Thermal conductivity measurement of thin films and bulk materials by 3 omega method
This final year project presents the thermal conductivity characterization of Silicon bulk substrate and several thin films such as Silicon dioxide, amorphous Carbon films and Bismuth telluride using the 3-Omega technique. We firstly study the theoretical concept of the 3-Omega method as well as...
Saved in:
Main Author: | |
---|---|
Other Authors: | |
Format: | Final Year Project |
Language: | English |
Published: |
2011
|
Subjects: | |
Online Access: | http://hdl.handle.net/10356/45353 |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
Institution: | Nanyang Technological University |
Language: | English |
id |
sg-ntu-dr.10356-45353 |
---|---|
record_format |
dspace |
spelling |
sg-ntu-dr.10356-453532023-07-07T15:49:24Z Thermal conductivity measurement of thin films and bulk materials by 3 omega method Tham, Wai Hoe. Tay Beng Kang School of Electrical and Electronic Engineering DRNTU::Engineering::Electrical and electronic engineering::Microelectronics This final year project presents the thermal conductivity characterization of Silicon bulk substrate and several thin films such as Silicon dioxide, amorphous Carbon films and Bismuth telluride using the 3-Omega technique. We firstly study the theoretical concept of the 3-Omega method as well as the heat transport mechanism in nano-scaled dimensions. There are two types of circuits which are widely used for the 3-Omega method namely the Wheatstone bridge setup and Differential Amplifier setup. For our project, we will be concentrating on the differential amplifier setup where the circuit is fabricated and validated its feasibility in measuring the thermal conductivities of the samples above. Results obtained are then compared to the Wheatstone bridge setup results as well as the literature reference values. A gold thin wire is deposited on top of the samples which functions as the heater and thermometer which generates the third harmonic voltage. The temperature coefficient resistance of the thin wire is found to be ranged from 0.0021ppm/K to 0.0030ppm/K. The bulk Silicon thermal conductivity was found to be 147±1Wm/K with thermal diffusivity of81.21 10 6m2 / s . The thermal conductivities of 1μm and 100nm thick Silicon dioxide are 1.356 ±0.1Wm/K and 1.0535±0.1Wm/K. As for 100nm thick Carbon thin films, the thermal conductivity is found to be 0.367±0.001Wm/K. Finally, Bismuth telluride film with thickness of 210nm has a thermal conductivity of 0.1575±0.01Wm/K. Bachelor of Engineering 2011-06-13T02:41:05Z 2011-06-13T02:41:05Z 2011 2011 Final Year Project (FYP) http://hdl.handle.net/10356/45353 en Nanyang Technological University 87 p. application/pdf |
institution |
Nanyang Technological University |
building |
NTU Library |
continent |
Asia |
country |
Singapore Singapore |
content_provider |
NTU Library |
collection |
DR-NTU |
language |
English |
topic |
DRNTU::Engineering::Electrical and electronic engineering::Microelectronics |
spellingShingle |
DRNTU::Engineering::Electrical and electronic engineering::Microelectronics Tham, Wai Hoe. Thermal conductivity measurement of thin films and bulk materials by 3 omega method |
description |
This final year project presents the thermal conductivity characterization of
Silicon bulk substrate and several thin films such as Silicon dioxide, amorphous Carbon
films and Bismuth telluride using the 3-Omega technique. We firstly study the theoretical
concept of the 3-Omega method as well as the heat transport mechanism in nano-scaled
dimensions. There are two types of circuits which are widely used for the 3-Omega
method namely the Wheatstone bridge setup and Differential Amplifier setup. For our
project, we will be concentrating on the differential amplifier setup where the circuit is
fabricated and validated its feasibility in measuring the thermal conductivities of the
samples above. Results obtained are then compared to the Wheatstone bridge setup
results as well as the literature reference values.
A gold thin wire is deposited on top of the samples which functions as the heater
and thermometer which generates the third harmonic voltage. The temperature coefficient
resistance of the thin wire is found to be ranged from 0.0021ppm/K to 0.0030ppm/K. The
bulk Silicon thermal conductivity was found to be 147±1Wm/K with thermal diffusivity
of81.21 10 6m2 / s . The thermal conductivities of 1μm and 100nm thick Silicon dioxide
are 1.356 ±0.1Wm/K and 1.0535±0.1Wm/K. As for 100nm thick Carbon thin films, the
thermal conductivity is found to be 0.367±0.001Wm/K. Finally, Bismuth telluride film
with thickness of 210nm has a thermal conductivity of 0.1575±0.01Wm/K. |
author2 |
Tay Beng Kang |
author_facet |
Tay Beng Kang Tham, Wai Hoe. |
format |
Final Year Project |
author |
Tham, Wai Hoe. |
author_sort |
Tham, Wai Hoe. |
title |
Thermal conductivity measurement of thin films and bulk materials by 3 omega method |
title_short |
Thermal conductivity measurement of thin films and bulk materials by 3 omega method |
title_full |
Thermal conductivity measurement of thin films and bulk materials by 3 omega method |
title_fullStr |
Thermal conductivity measurement of thin films and bulk materials by 3 omega method |
title_full_unstemmed |
Thermal conductivity measurement of thin films and bulk materials by 3 omega method |
title_sort |
thermal conductivity measurement of thin films and bulk materials by 3 omega method |
publishDate |
2011 |
url |
http://hdl.handle.net/10356/45353 |
_version_ |
1772827293254680576 |