Direct observation of heat dissipation in individual suspended carbon nanotubes using a two-laser technique
Creators
- 1. Department of Materials Science, University of Southern California, Los Angeles, California 90089 (United States)
- 2. Department of Mechanical Engineering and Center for Nano and Molecular Science and Technology, Texas Materials Institute, University of Texas of Austin, Austin, Texas 78712 (United States)
- 3. Department of Electrical Engineering, University of Southern California, Los Angeles, California 90089 (United States)
- 4. Department of Physics, University of Southern California, Los Angeles, California 90089 (United States)
Description
A two-laser technique is used to investigate heat spreading along individual single walled carbon nanotube (SWCNT) bundles in vacuum and air environments. A 532 nm laser focused on the center of a suspended SWCNT bundle is used as a local heat source, and a 633 nm laser is used to measure the spatial temperature profile along the SWCNT bundle by monitoring the G band downshifts in the Raman spectra. A constant temperature gradient is observed when the SWCNT bundle is irradiated in vacuum, giving direct evidence of diffusive transport of the phonons probed by the Raman laser. In air, however, we observe an exponentially decaying temperature profile with a decay length of about 7 μm, due to heat dissipation from the SWCNT bundle to the surrounding gas molecules. The thermal conductivity of the suspended carbon nanotube (CNT) is determined from its electrical heating temperature profile as measured in vacuum and the nanotube bundle diameter measured via transmission electron microscopy. Based on the exponential decay curves measured in three different CNTs in air, the heat transfer coefficient between the SWCNTs and the surrounding air molecules is found to range from 1.5 x 103 to 7.9 x 104 W/m2 K, which is smaller than the 1 x 105 W/m2 K thermal boundary conductance value calculated using the kinetic theory of gases. This measurement is insensitive to the thermal contact resistance, as no temperature drops occur at the ends of the nanotube. It is also insensitive to errors in the calibration of the G band temperature coefficient. The optical absorption is also obtained from these results and is on the order of 10-5.
Additional details
Identifiers
- DOI
- 10.1063/1.3627236;
Publishing Information
- Journal Title
- Journal of Applied Physics
- Journal Volume
- 110
- Journal Issue
- 4
- Journal Page Range
- p. 044328-044328.5
- ISSN
- 0021-8979
- CODEN
- JAPIAU
INIS
- Country of Publication
- United States
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 43126439
- Subject category
- S77: NANOSCIENCE AND NANOTECHNOLOGY; S75: CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY; S36: MATERIALS SCIENCE;
- Descriptors DEI
- ABSORPTION; AIR; CARBON; COOLING; HEAT TRANSFER; HEATING; LASER RADIATION; NANOTUBES; PHONONS; RAMAN SPECTRA; TEMPERATURE COEFFICIENT; TEMPERATURE GRADIENTS; TEMPERATURE MEASUREMENT; THERMAL CONDUCTIVITY; TRANSMISSION ELECTRON MICROSCOPY; VISIBLE RADIATION
- Descriptors DEC
- ELECTROMAGNETIC RADIATION; ELECTRON MICROSCOPY; ELEMENTS; ENERGY TRANSFER; FLUIDS; GASES; MICROSCOPY; NANOSTRUCTURES; NONMETALS; PHYSICAL PROPERTIES; QUASI PARTICLES; RADIATIONS; REACTIVITY COEFFICIENTS; SORPTION; SPECTRA; THERMODYNAMIC PROPERTIES
Optional Information
- Notes
- (c) 2011 American Institute of Physics