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This page was prepared by ECE undergraduate student Sumit Dutta.



SWNTDiamondGraphite
Diamond (top left), graphite (bottom left), & nanotube (right) structural comparison.
Carbon nanotubes are hollow cylinders of carbon atoms arranged in a honeycomb pattern. The diameter of typical nanotubes is just a few nanometers across, about ten thousand times thinner than a human hair. Carbon with different atomic arrangements also makes up diamond (the best heat conductor known to man) and the graphite of No. 2 pencils. The thermal properties of single-wall carbon nanotubes (SWNTs) are also thought to be outstanding, while the thin tubular whiskers are much more flexible than diamond.

At the same time, SWNTs can be electrically conducting, almost 100 times greater than copper. Hence, a great deal of interest exists in these nanomaterials, both for their electrical and thermal properties.

Thermal Conductance of an Individual Single-Wall Carbon Nanotube above Room Temperature



Matchstick (left) & possible nanotube heat sink (right).
Matchstick (left) & possible nanotube heat sink (right).
In this paper, the thermal properties of SWNTs are extracted from electrical measurements. A nanoscale form of Ohm's law relates the measured voltage to the resistance, accounting for the temperature along the SWNT. The thermal conductivity is extracted from room temperature to nearly the burning point of SWNTs (~600 C). The thermal conductivity of SWNTs is found to be maximum near room temperature, but to decrease above it as nearly 1/T. Combined with other experimenters' results, the data yields a simple model equation for the expected thermal conductivity at a given temperature and nanotube length. This study of SWNT thermal conductivities above room temperature shows that SWNTs have indeed thermal properties similar to diamonds, but are more flexible and less expensive. SWNTs could be used as advanced thermal nanomaterials, heat sinks, or heat pipes that direct heat around corners.

Further reading:



Electrical and Thermal Transport in Metallic Single-Wall Carbon Nanotubes on Insulating Substrates



Carbon nanotube as a wire interconnect.
Nanotube as a wire interconnect between two electrodes.
Though carbon nanotubes conduct heat and electricity, their length and shape determine how well they perform when placed on insulating substrates, as a base layer for electronic circuits. This study simulates nanotubes' electrical and thermal transport properties, pointing to where SWNT performance is optimal. Carbon nanotubes vibrate due to heating, similar to how violin strings oscillate when plucked. At higher voltages, carbon nanotubes' self-heating changes their thermal conductivity as well. These factors become more important at room temperature and above. The voltage at which SWNTs break down is proportional to the SWNT length, as temperature increases with voltage. Better electrical transport implies improvement in energy efficiency in practically all everyday electronics. SWNTs efficiently carry electricity when they have small voltages across them, as this also maximizes heat transport.

Further reading:



Thickness and Stoichiometry Dependence of the Thermal Conductivity of GeSbTe Films



Flash and phase change memory setup.
Comparison of how a bit of information is stored in flash in electrons and in PCM in the GeSbTe film.
Phase change memory (PCM) is a way to store information without keeping it powered up all the time. It is potentially smaller than currently used technologies, such as the flash memory used in USB flash drives, iPods, and cell phones. The primary compound used for PCM is a film of germanium, antimony, and tellurium (GeSbTe, or GST) that can change between a crystallized phase at warmer temperatures and amorphous phase at colder temperatures. These films come in varying thicknesses and have varying proportions of Ge, Sb, and Te (stoichiometric variations). The energy needed to change the memory state, or phase, in PCM is determined by thermal conductivity, which this experiment measures for different thickness and stoichiometry. Rewritable disks such as DVD-RW use PCM. Film thickness primarily determines the quickness of phase change, while stoichiometry gives a unique set of phase change temperatures. These properties can be manipulated to suit different environments, whether they be inside a hot computer or onboard a satellite.

Further reading:



Monte Carlo Simulation of Joule Heating in Bulk and Strained Silicon



Transverse Acoustic WaveLongitudinal Acoustic Wave
Demonstration of transverse (top) and longitudinal (bottom) heat radiation waves in a silicon substrate (Courtesy: Université Laval).
Silicon, a common substrate on which circuits are built, undergoes heat generation when charge flows in the circuit. A comprehensive electrothermal analysis of silicon is essential to determine how circuit components may be affected. Nanoscale electronics offer compact solutions to memory and processor size woes, but many nanoscale devices are sensitive to thermal changes in the substrate. Traditional methods of estimating heating in silicon ignore the variety of atomic vibrations. These vibrations are called phonons. The Monte Carlo simulation method handles a variety of electric fields and treats for different phonon scattering. A key forte of the Monte Carlo technique is the distinction between vibration types. Longitudinal waves are similar to those found in earthquakes or sound. On the other hand, transverse waves are perpendicular to the direction of motion, like a vibrating violin string. Two types of silicon were studied: strained silicon and the more resistive bulk silicon. Strained silicon involves extra preparation as silicon atoms are more widely spaced, but conductivity improves. Comparisons were made between phonon energies categorized by vibration type. This type of simulation can be repeated with other substrates like germanium.

Further reading:



Various Pop Lab Press Articles


This page was prepared by ECE undergraduate student Sumit Dutta.