Published August 15, 2011 | Version v1
Journal article

Direct observation of heat dissipation in individual suspended carbon nanotubes using a two-laser technique

  • 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

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

Optional Information

Notes
(c) 2011 American Institute of Physics