Title: Vielitzer Stra
1- Vielitzer Straße 43
- 95100 Selb
- GERMANY
- Tel. 0049 9287 8800
- Fax 0049 9287 70488
- Email info_at_linseis.de
Linseis Inc. 20 Washington Road P.O.Box
666 Princeton-Jct. NJ 08550 Tel. (609)
799-6282 Fax (609) 799-7739 Email
info_at_linseis.com
2The Company
- Since 1957 Linseis Corporation delivers
outstanding service, know how and leading
innovative products in the field of thermal
analysis and thermal physical properties. We are
driven by innovation and customer satisfaction.
Customer orientation, innovation, flexibility and
last but not least highest quality are what
Linseis stands for from the very beginning.
Thanks to these fundamentals our company enjoys
an exceptional reputation among the leading
scientific and industrial companies. -
-
- Claus Linseis
- Managing Director
3ASTM E 1461 - 01
- Standard Test Method for Thermal Diffusivity by
the Flash Method - A small, thin disc specimen is subjected to a
high intensity short duration radiant energy
pulse. The energy of the pulse is absorbed on the
front surface of the specimen and the resulting
rear face temperature rise (thermogram) is
recorded. The thermal diffusivity value is
calculated from the specimen thickness and the
time required for the rear face temperature - rise to reach certain percentages of its maximum
value. When the thermal diffusivity of the sample
is to be determined over a temperature range, the
measurement must be repeated at each temperature
of interest.
4Terminology
- 1 Definitions of Terms Specific to This Standard
- 1.1 thermal conductivity, l, of a solid
materialthe time - rate of steady heat flow through unit thickness
of an infinite slab of a homogeneous material in
a direction perpendicular to the surface, induced
by unit temperature difference. The property must
be identified with a specific mean temperature,
since it varies with temperature. - 1.2 thermal diffusivity, a, of a solid
materialthe property given by the thermal
conductivity divided by the product of the
density and heat capacity per unit mass.
5Classification of some Thermophysical Properties
Thermophysical Properties
Thermodynamic Properties
Transport Properties
Thermal Diffusivity LFA
Specific Heat DSC
Thermal Expansion Dilatometer
Thermal Conductivity
Mass Diffusion Coefficient
Electric Resistivity
Kinematic Viscosity
6Thermal Diffusivity Calculation
- Calculation
- First determine the baseline and maximum rise to
give - the temperature difference, ?Tmax Determine the
time required from the initiation of the pulse
for the rear face temperature to reach ?T½ . This
is the half time, t½. Calculate the thermal
diffusivity, a, from the specimen thickness, L
squared and the half time t½, as follows - ? 0.13879 L2/t½
7Determination of Thermal Diffusivity
The quantities measured are temperature (T),
time (t) and voltage change (?V). Note ?V
?T.
Experimental Data
8Measurement Schematic
9Real Measurement vs. Adiabatic
The two graphs show a true measurement vs. an
ideal case of no heat loss (i.e. adiabatic) The
difference between the two must be accounted for
using the correction models contained by the
software.
10Significance and Use
- Significance and Use
-
- Thermal diffusivity is an important property,
required for such purposes as design applications
under transient heat flow conditions,
determination of safe operating temperature,
process control, and quality assurance. - The flash method is used to measure values of
thermal diffusivity, a, of a wide range of solid
materials. It is particularly advantageous
because of simple specimen geometry, small
specimen size requirements, rapidity of
measurement and ease of handling, with a single
apparatus, of materials having a wide range of
thermal diffusivity values over a large
temperature range.
11Thermal Diffusivity
- It is a measure of how well a material can
transmit heat under transient conditions. Since a
material does not just transmit heat, but must be
warmed by it as well, the thermal diffusivity
involves thermal conductivity, specific heat and
density. - Characteristics
- Thermal diffusivity is always a function of
temperature and is directional for anisotropic
materials - Thermal diffusivity may increase or decrease as a
function of temperature, e.g. - - graphite and many ceramics decrease with
temperature - - many metal alloys increase with temperature
- 3. Thermal diffusivity maybe dominated by the
electronic or lattice contributions depending
upon the type of material
12The System II
13The Instrument
Detector Furnace Laser / Xenon pulse source
14The Specifications
- Modular Design
- Different furnaces -125 up to 500C
- RT up to 500X
- RT up to 1250C
- RT up to 1600C
- Different pulse source Xenon or Laser pulse
source (exchangeable) - Different Sensors MCT detector (cryogenic
application) - InSb detector (standard)
- Sample robot round samples
- up to 6 samples 10 mm diameter
- up to 6 samples 12,7 mm diameter
- up to 3 samples 25,4 mm diameter
- square samples
- up to 6 samples 10x10 mm
- liquid samples
- Aluminum / Sapphire / Platinum
15XFA 500 Xenon Flash
Detector
Iris
Furnace
Sample Carrier
Xenon Flash
16LFA 1000 Laser Flash
Detector
Iris
Furnace
Sample Carrier
Laser
17Technical Specifications
18Sample Holders
19Sample Holders II
20Sample Holder For Liquids
Sample container Lid
Sample container Crucible
Liquid
21Sample Preparation
Graphite coating
- Samples are normally coated with a graphite film
before testing. The graphite serves several
purposes. When testing samples that do not
naturally have a high value of emissivity or
absorptivity, the graphite increases the energy
absorbed on the laser side (bottom) and increases
the temperature signal on the detector side (top)
of the sample. Also, a uniform graphite coating
applied to both sample and reference material
helps maintain similar absorptive and emissive
efficiencies among samples, which is needed for
accurate specific heat measurements.
22Application Areas
23Application Areas II
Silver, Copper, Silicon Carbide
24The Software
Software All thermo analytical devices of
LINSEIS are PC controlled, the individual
software modules exclusively run under Microsoft
Windows operating systems. The complete
software consists of 3 modules temperature
control, data acquisition and data evaluation.
The Linseis 32 bit software encounters all
essential features for measurement preparation,
execution and evaluation, just like with other
thermo analytical experiments. Due to our
specialists and application experts LINSEIS was
able to develop this easy understandable and
highly practical software.
25Applications
26TC vs. Sample Thickness
27TC vs. Temperature
28PTFE
29PTFE Applications
- Chemical processing and petrochemical sectors
used for vessel linings, seals, spacers, gaskets,
well-drilling parts and washers, since PTFE is
chemically inert and resistant to corrosion - Laboratory applications Tubing, piping,
containers and vessels due to resistance to
chemicals and the absence of contaminants
attaching to the surface of PTFE products - Electrical industry used as an insulator in the
form of spacers, tubing and the like - Virgin PTFE had been approved by the FDA for use
in the pharmaceutical, beverage, food and
cosmetics industries in the form of conveyor
components, slides, guide rails, along with other
parts used in ovens and other heated systems. - Semiconductor sector used as an insulator in the
production of discrete components such as
capacitors and in the chip manufacturing process.
30Thermal Diffusivity
31Combined Result
32Ceramics
33Thermal Diffusivity
34Combined Results
35Inconel 600
36Thermal Diffusivity
37Thermal Conductivity
38Application Example Graphite (Polycrystalline)
- Graphite is an excellent material for checking
the performance of a Laser/Xenon Flash Thermal
Analyzer. The analyzed material shows a maximum
thermal diffusivity around room temperature. The
specific heat of the material which can be
analyzed by comparative method or by using a DSC
/ High Temperature DSC shows a significant
increase at higher temperatures.
39Application Graphite
40Application Example Aluminum Copper
- The pure metals Copper and Aluminum are used in
this example to demonstrate the performance of
the Linseis Laser Flash device. The measurement
results of the two materials are compared with
literature values. The measured results vary
within 2 of the given literature values this
demonstrates the excellent performance of the
instrument.
41Application Aluminum Copper
42Application Example Isotropic Graphite (AIST)
- This graph shows the Thermal Diffusivity values
measured on a Linseis LFA 1000 compared to the
values measured at AIST Japan. The literature
values of the used Isotropic Graphite from AIST
the measured results on the LFA 1000 vary by less
than 2. (National Institute of Advanced
Industrial Science and Technology, Japan)
43Isotropic Graphite (AIST)
44The Best Method
- Best method for measuring Thermal Diffusivity
?Thermal Conductivity - The flash method is the most accurate and
fastest way of measuring the thermal diffusivity.
It has bee estimated that world-wide over 80 of
the thermal diffusivity measurements are
conducted using the laser flash system
45Advantages of Flash Diffusivity Measurement
- Easy sample preparation because of simple
geometry - Sample sizes are typically 12,7 or 25,4 mm Ø or
10mm square and range from 0.1 to 6 mm thick. - 2. Less material is required because of small
samples Some test methods used to measure
thermal conductivity directly require very large
samples i.e. 30cm x30cm x 5cm in some case - Fast measurement time due to small samples
- With small samples steady state is reached
quickly. Some thermal conductivity methods
require days to complete a set of measurement. - High accuracy
- Depending upon the material accuracies of /-
3-4 or better can be usually achieved - Wide thermal diffusivity / thermal conductivity
range - Thermal diffusivity 0.001 to 10 cm2/s
- Thermal conductivity 0.01 to 2000 W/m-K