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In-situ laser ultrasonic grain size measurement in superalloy
INCONEL 718Thomas Garcin1, Jean Hubert Schmitt 2, Matthias Militzer 1
1 The University of British Columbia, 2 Ecole Centrale Paris, Laboratoire Mécanique des Sols, Structures, et Matériaux – UMR CNRS 8579
Acknowledgement: Aubert & Duval, member of Eramet Group
.
2nd Workshop on Laser Ultrasonics for Metallurgy
(April 26-27th 2016, Vancouver, Canada)
1
Motivations
• Inconel 718 used in aviation industry
• High strength material obtained by forging process
• Control the microstructure evolution during forging
2
Ten
sile
Str
engt
hs
(Ksi
)
Temperature (°F)
±1 Gpa at 650°C
Goals
• Control the grain growth + dissolution of second phase particles prior to forging
• Starting structure has 20 µm polygonal grain
• + 2 to 3 % of delta phase precipitates
• Real monitoring of grain growth during soaking
3
Thermo-mechanical processing lab
4
Gleeble jaws assembly
5
LUMet laser probe
6
Real time sensing at high temperature
7
Principle of the technique
8
FEM simulation
Up to 50 waveforms measured per second
Broadband ultrasound pulse (2 to 30 MHz)
Analysis software
9
Measured ultrasonic parameters
10
• Time of arrival of echoes -> Velocity 𝑉
• Amplitude of echoes -> Attenuation α(𝑓)
𝑉 =2(𝑒 + 𝜖)
𝜏
α(𝑓) =20
2𝑒log𝐴𝑒𝑐ℎ𝑜(𝑖)
𝐴𝑒𝑐ℎ𝑜(𝑗)
Filtered signal
𝜏
Velocity of ultrasonic wave
11
𝐶𝑖𝑗𝑘𝑙 = 𝑐′𝑖𝑗𝑘𝑙𝑓(𝑜𝑑𝑓)
What can be investigated ? Phase transformationSecond phase/Precipitation Recrystallization
EBSD to Velocity map (mm/µs)
Pro
pag
atio
n (𝑛
)
Velocity Distribution 𝑉 =
𝑃ℎ𝑎𝑠𝑒𝑠
𝐾(𝑜𝑑𝑓)
𝜌Pure Titanium
Rotated Elastic Tensor
Attenuation and scattering by grain
12
V1 V2<V1
Scattering in bi-crystalPro
pag
atio
n (𝑛
)
Scattering depends on ultrasonic wavelength
Scattering depends on grain boundary disorientation and
incidence angle and grain volume
Nicoletti et al. 1994
Large grain size = High attenuation
Other sources of attenuation
13
𝛼(𝑓) = 𝑎 + 𝑏𝑓𝑛 + 𝑐𝑓𝑚
Grain Scattering Diffraction(sample geometry)
Internal Friction/Gain
Thic
knes
s e
TWO ECHOES METHOD
D = 2e D = 4e
How to measure grain size ?
14
𝛼(𝑓) = 𝑎 + 𝑏𝑓𝑛
𝑏 = 𝐶(𝑇) 𝐷𝑖𝑛−1(𝑡) − 𝐷0
𝑛−1(𝑡0 𝑓𝑛
1) Reference sample 𝐷02) ONE ECHO METHOD
Isolate only grain scattering
Measurement precision < 10 %
Frequency dependant grain size parameter
Reference
Current
Reference
Current
High Scattering
Low Scattering
Experiments
15
• Isothermal holding at 1050°C for various time
• Laser ultrasound measurement of mean grain size
• Validation with metallography and modeling
LUMet measurement
Microstructure evolution
16
• Grain growth during isothermal holding
• Second phase is almost fully dissolve after 175 s
Stage of heterogeneous grain growth
17
• Local Nb microsegregations affect the stability of the second phase leading to heterogeneous grain grow
Fraction of large grain
18
• Grains larger than the maximum diameter in initial state
• Conserve grain with aspect ration < 0.3 , i.e. twins
• Fraction = Ratio the threshold area by the total area
• Renormalization
Metallographic analysis
19
• Evaluation of the mean grain size EQAD =
• Maximum 1% largest grain diameter 4 𝐴 𝜋
Attenuation measurement
20
• Single echo method, i.e. with a reference sample
• Measure of the relative change in grain size
Correlation at 1050°C
21
• Evolution of the scattering parameter b with the relative change in mean grain size.
• Direct measurement of the coefficient C*
Linear regression coefficient C* = 0.022
Grain grow tests
22
• Insight into the grain growth behavior.
• Different grain growth stages
• 1) Zener
• 2) Rapid grain growth
• 3) Parabolic
Criteria for abnormal grain growth
23
• Normalization procedure
• Time at the onset of abnormal grain growth
Conclusions
24
• The δ-phase precipitates dissolve in the sample at 1050 C leading to heterogeneous grain growth.
• Ultrasonic attenuation monitored in situ the occurrence of this heterogeneous growth stage
• Direct quantification of the onset and completion of heterogeneous grain growth.