Non-destructive thickness measurement systems and methods
View Patent ↗The present invention generally relates to improved non-destructive thickness measurement systems and methods. Embodiments of the present invention utilize quarter wave resonant frequency to measure the thickness of high-temperature pipe walls. In one embodiment, an improved non-destructive thickness measurement system is provided that utilizes Gaussian white noise to produce maximum mechanical resonance in the pipe wall and laser vibrometers to detect the pipe wall's maximum displacement.
1. A system for measuring thickness of an object having an outer surface comprising:
a vibration application mechanism configured to apply a vibration to the object wherein the vibration comprises white noise having a predetermined frequency range that is less than the entire white noise spectrum;
a vibration monitoring device configured to gather displacement data for a discrete location on the outer surface of the object; and
a data processing system configured to determine a resonant frequency of the object based at least in part on the displacement data gathered by the vibration monitoring device and to calculate the thickness of the object at the discrete location based at least in part on the resonant frequency;
wherein the data processing system is further configured to calculate the wave number (“n”) by solving the equation:
n
=
2
(
d
ref
*
f
ref
V
ref
+
1
4
)
where d ref is a known thickness of a reference object, f ref is a resonant frequency of the reference object, and V ref is a velocity of a wave through the reference object, wherein the object and the reference object comprise the same material; and
calculate the thickness of the object by solving the equation:
d
=
(
2
n
-
1
)
V
4
f
where V is equal to V ref and f is equal to f ref .
2. The system of claim 1 further comprising a couplant to facilitate the transfer of vibration from the vibration application mechanism to the object.
3. The system of claim 1 , wherein the white noise has a Gaussian distribution, the Gaussian distribution having frequency values that are independent of each other.
4. The system of claim 1 , further comprising a second vibrometer configured to gather displacement data for a second discrete location on the surface of the object.
5. The system of claim 1 , wherein the vibration application mechanism is a transducer configured to operate at a temperature over 1000 degrees F.
6. The system of claim 1 , wherein the vibration monitoring device is a laser vibrometer.
7. The system of claim 1 , wherein the data processing system is further configured to transform the displacement data into a frequency-domain format using a Fast Fourier Transform (FFT) analysis.
8. The system of claim 1 , wherein the object is a ductile iron pipe.
9. The system of claim 1 , wherein the predetermined frequency range is based at least in part on a range of expected thicknesses of the object and a material of the object.
10. The system of claim 2 , wherein the couplant is molten metal.
11. The system of claim 3 , wherein the vibration application mechanism is further configured to filter the white noise to obtain the Gaussian distribution.
12. The system of claim 7 , wherein the data processing system is further configured to apply a Hanning window to the displacement data before the FFT analysis.
13. The system of claim 9 , wherein a minimum frequency of the predetermined frequency range is based at least in part on a maximum thickness of the object and a maximum frequency of the predetermined frequency range is based at least in part on a minimum thickness of the object.