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High Temperature Emissivity Measurement

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Title: High Temperature Emissivity Measurement


1
High Temperature Emissivity Measurement
  • Investigating the emissivity of welded stainless
    steel
  • Greg Angelides Rafael Jaramillo
  • Linda McLaren

2
Presentation Overview
  • Importance of knowing high-temp emissivity
  • Theoretical background
  • Experimental Setup
  • Results
  • Discussion of results and errors
  • Suggestions for future work

3
Emissivity and Welding
  • Ability to control temp. around weld
  • HEF is crucial to weld properties
  • Emissivity figures in heat equations

4
Variable Emissivity
  • Carbonization of metal surface, due to heat of
    welding process changes e
  • Change in metal temperature changes e

We will attempt to make a model which can predict
changes in emissivity due to varying temperature
and surface conditions
5
Carbonization in samples
sample 1
sample 2
sample 3
sample 4
sample 5
6
TheoryStefan-Boltzmann Equation
  • Q es(Tsample4 - Tsurrounding4)
  • Q - heat radiated e - emissivity
  • s - Stefan-Boltzmann constant

7
Experimental Overview
  • In order to calculate e, we design an experiment
    to measure all other variables in the
    Stefan-Boltzmann equation
  • T of sample
  • T of surroundings
  • Q radiated

8
Initial Experiment Cold Temperature Emissivity
  • To test of our theory and equipment, we first
    conducted an experiment around room temperature
  • (samples heated to 40 oC)

9
Experimental Setup
hot plate
sample
IR camera
10
Data Acquisition
  • IR camera image is recorded on VHS and analyzed
    on computer
  • Pixel level is easily converted into emission
    level

Example of infrared image
11
Emittance Measurement Trick
  • IR camera does not measure real Q
  • Gives relative, unitless emission levels
  • We use the following equation to convert emission
    levels to emittance

(target lvl.) (background lvl.)
(reference lvl.) (background lvl.)
e
(reference e)
12
Reference Emittance Value
  • Must calculate a reference emittance value for
    some point on the sample
  • Need the actual temp. of a point, as well as the
    IR cameras indicated temp.
  • IR camera emittance set to unity

eIRs ( Tcamera 4 Tsurrounding4) eactuals
(Tactual4 Tsurrounding4)
desired value
13
Cold Temp Data
14
High Temperature Experiment
  • Must modify experimental setup to accommodate
    temperatures up to 450 oC
  • Data is taken every 50 oC, from 50 oC to
  • 450 oC
  • In addition to testing our five welded samples,
    we will now test a clean, unwelded sample.

15
Experimental Setup
16
Analysis of Results
  • Attempt to fit data to following mathematical
    model

etotal einitial T(temp) C(color)
17
Isolating the Temperature Dependence
etotal einitial C(color) T(temp)
ecold einitial C(color)
etotal
T(temp)

ecold
18
Graphing the Temperature Dependence
19
Isolating the Effect of Weld-Produced Color Bands
etotal einitial T(temp)
C(color) ereference einitial T(temp)
etotal
C(color)
ereference
20
Graphing the Color-Band Dependence
21
Graphing the Color-Band Dependence
22
Using C(color) and T(temp)
  • With accurate graphs of the functions C(color)
    and T(temp), one could calculate the emissivity
    etotal with the following equation

etotal einitial T(temp) C(color)
23
Sources of Error
  • Camera placement
  • Heating of camera condensation on lens
  • Inconsistent surrounding temperature
  • Direct thermocouple measurements insufficient
    contact with samples

24
Sources of Error
  • Further carbonization of samples

before heating
after heating
25
Suggestion for Future Work
  • Create a more uniform environment
  • Isolate camera from heat
  • Improve camera resolution
  • Weld thermocouple leads to samples
  • Account for further carbonization

26
Welding So Hot, Its Cool !!!
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