Suyun Ham and John S. Popovics
The University of Illinois at Urbana-Champaign
Damage level inspection of Concrete tie using a Fully Contactless Ultrasonic Scans
2014 International Crosstie and Fastening system Symposium
Suyun Ham and John S. Popovics The University of Illinois at - - PowerPoint PPT Presentation
Damage level inspection of Concrete tie using a Fully Contactless Ultrasonic Scans Suyun Ham and John S. Popovics The University of Illinois at Urbana-Champaign 2014 International Crosstie and Fastening system Symposium 2 Pr Presen esenta
The University of Illinois at Urbana-Champaign
2014 International Crosstie and Fastening system Symposium
2 (contactless = noncontact = air-coupled)
<J.R. Edwards>
< Naus et al., 2008>
<Walker et al. 2006>
Development and verification of cost- effective,
<S. Naar> <J.R. Edwards>
Concrete crossties are important components
Zeman,2010
that can result in track geometry problems
hydraulic pressure cracking may contribute to RSD
Zeman,2010
Surface guided wave Contactless MEMS Receiver Contactless electrostatic Sender Air Concrete
Possible height
= 4 ~ 50mm
50mm
0.01 0.02 0.03 0.04 0.05 0.06 70 72.5 75 77.5 80 82.5 85 87.5 90
Amplitude (V)
incident Angle (degree)
Contactless MEMS receiver
Contactless electrostatic Sender
Contact
Electrostatic Transducer PZT Transducer
Contactless Contact
Accelerometer
Contactless
MEMS
Condenser Mic Dynamic Mic
Best
π πA π ππA
Contactless MEMS receiver
Contactless electrostatic Sender
Consistency, cost and size effective
2.2 2.4 2.6 2.8 3 3.2 3.4 x 10
0.5 1 1.5 x 10
Time(sec) Amplitude(V)
+6 mm +4 mm +2 mm 0 mm
Reliable array system! Multi lti MEM EMS S se senso sor a r arra rray
Contactless MEMS receiver
Contactless electrostatic Sender
4 axial Scan
4D scan
Crosshair Laser targeting Contactless capacitance transducer Micro processer Signal process Gyro tilt sensor Contactless sensor bracket Adjustable height Contactless MEMS sensor
Rapid robotic system
It was built by own technique with out purchasing
Key Key fea feature of contactles ture of contactless s sens sensing: ing:
1 2 3 4 5 6 x 10
0.02 0.04 0.06 Amplitude(V) Time(sec) Accelerometer MEMS Sensor Condensor Microphone Dynamic Microphone
1.5 2 2.5 3 3.5 4 4.5 5 x 10
0.01 0.02 0.03 0.04 Amplitude(V) Time(sec) 1st Try with same Accelerometer 2nd Try with same Accelerometer 3rd Try with same Accelerometer
Accelerometer (contact)
2 3 4 x 10
0.005 0.01 Amplitude(V) Time(sec) MEMS 1 at same location MEMS 2 at same location
Key Key fea feature of contactles ture of contactless s sens sensing: ing:
Smoo Smooth th Me Medium dium Extr Extreme emely y Rou
gh
Distance
1 2 3 4 5 6 7 x 10
0.2 0.4 0.6 Amplitude(V) Time(sec)
1 2 3 4 5 6 7 x 10
0.2 0.4 0.6 Amplitude(V) Time(sec) 1 2 3 4 5 6 7 x 10
0.2 0.4 0.6 Amplitude(V) Time(sec)
surface wave behavior
a field testing prototype.
Receiver array Sender
R1 : no damage R2 : middle level of RSD R3 : serious RSD
Fast Scanning!!
2.5 3 3.5 4 4.5 5 5.5 6 6.5 7 7.5 x 10
2 4 6 8 x 10
Time(sec) Amplitude(V)
No Pad
R3 serious level damage
2.5 3 3.5 4 4.5 5 5.5 6 6.5 7 7.5 x 10
2 4 6 8 x 10
Time(sec) Amplitude(V)
No Pad
R2 middle level damage
π2 πz2 πΉ(π¨, π’) β π ππ’ πΉ π¨, π’
D is the ultrasonic diffusivity (through random media), π is the energy dissipation rate, πΉ π¨, π’ is the ultrasonic energy density as a function of time t and propagation distance z πΉ π¨, π’ = π0
1 2 ππΈπ’ π
βπ¨2 4πΈπ’πβππ’
ππ πΉ π¨, π’ + 0.51πππ’ = π· β π¨2 4πΈπ’ β ππ’
(Weaver 1998) (Weaver & Sachse 1995)
Analysis of scatter field ; diffuse wave
(Quiviger et al. 2012)
2.8 3 3.2 3.4 3.6 3.8 4 4.2 x 10
1 2 3 4 x 10
Time(sec) Amplitude(V)
r0 r1 r2
r1 r2 r3
R1 R2 R3
r1 r2 r3
Integrated signal energy analysis
Savr t = 1 ππππ’β
y=1 ππππ’β
Tavr_y t
Statistical analysis for inhomogeneous material Array averaged = Group = position, p1, p2β¦. Total seventy signal of each damage region
2 3 4 x 10
2 4 6 x 10
Time(sec) Amplitude(V)
avrsensor1 avr P1 avr P2 avr P3 avr P4 avr P5 avr P6 avr P7 avr P8 avr P9 avr P10 2 3 4 x 10
2 4 6 x 10
Time(sec) Amplitude(V)
avrsensor2 avr P1 avr P2 avr P3 avr P4 avr P5 avr P6 avr P7 avr P8 avr P9 avr P10 2 3 4 x 10
2 4 6 x 10
Time(sec) Amplitude(V)
avrsensor3 avr P1 avr P2 avr P3 avr P4 avr P5 avr P6 avr P7 avr P8 avr P9 avr P10
R1 : No damage R2 : Middle level R3 : Serious Damage Each one has seven averaged data
2 3 4 x 10
Time(sec) ln(E)2
region =1, position =1 1 2 3 4 5 6 7 8 9 10 2 3 4 x 10
Time(sec) ln(E)2
region =2, position =1 1 2 3 4 5 6 7 8 9 10 2 3 4 x 10
Time(sec) ln(E)2
region =3, position =1 1 2 3 4 5 6 7 8 9 10
R1 : No damage R2 : Middle level R3 : Serious Damage Seven Averaged data
2 3 4 x 10
Time(sec) ln(E)
region =3, position =10
avera average ged d da data ta on
position
1 ha has s 7 si 7 sign gnals als So, So, a B a Box
plot ha has sev seven en array si array signa gnals ls
Area of ln(E)
2 3 4 x 10
Time(sec) ln(E)2
region =3, position =1 1 2 3 4 5 6 7 8 9 10
10 d diff iffere rent t position sition
1 2 3 4 5 6 7 8 9 10
Position area of ln(E)
2 range from =0.002s, to =0.0035s
Area of ln(E) ln(E)
1 2 3 4 5 6 7 8 9 10
Position area of ln(E)2
range from =0.002s, to =0.0035s
1 2 3 4 5 6 7 8 9 10
Position area of ln(E)2
range from =0.002s, to =0.0035s
1 2 3 4 5 6 7 8 9 10
Position area of ln(E)2
range from =0.002s, to =0.0035s
R1 R2 R3
applicable to concrete giving good signal to noise ratio providing many consistent data and thus enabling imaging techniques.
paths, from one measurement set-up, with excellent consistency and SNR which enables statistically relevant data.
RSD damage levels in concrete tie test samples from in-place measurements.
New ultrasonic technique isβ¦
This work is supported by research grants from the ASNT fellowship Award 2012, AAR Tech Scanning program and the National Science Foundation.
By Joshua S. Ham ,2013