes have made them stable. The carbon nanotubes harden on the PET to create a network where the electrically conducting polymers can be firmly anchored. That means that this layer is durable in the long run. Ivica Kolaric, project manager from Fraunhofer Institute for Manufacturing Engineering and Automation, admits that the electrical resistance of our layer is somewhat greater than that of the ITO, but it's easily enough for an application in electrical systems. Its merits are more than convincing: carbon is not only low-cost and available all over the world. It is also a renewable resource that can be yielded from organic matter such as wood.

There are a whole series of implementations for the new technology. This foil is flexible and can be used in a variety of ways. Even with this photovoltaic foils can be made to corrugated roofs or other uneven structures. The researcher has already set up pilot production where the foil can be enhanced for a wide range of applications.

Saturday, January 29, 2011

Nanocomposites to monitor wind turbine blade structure

Gary D. Seidel, assistant professor of aerospace engineering in the College of Engineering atVirginia Tech developed a carbon nanotube-enhanced composite for structural health monitoring sensors to improve the resiliency of huge wind turbine blades.

Wind turbine blades enjoy a steady wind but can be damaged by gust-induced vibrations. Seidel proposes to create tiny sensor patches that can be selectively placed in key locations where it is anticipated that damage will start. The patches are made of the same base material as the blade but sprinkled with carbon nanotubes, resulting in a nanocomposite sensor which adds negligible weight to the structure.

The submicroscopic carbon nanotubes can be highly conductive, like invisible, extremely lightweight, electrical wires. Placing the highly conducting carbon nanotubes inside a polymer material makes the resulting nanocomposite patch's conductivity sensitive to deformation. As the material is deformed by a stress on the blade, the nanotubes shift, move closer together, and their conductivity jumps – one mechanism behind the phenomenon known as a piezoresistive response. The change in the nanocomposite conductivity sends a signal to the wind turbine control center, allowing the operator to then know which blade is stressed and should be turned off to prevent further damage to that turbine.

Seidel's focus is on assessing the sensing capabilities of the nanocomposite and building multiscale models for use in structural health monitoring software algorithms. His preliminary models have demonstrated that he can create nanocomposites that respond to stresses with conductivity changes.

Based on the mechanism behind the piezoresistive response of our nanocomposites, necessary tools will be created for nanocomposite sensor development and tailoring for the wind turbine blade application.

Monday, February 22, 2010

STRANGE CARBON NANOTUBES!

Carbon nanotubes (CNTs) are 'strange' nanostructures in a sense that they have both high mechanical strength and extreme flexibility. Deforming a carbon nanotube into any shape would not easily break the structure, and it recovers to original morphology in perfect manner. Researchers in China are exploiting this phenomenon by making CNT sponges consisting of a large amount of interconnected nanotubes, thus showing a combination of useful properties such as high porosity, super elasticity, robustness, and little weight (1% of water density).



The nanotube sponges not only show exciting properties as a porous material but they also are very promising to be used practically in a short time. The production method is simple and scalable, the cost is low, and the sponges can find immediate use in many fields related to water purification.



One of the researchers explains that the nanotube sponges are a completely new structure compared with artificial porous materials in several aspects. The sponge is built entirely with nanotubes through a random (yet desired) interconnection. With a high porosity of >99%, the sponge can be compressed to less than 10% of its original volume yet still recover perfectly. Usually, porous materials tend to become brittle at increasing porosity, thus obtaining a material with both high porosity and flexibility has been challenging.



Carbon nanotubes could take advantage of their high surface area and excellent mechanical strength and flexibility. The scientists synthesized the sponges by a chemical vapor deposition (CVD) process during which the CNTs (multi-walled nanotubes with diameters in the range of 30 to 50nm and lengths of tens to hundreds of micrometers,) self-assembled into a porous, interconnected, three-dimensional framework.



The growth process of the sponges is like a consecutive stacking and penetration of numerous CNT 'piles' into centimeter thickness, which is substantially different from aligned arrays where most of CNTs grow continuously from the bottom to top surface or thin sheets where CNTs were densified into a two-dimensional network during vacuum filtration.

According to the scientists, the CNT sponges are capable of absorbing a wide range of solvents and oils with excellent selectivity, recycle ability, and absorption capacities up to 180 times their own weight, two orders of magnitude higher than activated carbon.



The potential application areas for these sponges are vast. They could be used in large-area oil spill clean-ups, water purification and toxic gas filtration. In addition to environmental applications, the CNT sponges can find use as protective coating, thermal insulator, and high strength-to-weight composite. For example, the sponges can absorb mechanical energy during large-strain deformation, therefore resist foreign force or impact. Their high surface area and porosity are also useful for supporting fine catalyst particles in photo-catalytic devices and fuel cells.

Thursday, January 14, 2010

NEW METHOD PRESENTED FOR SYNTHESIS & GROWTH OF CARBON NANOTUBES

Researchers at the Plasma Physics Research Center of Iran's Islamic Azad University devised a new method to improve the synthesis and growth of carbon nanotubes. Carbon nanotubes synthesized in this new way can be used in manufacturing electron emitters and solid devices with high thermal conductivity.

Since 1991, along with the discovery of carbon nanotubes, researchers have always attempted to optimize their production and to utilize them in different industries. Majid Mojtahedzadeh Larijani, one of the researchers, undertook this study with the aim of synthesizing carbon nanotubes by a novel method, which is the growth on the beds with catalytic base by means of ionic bombardment.
The bed used in this study was steel. First in the process, sub-layer underwent surface was treated by argon ionic bombardment at different ion energies and doses. Then by Chemical Vapor Deposition method carbon nanotube growth on bombarded samples using hydrogen and steel gases was accomplished.

The results showed that ion energy and dose in which sub-layer surface turns into fine grains are very appropriate for the growth of dense and adhesive carbon nanotubes. These nanotubes could be applied for manufacturing electron emitters and solid devices with high thermal conductivity in electronics industry.

Monday, November 9, 2009

ILL EFFECTS OF CARBON NANOTUBE

Excerpt: Inhaled carbon nanotubes accumulate within cells at the pleural lining of the lung as visualized by light microscopy.

Carbon nanotubes are being considered for use in everything from sports equipment to medical applications, but a great deal remains unknown about whether these materials cause respiratory or other health problems. Now a collaborative study from North Carolina State University, The Hamner Institutes for Health Sciences, and the National Institute of Environmental Health Sciences shows that inhaling these nanotubes can affect the outer lining of the lung, though the effects of long-term exposure remain unclear.

Using mice in an animal model study, the researchers set out to determine what happens when multi-walled carbon nanotubes are inhaled. Specifically, researchers wanted to determine whether the nanotubes would be able to reach the pleura, which is the tissue that lines the outside of the lungs and is affected by exposure to certain types of asbestos fibers which cause the cancer mesothelioma. The researchers used inhalation exposure and found that inhaled nanotubes do reach the pleura and cause health effects.

Short-term studies do not allow conclusions about long-term responses such as cancer. However, the inhaled nanotubes "clearly reach the target tissue for mesothelioma and cause a unique pathologic reaction on the surface of the pleura, and caused fibrosis," says Dr. James Bonner, associate professor of environmental and molecular toxicology at NC State and senior author of the study. The "unique reaction" began within one day of inhalation of the nanotubes, when clusters of immune cells (lymphocytes and monocytes) began collecting on the surface of the pleura. Localized fibrosis, or scarring on parts of the pleural surface that is also found with asbestos exposure, began two weeks after inhalation.

The study showed the immune response and fibrosis disappeared within three months of exposure. However, this study used only a single exposure to the nanotubes. "It remains unclear whether the pleura could recover from chronic, or repeated, exposures," Bonner says. "More work needs to be done in that area and it is completely unknown at this point whether inhaled carbon nanotubes will prove to be carcinogenic in the lungs or in the pleural lining."

The mice received a single inhalation exposure of six hours as part of the study, and the effects on the pleura were only evident at the highest dose used by the researchers - 30 milligrams per cubic meter (mg/m3). The researchers found no health effects in the mice exposed to the lower dose of one mg/m3.

Tuesday, February 17, 2009

DESCRIPTION OF DIFFERENT TYPES OF CNT

1. SWCNT [Short Length]


SSA: 450 - 550 m2/g
Conductivity: 102~~10-4 S/cm
SWNTs Ash :  1.6 wt%              Metal Content: Nil              Thermal conductivity: 3000 ± 450 W/m.K Density: 1.33 - 1.4g.cm3           Color: Black                   Current Carrying Capacity: 1 Billion A/cm2 Tensile Strength: 45 Billion Pa                 Temperature stability: 2800 degrees Celcius in vacuum Rate:

Single-walled nanotubes (SWNTs) Purity : 98 vol% (carbon nanotubes)
 70 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 3 - 8 µm

Amorphous Carbon Content - 2 wt%          Price Range 1-10gms($120/gm) ; 11-25gms($110/gm) ;       26-50gms($100/gm);       51-100gms($90/gm);       101-250gms($80/gm);         251-500gms($70/gm) 501-1000gms($60/gm)

 Single-walled nanotubes (SWNTs) Purity -  90 vol% (carbon nanotubes)
 65 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 3 - 8 µm

Amorphous Carbon Content <5 wt% Price Range 1-10gms($110/gm);               11-25gms($100/gm) 26-50gms($90/gm);         51-100gms($80/gm) ;      101-250gms($70/gm) ;        251-500gms($60/gm) 501-1000gms($50/gm)

S-SL-3 Single-walled nanotubes (SWNTs)      Purity -  80 vol% (carbon nanotubes)
50 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 3 - 8 µm

Amorphous Carbon Content - 5 wt% Price Range 1-10gms($100/gm);     11-25gms($90/gm);                26-50gms($80/gm);      51-100gms($70/gm);      101-250gms($60/gm);          251-500gms($50/gm) ;  501-1000gms($40/gm)

2.      SWCNT [Medium Length]                          SSA: 450 - 550m2/g Conductivity: 102~~10-4 S/cm SWNTs Ash : 1.6 wt%                Metal Content: Nil               Thermal conductivity: 3000 ± 450 W/m.K Density: 1.33 - 1.4g.cm3              Color: Black                      Current Carrying Capacity: 1 Billion A/cm2 Tensil Strength: 45 Billion Pa                                  Temperature stability: 2800 degrees Celcius in vacuum

S-ML-1 Single-walled nanotubes (SWNTs) Purity - 98 vol% (carbon nanotubes)
 70 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 5 - 15 µm

Amorphous Carbon Content -2 wt%              Price Range 1-10gms($120/gm)    11-25gms($110/gm)      26-50gms($100/gm)         51-100gms($90/gm)         101-250gms($80/gm)         251-500gms($70/gm) 501-1000gms($60/gm)

S-ML-2 Single-walled nanotubes (SWNTs) Purity -  90 vol% (carbon nanotubes)
65 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 5 - 15 µm

Amorphous Carbon Content -5 wt%       Price Range       1-10gms($110/gm)         11-25gms($100/gm) 26-50gms($90/gm)     51-100gms($80/gm)      101-250gms($70/gm)                 251-500gms($60/gm) 501-1000gms($50/gm)

S-ML-3 Single-walled nanotubes (SWNTs) Purity -  80 vol% (carbon nanotubes)
 50 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 5 - 15 µm

Amorphous Carbon Content - 5 wt%     Price Range          1-10gms($100/gm)           11-25gms($90/gm)26-50gms($80/gm)          51-100gms($70/gm)        101-250gms($60/gm)            251-500gms($50/gm)501-1000gms($40/gm)

3.    SWCNT [Long Length] SSA: 450 - 550 m2/g      Conductivity: 102~~10-4 S/cm 
SWNTs Ash 1.6 wt%              Metal Content: Nil            Thermal conductivity: 3000 ± 450 W/m.K Density: 1.33 - 1.4g.cm3          Color: Black            Current Carrying Capacity: 1 Billion A/cm2           Tensil Strength: 45 Billion Pa              Temperature stability: 2800 degrees Celcius in vacuum

S-LL-1 Single-walled nanotubes (SWNTs) Purity 98 vol% (carbon nanotubes)
70 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 15 - 30 µm

Amorphous Carbon Content - 2 wt%       Price Range    1-10gms($120/gm)               11-25gms($110/gm)26-50gms($100/gm)         51-100gms($90/gm)           101-250gms($80/gm)             251-500gms($70/gm)501-1000gms($60/gm)

 S-LL-2 Single-walled nanotubes (SWNTs) Purity  90 vol% (carbon nanotubes)
65 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 15 - 30 µm

Amorphous Carbon Content - 5 wt%         Price Range     1-10gms($110/gm)         11-25gms($100/gm)26-50gms($90/gm)           51-100gms($80/gm)          101-250gms($70/gm)        251-500gms($60/gm)501-1000gms($50/gm)

S-LL-3 Single-walled nanotubes (SWNTs) Purity  80 vol% (carbon nanotubes)
50 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 15 - 30 µm

Amorphous Carbon Content - 5 wt%          Price Range      1-10gms($100/gm)          11-25gms($90/gm)26-50gms($80/gm)            51-100gms($70/gm)             101-250gms($60/gm)          251-500gms($50/gm)501-1000gms($40/gm)

4.     MWCNT [Short Length]       SSA: 50 - 350 m2/g            Conductivity: 102~~10-4 S/cm              SWNTs Ash - 1.6 wt%             Metal Content: Nil           Thermal conductivity: 2400 ± 400 W/m.K         Color: Black                 Current Carrying Capacity: 1 Billion A/cm2          Tensil Strength: 45 Billion Pa Temperature stability: 700 degrees Celcius in vacuum

M - SL - 1 Multi-walled nanotubes (MWNTs) Purity - 90 vol% (CNTs)
70 vol% (Multi-walled nanotubes)
Average Diameter 4 - 12+ (TEM)
Length 3 - 10 µm

Amorphous Carbon Content - 5 wt%           Price Range                1-10gms($60/gm)11-25gms($55/gm)26-50gms($50/gm)          51-100gms($45/gm)             101-250gms($40/gm)           251-500gms($35/gm)501-1000gms($30/gm)   

M - SL - 2 Multi-walled nanotubes (MWNTs)    Purity -  80 vol% (CNTs)
65 vol% (Multi-walled nanotubes)
Average Diameter 4 - 12+ (TEM)
Length 3 - 10 µm

Amorphous Carbon Content - 6 wt%             Price Range       1-10gms($50/gm)           11-25gms($45/gm)26-50gms($40/gm)             51-100gms($35/gm)         101-250gms($30/gm)       251-500gms($25/gm)501-1000gms($20/gm)

M - SL - 3 Multi-walled nanotubes (MWNTs) Purity- 65 vol% (carbon nanotubes)
50 vol% (Multi-walled nanotubes)
Average Diameter 4 - 12+ (TEM)
Length 3 - 10 µm

Amorphous Carbon Content - 8 wt%      Price Range      1-10gms($40/gm)               11-25gms($35/gm)26-50gms($30/gm)             51-100gms($25/gm)         101-250gms($20/gm)        251-500gms($15/gm)501-1000gms($10/gm)

5.  MWCNT [Medium Length] SSA: 50 - 350 m2/g           Conductivity: 102~~10-4 S/cm              SWNTs Ash : - 1.6 wt%               Metal Content: Nil              Thermal conductivity: 2400 ± 400 W/m.K Color: Black                   Current Carrying Capacity: 1 Billion A/cm2     Tensil Strength: 45 Billion Pa Temperature stability: 700 degrees Celcius in vacuum


M - ML - 1 Multi-walled nanotubes (MWNTs) Purity - 90 vol% (CNTs)
70 vol% (Multi-walled nanotubes)
Average Diameter 4 - 12 (TEM)
Length 5 - 15 µm

Price Range   1-10gms($60/gm)    11-25gms($55/gm)    26-50gms($50/gm)          51-100gms($45/gm)101-250gms($40/gm)    251-500gms($35/gm)    501-1000gms($30/gm)



M - ML - 2 Multi-walled nanotubes (SWNTs)
Purity > 80 vol% (carbon nanotubes)
>65 vol% (Multi-walled nanotubes)
Average Diameter 4 - 12+ (TEM)
Length 5 - 15 µm

Amorphous Carbon Content - 6 wt%           Price Range 1-10gms($50/gm)               11-25gms($45/gm)26-50gms($40/gm)           51-100gms($35/gm)           101-250gms($30/gm)        251-500gms($25/gm)501-1000gms($20/gm)

 M - ML - 3 Multi-walled nanotubes (MWNTs) Purity - 70 vol% (CNTs)
50 vol% (Multi-walled nanotubes)
Average Diameter 4 - 12 + (TEM)
Length 5 - 15 µm

Amorphous Carbon Content - 8 wt%           Price Range    1-10gms($40/gm)            11-25gms($35/gm)26-50gms($30/gm)        51-100gms($25/gm)       101-250gms($20/gm)              251-500gms($15/gm)501-1000gms($10/gm)


6. MWCNT [Long Length]      SSA: 50 - 350 m2/g       Conductivity: 102~~10-4 S/cm                          SWNTs Ash- 1.6 wt%       Metal Content: Nil            Thermal conductivity: 2400 ± 400 W/m.K          Color: Black              Current Carrying Capacity: 1 Billion A/cm2       Tensil Strength: 45 Billion Pa Temperature stability: 700 degrees Celcius in vacuum

M - LL - 1 Multi-walled nanotubes (MWNTs) Purity - 90 vol% (CNTs)
 70 vol% (Multi-walled nanotubes)
Average Diameter 4 - 12 + (TEM)
Length 15 - 30 µm

Amorphous Carbon Content - 5 wt%        Price Range          1-10gms($60/gm)         11-25gms($55/gm)26-50gms($50/gm)                51-100gms($45/gm)          101-250gms($40/gm)      251-500gms($35/gm)501-1000gms($30/gm)

 M - LL - 2 Multi-walled nanotubes (MWNTs) Purity - 80 vol% (CNTs)
 65 vol% (Multi-walled nanotubes)
Average Diameter 4 - 12 + (TEM)
Length 15 - 30 µm

Amorphous Carbon Content -6 wt%         Price Range    1-10gms($50/gm)    11-25gms($45/gm)           26-50gms($40/gm)          51-100gms($35/gm)         101-250gms($30/gm)          251-500gms($25/gm)501-1000gms($20/gm)

M - LL - 3 Multi-walled nanotubes (MWNTs) Purity - 70 vol% (CNTs)
 50 vol% (Multi-walled nanotubes)
Average Diameter 4 - 12 + (TEM)
Length 15 - 30 µm

Amorphous Carbon Content - 8 wt%      Price Range 1-10gms($40/gm)     11-25gms($35/gm)        26-50gms($30/gm)      51-100gms($25/gm)     101-250gms($20/gm)    251-500gms($15/gm)   501-1000gms($10/gm)

7. COOH - FUNCTIONALIZED SWCNT [Short Length] -COOH content: 0.5 ~ 3 wt% SSA: 350 - 500 m2/g Conductivity: 102~~10-4 S/cm Metal Content: Nil Content of -OH: < 2 wt% Color: Black Ash: <1>3wt%
Current Carrying Capacity: 1 Billion A/cm2
Tensil Strength: 45 Billion Pa
Temperature stability: 2800 degrees Celcius in vacuum
Thermal conductivity: 2400 ± 400 W/m.K


SC - SL - 1 Single-walled nanotubes-COOH functionalized
Purity > 98 vol% (carbon nanotubes)
> 70 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 3 - 8 µm
Amorphous Carbon Content <2 wt% Price Range 1-10gms($200/gm)11-25gms($180/gm)26-50gms($160/gm) SC - SL - 2 Single-walled nanotubes-COOH functionalized Purity > 90 vol% (carbon nanotubes)
> 65 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 3 - 8 µm
Amorphous Carbon Content <5 wt% Price Range 1-10gms($190/gm)11-25gms($170/gm)26-50gms($150/gm) SC - SL - 3 Single-walled nanotubes-COOH functionalized Purity > 80 vol% (carbon nanotubes)
> 50 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 3 - 8 µm
Amorphous Carbon Content <5 wt% Price Range 1-10gms($180/gm)11-25gms($160/gm)26-50gms($140/gm) 8. COOH - FUNCTIONALIZED SWCNT [Medium Length] -COOH content: 0.5 ~ 3 wt% SSA: 350 - 500 m2/g Conductivity: 102~~10-4 S/cm Metal Content: Nil Content of -OH: < 2 wt% Color: Black Ash: <1>3wt%
Current Carrying Capacity: 1 Billion A/cm2
Tensil Strength: 45 Billion Pa
Temperature stability: 2800 degrees Celcius in vacuum
Thermal conductivity: 2400 ± 400 W/m.K


SC - ML - 1 Single-walled nanotubes-COOH functionalized
Purity > 98 vol% (carbon nanotubes)
> 70 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 5 - 15 µm
Amorphous Carbon Content <2 wt% Price Range 1-10gms($200/gm)11-25gms($180/gm)26-50gms($160/gm) SC - ML - 2 Single-walled nanotubes-COOH functionalized Purity > 90 vol% (carbon nanotubes)
> 65 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 5 - 15 µm
Amorphous Carbon Content <5 wt% Price Range 1-10gms($190/gm)11-25gms($170/gm)26-50gms($150/gm) SC - ML - 3 Single-walled nanotubes-COOH functionalized Purity > 80 vol% (carbon nanotubes)
> 50 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 5 - 15 µm
Amorphous Carbon Content <5 wt% Price Range 1-10gms($180/gm)11-25gms($160/gm)26-50gms($140/gm) 9. COOH - FUNCTIONALIZED SWCNT [Long Length] -COOH content: 0.5 ~ 3 wt% SSA: 350 - 500 m2/g Conductivity: 102~~10-4 S/cm Metal Content: Nil Content of -OH: < 2 wt% Color: Black Ash: <1>3wt%
Current Carrying Capacity: 1 Billion A/cm2
Tensil Strength: 45 Billion Pa
Temperature stability: 2800 degrees Celcius in vacuum
Thermal conductivity: 2400 ± 400 W/m.K


SC - LL - 1 Single-walled nanotubes-COOH functionalized
Purity > 98 vol% (carbon nanotubes)
> 70 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 15 - 30 µm
Amorphous Carbon Content <2 wt% Price Range 1-10gms($200/gm)11-25gms($180/gm)26-50gms($160/gm) SC - LL - 2 Single-walled nanotubes-COOH functionalized Purity > 90 vol% (carbon nanotubes)
> 65 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 15 - 30 µm
Amorphous Carbon Content <5 wt% Price Range 1-10gms($190/gm)11-25gms($170/gm)26-50gms($150/gm) SC - LL - 3 Single-walled nanotubes-COOH functionalized Purity > 80 vol% (carbon nanotubes)
> 50 vol% (single-walled nanotubes)
Average Diameter 0.7 - 2nm (TEM)
Length 15 - 30 µm
Amorphous Carbon Content <5 wt% Price Range 1-10gms($180/gm)11-25gms($160/gm)26-50gms($140/gm) 10. OH - FUNCTIONALIZED MWCNT [Short Length] SSA: > 300 m2/g
Conductivity: 102~~10-4 S/cm
Metal Content: Nil
Content of -OH: 1 - 6 wt%
Color: Black
Temperature stability: 700° Celcius in Air


MO - SL - 1 Multi-walled nanotubes-OH functionalized
Purity > 90 vol% (carbon nanotubes)
> 70 vol% (single-walled nanotubes)

Average Diameter 4 - 12+ nm (TEM)
Length 3- 10 µm
Amorphous Carbon Content <5 wt% Price Range 1-10gms($160/gm)11-25gms($140/gm)26-50gms($130/gm) MO - SL - 2 Multi-walled nanotubes-OH functionalized Purity > 80 vol% (carbon nanotubes)
> 65 vol% (single-walled nanotubes)

Average Diameter 4 - 12+ nm (TEM)
Length 3- 10 µm
Amorphous Carbon Content <6 wt% Price Range 1-10gms($150/gm)11-25gms($130/gm)26-50gms($120/gm) MO - SL - 3 Multi-walled nanotubes-OH functionalized Purity > 70 vol% (carbon nanotubes)
> 50 vol% (single-walled nanotubes)

Average Diameter 4 - 12+ nm (TEM)
Length 3- 10 µm
Amorphous Carbon Content <6 wt% Price Range 1-10gms($140/gm)11-25gms($120/gm)26-50gms($110/gm) 11. OH - FUNCTIONALIZED MWCNT [Medium Length] SSA: > 300 m2/g
Conductivity: 102~~10-4 S/cm
Metal Content: Nil
Content of -OH: 1 - 6 wt%
Color: Black
Temperature stability: 700° Celcius in Air


MO - ML - 1 Multi-walled nanotubes-OH functionalized
Purity > 90 vol% (carbon nanotubes)
> 70 vol% (single-walled nanotubes)

Average Diameter 4 - 12+ nm (TEM)
Length 5- 15 µm
Amorphous Carbon Content <5 wt% Price Range 1-10gms($160/gm)11-25gms($140/gm)26-50gms($130/gm) MO - ML - 2 Multi-walled nanotubes-OH functionalized Purity > 80 vol% (carbon nanotubes)
> 65 vol% (single-walled nanotubes)
Average Diameter 4 - 12+ nm (TEM)
Length 5- 15 µm
Amorphous Carbon Content <6 wt% Price Range 1-10gms($150/gm)11-25gms($130/gm)26-50gms($120/gm) MO - ML - 3 Multi-walled nanotubes-OH functionalized Purity > 70 vol% (carbon nanotubes)
> 50 vol% (single-walled nanotubes)
Average Diameter 4 - 12+ nm (TEM)
Length 5- 15 µm
Amorphous Carbon Content <6 wt% Price Range 1-10gms($140/gm)11-25gms($120/gm)26-50gms($110/gm) 12. OH - FUNCTIONALIZED MWCNT [Long Length] SSA: > 300 m2/g
Conductivity: 102~~10-4 S/cm
Metal Content: Nil
Content of -OH: 1 - 6 wt%
Color: Black
Temperature stability: 700° Celcius in Air


MO - LL - 1 Multi-walled nanotubes-OH functionalized
Purity > 90 vol% (carbon nanotubes)
> 70 vol% (single-walled nanotubes)
Average Diameter 4 - 12+ nm (TEM)
Length 15- 30 µm
Amorphous Carbon Content <5 wt% Price Range 1-10gms($160/gm)11-25gms($140/gm)26-50gms($130/gm) MO - LL - 2 Multi-walled nanotubes-OH functionalized Purity > 80 vol% (carbon nanotubes)
> 60 vol% (single-walled nanotubes)

Average Diameter 4 - 12+ nm (TEM)
Length 15- 30 µm
Amorphous Carbon Content <6 wt% Price Range 1-10gms($150/gm)11-25gms($130/gm)26-50gms($120/gm) MO - LL - 3 Multi-walled nanotubes-OH functionalized Purity > 70 vol% (carbon nanotubes)
> 50 vol% (single-walled nanotubes)
Average Diameter 4 - 12+ nm (TEM)
Length 15- 30 µm
Amorphous Carbon Content <6 wt% Price Range 1-10gms($140/gm)11-25gms($120/gm)26-50gms($110/gm)

Tuesday, January 6, 2009

NEW THEORY EXPLAINS ELECTRONIC AND THERMAL BEHAVIOR OF NANOTUBES

Recently researchers made an important theoretical breakthrough in the understanding of energy dissipation and thermal breakdown in metallic carbon nanotubes. Their discovery will help move nanotube wires from laboratory to marketplace.We all know about the remarkable electrical and mechanical properties of metallic carbon nanotubes make them promising candidates for interconnects in future nanoscale electronic devices. But, like tiny metal wires, nanotubes grow hotter as electrical current is increased. At some point, a nanotube will burn apart like an element in a blown fuse. So, heat dissipation is a fundamental problem of electronic transport at the nanoscale.

To fully utilize nanotubes as interconnects, CNT must be characterized properly and there by getting their behavior and operating limits.Up to now, no coherent interpretation had been proposed that reconciled heat dissipation and electronic transport, and described thermal effects in metallic carbon nanotubes under electronic stress. Now in this research some theoretical results not only reproduce experimental data for electronic transport, they also explain the odd behavior of thermal breakdown in these nanotubes. For example, in both theory and experiment, the shorter the nanotube, the larger the current that can be carried before thermal breakdown occurs. Also, the longer the nanotube, the faster the rise in temperature as the threshold current for thermal heating is reduced.In nanotubes, heat generated by electrical resistance creates atomic vibrations in the nanostructure, which causes more collisions with the charge carriers. The additional collisions generate more heat and more vibrations, followed by even more collisions in a vicious cycle that ends when the nanotube burns apart, breaking the circuit.Short nanotubes can carry more current before burning apart because they dissipate heat better than longer nanotubes. Although the entire nanotube experiences resistance heating, the electrical contacts at each end act as heat sinks, which in short nanotubes are relatively close to one another, leading to efficient heat removal. This phenomenon also explains why the highest temperature always occurs in the middle of the nanostructure. In another important finding, researchers have revised the common belief that charge carriers go ballistic in short metallic nanotubes having high currents.

Researchers had previously thought that charge carriers traveled from one terminal to the other like a rocket; that is, without experiencing collisions.They have shown that the high current level in short metallic nanotubes is not due to ballistic transport, but to reduced heating effects. Owing to their large concentration, the charge carriers collide efficiently among themselves, which prevent them from going ballistic. Even in short nanostructures, the current level is determined by a balance between the attractive force of the external electric field and the frictional force caused by the nanotube thermal vibrations. The collisions among charge carriers help the energy transfer to the nanotubes which results in heat dissipation.

Monday, December 29, 2008

Harmful Carbon Nanotubes!!!

A recent study revealed that carbo nanotube could be as harmful as asbestos if inhaled in sufficient quantities. The study used established methods to see if specific types of nanotubes have the potential to cause mesothelioma — a cancer of the lung lining that can take 30-40 years to appear following exposure. The results show that long, thin multi-walled carbon nanotubes that look like asbestos fibers, behave like asbestos fibers.

Discovered nearly 20 years ago, carbon nanotubes have been described as the wonder material of the 21st Century. Light as plastic and stronger that steel, they are being developed for use in new drugs, energy-efficient batteries and futuristic electronics. But since their discovery, questions have been raised about whether some of these nanoscale materials may cause harm and undermine a nascent market for all types of carbon nanotubes, including multi- and single-walled carbon nanotubes. Leading forecasting firms say sales of all nanotubes could reach $2 billion annually within the next four to seven years, according to an article in the U.S. publication Chemical & Engineering News.

Andrew Maynard, Chief Science Advisor to the Project on Emerging Nanotechnologies opined that this study is exactly the kind of strategic, highly focused research needed to ensure the safe and responsible development of nanotechnology.

Widespread exposure to asbestos has been described as the worst occupational health disaster in U.S. history and the cost of asbestos-related disease is expected to exceed $200 billion, according to major U.S. think tank RAND Corporation.

The toll of asbestos-related cancer, first noticed in the 1950s and 1960s, is likely to continue for several more decades even though usage reduced rapidly some 25 years ago. While there are reasons to suppose that nanotubes can be used safely, this will depend on appropriate steps being taken to prevent them from being inhaled in the places they are manufactured, used and ultimately disposed of. Such steps should be based on research into exposure and risk prevention, leading to regulation of their use.

Examination revealed the potential for long and short carbon nanotubes, long and short asbestos fibers, and carbon black to cause pathological responses known to be precursors of mesothelioma. Material was injected into the abdominal cavity of mice — a sensitive predictor of long fiber response in the lung lining. This showed that long, thin carbon nanotubes showed the same effects as long, thin asbestos fibers.

This is a wakeup call for nanotechnology in general and carbon nanotubes in particular.

Thursday, September 4, 2008

SHATTERED BONES: ANSWER IS CARBON NANO TUBE

Human bones can be broken in accidents, or they can be disintegrated when ravaged by disease and time. But scientists at the University of California may have a new weapon in the battle against forces that damage the human skeleton. They have found a way to create a stronger and safer frame than the artificial bone scaffolds currently in use.

Carbon Nanotube, incredibly strong molecules just billionths of a meter wide, can function as scaffolds for bone regrowth, according to researchers led by Robert Haddon at the same University.

Human Bone is having two parts. One is organic and another one is inorganic. The organic part is made of collagen, which is the most abundant protein in mammals. The inorganic component is a type of calcium crystal named hydroxyapatite. The collagen forms a sort of natural scaffold over which the calcium crystals organize into bone. The idea in Haddon's research is to use the nanotubes as substitutes for the collagen to promote new bone growth when bones have been broken or worn down.

Tuesday, September 2, 2008

CNT: SUBSTITUTE FOR SILICON

The electrical properties of CNTs are extremely sensitive to defects which can be introduced during the growth, by mechanical strain, or by irradiation with energetic particles such as electrons, heavy ions, alpha-particles, and protons. When highly energetic particles collide, a latchup, electrical interference, charging, sputtering, erosion, and puncture of the target device can occur. Therefore the information on the effects of various types of high energetic irradiation on CNTs and other nanomaterials will be important in developing radiation-robust devices and circuits of nanomaterials under aerospace environment. As a result, degradation of the device performance and lifetime or even a system failure of the underlying electronics may happen. Researchers in South Korea conducted a systematic study of the effects of proton irradiation on the electrical properties of CNT network field effect transistor (FET) devices showing metallic or semiconducting behaviors. The most important outcome of this work is that no significant change in the electrical properties of CNT-based FET was observed, even after high-energy proton beam irradiated directly on the device. This result show that CNT-based devices can be a promising substitute for classical silicon-based devices, which are known to be very fragile against proton radiations.

It has been reported previously that electronic devices became more radiation tolerant when their dimensions are reduced.For example, multi-quantum well or quantum dot devices can be tens or hundreds times more radiation tolerant than conventional bulk devices. It even was shown that quantum dot/CNT-based photovoltaic devices were five orders of magnitude more resistant than conventional bulk solar cells.