Noise
Including instrument noise and environmental noise.
Instrument noise:
- Fading Noise
- Laser Noise
Fading noise
Still need some backscatter energy to make data reliable.
Show the higher amplitude level in short distance. The amplitude change to a lower level because of interference of wave.
We could use multiple laser frequencies to mitigate the noise level. sacrifice spatial resolution to significantly reduce the noise.
Laser drifting noise
If the instrument is unstable, there will be laser drifting noise. Independent to the channel.
Could be easily removed using many signal processing method.
DAS Dynamic Range
we could only measure: \(\|\delta \phi\|<\phi\);
\[\|\delta \varepsilon_{xx}\|<\frac{\lambda}{4nL_G\xi}\]Convert to strain rate:
\[\|\dot{\varepsilon}\|=\frac{\|\delta\varepsilon_{xx\|}}{dt}=\dots\]Exceeding the dynamic range
It is different from geophone(maybe it will be similar in intensity-based system, but different in phase-based system)
Sample rate in DAS interrogators
Maximum pulse rate != output sampling rate. Down-sample is OK if we do not lose information.
DAS Spatial Resolution
- Gauge length and pulse.
- Mainly by gauge length because gauge length setting is usually larger.
GL should be much larger than pulse width or there will be some non-linear components in measurement.
文档信息
- 本文作者:Shenyao Jin
- 本文链接:https://shenyaojin.github.io/2022/07/13/das-issues/
- 版权声明:自由转载-非商用-非衍生-保持署名(创意共享3.0许可证)