Liberating multiple data products from a single DAS data stream

A key motivation for Indeximate is the mantra of “never delete the data”.  We’ve suffered in past careers by observing really interesting data live but not having the disk space to store it, nor the desire to handle the practicality of storing lots of disks nor the easy ability to load and process lots of disks.

A key feature of our Scattersphere is the storage of all recorded DAS data in the cloud – uploaded by our Indeximation step.  This gives us at our fingertips access to months of data – so what can we do with it?

This is where DAS gets exciting – the wide range of vibrations from near DC to infrasonic to ultrasonic is just incredible and hidden within that data is a wealth of data that is never really exploited. For example, if we are focussed on the health of the cable that we are monitoring we will profile this data for all things pertaining to integrity and/or the state of the deployment environment but ignore all the interesting data that might be in the watercolumn or the further seabed.   And in there lies a wealth of further information that could be helping us unlock a better understanding of the oceans.

A wealth of data hides in the DAS data stream

Thinking further, pulling the data to the cloud allows us to consider not just what is happening in the environment locally to the cable but potentially we can get an integrated view across multiple cables and start to build a networked picture of circumstances across both multiple distance scales as well as time scales – ultimately adding to our knowledge of global issues such as the effects of climate change – given enough time and data.

So what have we illustrated so far?   We’ve been slowly publishing a lot of phenomenological observations (take a look at our Micro Learnings web page and our blog) whilst we’ve been busy at work looking after the health of the cable.

So what aspects are practically available from a data reuse aspect?

  • Behaviour of the inter-tidal zone
  • Temperature change
  • Tidal Stream analysis (distinct from tidal analysis) / Ocean currents
  • Lunar tidal relationships
  • Wave Height information
  • Shipping Movement, speed, location, classification
  • Ocean Noise
  • Turbine vibration / piling / noise transmitted through seabed
  • Cetacean Monitoring / Marine Mammal Observations
  • Piling Noise
  • Human Terrestrial Activity on land sections – and this list just gets larger and larger – there’s no end really to what we might consider monitoring.

The growth of offshore wind is a huge opportunity – key of course is the transition to the electrical economy.  In doing so we of course need to ensure that impacts on the environment are closely monitored – the monitoring of our cables provides an opportunity to do just that.

Take a look at the image below snapped from 4C Offshore.

Power cables crossing the North Sea offer huge potential – courtesy 4C Offshore

The export cables, array cables and interconnects are not visible at this resolution but you can imagine – there’s a LOT.  What do you think of when you see this?  A net zero opportunity?  A risk to the environment?  An opportunity for energy security?  A risk to energy security?

We look at and envisage the greatest subsea monitoring network that humans have ever created.   Tens of thousands of km on the seabed – with a sensor every ten metres.   Thinking in those terms allows us to imagine how this network could be used in 10 or 20 years.   Our knowledge of the seabed and the marine environment will jump massively over the paucity of data that we have at the moment.  Both for the benefit of users and those species who live there but also just for the sake of knowledge itself.

So to the examples given – what evidence do we have?

Ocean Currents

Thermal change caused by ocean currents (31km y axis / 3.5 days x axis)

In this first image we are looking out over 3.5 days at a ~31km long stretch of cable in a rocky seabed in ~1km of water.  The red regions correspond to modest local heating and the blue regions local cooling.  Consider the green to be “ambient”.  The temperature changes occur at roughly the same time across the length of the cable (with some local direction changes) so it suggests we are sitting broadside to local current.  We are seeing warmer water flowing over in one direction followed by a period of cooling back to ambient.  This is then repeated. Regularly. 

Tidal Pressure on Cables

We also demonstrated from more predictable lunar tidal flows how we can measure diurnal variations associated with inflow and outflow of tidal regions of the coast.   These have been cleaned of temperature data and what we are looking at here is the strain on the fibre from the ebb and flow of tide!  This is the water pushing against the exposed cable causing strain – in excess of any temperature variation.

Cable tidal pressure (not temperature)
Tidal patterns on shore (head of water forcing the trace)

Human Activity

In this compelling, plaid like image we are looking at a cable on the shore, following a road heading towards the inter tidal zone and then waves coming in from shore.  They are interesting of course, but the real area of interest is the strong red signals.   Here we are looking at individual cars driving down the street which the fibre follows for about 1km.  Looking over long enough we see daily and weekly patterns corresponding to the density of human activity.   These can all be counted and profiled.

Close up view of human activity close to inter-tidal zone

Shipping Activity

In this next image we see the passage of a ship along and crossing the cable as well as wave action, here the red colouring is from the engine noise of the ship, blue again is waves.  These false colour images allow better meaning to be extracted from the data without difficulty.

Boat crossing cable amongst background noise of surface waves and engine noise

Taken further and looking over a long stretch of time and space, one of our signature images below shows the transit and crossing of a vessel over the cable – here there’s a huge wealth of information that can be extracted:  Vessel heading, cable beam pattern, engine noise, propeller noise, the acoustic noise of the ship hitting the swell (those green vertical chevrons).

Our “supernova” here is a false colour image of a ship crossing cable causing wake havoc for many km!

Vibration of nearby structures

Back in January we posted on the extraction of fundamental vibration modes from turbines that we don’t go into but pass by…   We are able to show how we could identify blade passing frequencies, the flexural mode of the tower (nodding) and gearbox / nacelle noise.   Over the long term these could be used to identify tower fatigue (especially during non-producing, feathered periods) and items such as gearbox wear.

Extracting turibine structural health information from vibration stream at a single point

Wave Height

We know that our sensors are sensitive to pressure which makes them ideal for picking up longitudinal sound waves underwater.  It also makes them exceptionally sensitive to changing water heights – i.e. swell and waves. With a small amount of ground truth data we can calibrate the response to wave height and produce an image of wave height variation with time across the whole cable as shown below.

Wave heigh variation from 10km x 30min
and similar data over much longer timescales – 3.5 days and 70km

DAS – Quantitative or Qualitative for subsea cable monitoring?

In our work we often get asked by customers about the two different types of DAS unit commonly found and which they should use. As it’s our tool of choice for extracting info on the condition of cables, we thought it was time to put together some of our thoughts on the topic.

A standard device for testing the quality of an optical fibre installation in subsea cables is an OTDR (Optical Time-Domain Reflectometer). An incoherent pulse of light is sent along a fibre, and the amplitude of the reflected light, when averaged over a number of pulses, tells us if there are bend losses, splices, connectors etc. The time delay between the launch and receive of the reflected signal tells us where the features are. If a coherent laser is used as the light source something different happens and with no time averaging early Distributed Acoustic Sensing (DAS) is born.

The coherency of the laser causes interference between light that is backscattered from different parts of the fibre, and the amplitude of the reflected light from each location is therefore very sensitive to change in the optical path length of the fibre (i.e. strain change or temperature change). The sensitivity to change is somewhat randomised in both magnitude and direction, and this led to changes in the optical architecture of DAS to enable optical phase to be tracked. An intensity only DAS is often referred to as Qualitative DAS (COTDR) and a phase and amplitude tracking DAS is similarly referred to as Quantitative DAS or Phase Coherent DAS.

Both interrogator types make measurements along the fibre giving independent outputs from sections of fibre a few metres long. These length of these sections of fibre is typically called the gauge length. Shorter gauge lengths give better spatial resolution but lower sensitivity to change.

A great source of information on the physical principles of DAS is provided in the recently updated SEAFOM MSP-02 V2.0 “DAS Parameters Definitions and Tests”.

This blog post is concerned about how measurements from these devices on the same cables provide a difference in output – when should each be used?

Qualitative DAS

These units are cheaper and easier to make but do have a high enough sensitivity. Because of these reasons they still have use in monitoring subsea cables. They are excellent devices for pinpointing specific events such as vessels or the arcing caused by a thumper during fault location. It is important to note that this detection approach comes with some major limitations. Firstly, any practically relevant low frequency information is distorted and lost, secondly there is no information on the sense/sign of the stimulus (tension/compression or heating/cooling), and thirdly a noisy environment at low frequencies will tend to scramble higher frequency signals creating harmonics that are not actually present in the signal. This signal distortion is predominantly caused by being unable to track the optical signal from cable strain larger than around 0.3 microns over each gauge. All significant low frequency signals and larger magnitude high frequency signals cause more strain than this, and result in this loss of information.

Single channel spectrogram from Qualitative DAS – under electrical load

This figure is a spectrogram of 30 minutes of data from a section of a UK export cable, 30 km from the shore. It shows the distortion of a pure 3 phase 50Hz electrical signal in a power cable by the action of waves which are occurring at a much lower frequency. This low frequency signal causes the sensitivity of the DAS to flip between positive and negative and leads to side bands in the frequency observed  hence we see distortion in the 50Hz and upper multiples of the 50Hz signal which are not present in the cable.   Care is needed on interpretation.

In qualitative systems, the maximum range is strongly correlated to the gauge length. To get distances longer than around 20 km, the length of the light pulse has to be increased to increase the amount of launched light. This reduces the spatial resolution.

Another issue that strongly affects Qualitative systems is an effect called fading. Fading occurs due to the random nature of the backscattered reflections, occasionally these can add together in such a way to give either a null response to a stimulus or no significant backscattered light. In a quiet environment, these fading effects can render specific channels useless for minutes before environmental conditions change enough to restore sensitivity. In a subsea environment this is generally less of an issue due to the noise of the environment, but it is something to be aware of.

Quantitative DAS

In a quantitative system, the optical backscatter is measured in a different way. Instead of just measuring the amplitude of the backscattered light, the optical phase of the light is measured. There are a number of techniques to achieving this, but all are more complex than simply measuring the amplitude. If the phase is measured, then absolute information about the strain or temperature change can be established Since the fibre effectively becomes a double pass interferometer, a gauge length strain of 0.5 optical wavelengths would give us around one ‘fringe’ (2Pi radians). The wavelength of the light used (typically 1550nm in vacuum)is very close to 1 micron in glass. Straining the fibre also modifies the refractive index of the fibre so in practice we end up with around 10 radians of phase change for each micron of strain. A similar calculation can be done for temperature sensitivity, here we typically get around 1000 radians of phase change for each degree change in temperature (depending on the cable construction and the gauge length). Typical sensitivities of phase measurement are around 0.001 radians (when averaged over a second), so the origin of the extreme sensitivity to change becomes clear.

A quantitative system has a similar sensitivity to a qualitative system (when not faded), but since the changes in phase are tracked, temperature and strain changes can be observed and understood. We can now quantify changes in temperature of the cable, or measure the effect of strain on the fatigue life. Another advantage of tracking phase rather than amplitude is that the distortion of signals is vastly reduced, as discussed above. This creates measurement problems and is best avoided. For example, we may be interested in looking for a 300 Hz grounding signal and need to be sure that the 300 Hz signal that is observed is real, not just a measurement artefact.

Quantitative systems have also had the benefit of much development in recent years, pushing the maximum range to further than possible with older qualitative machines (without compromising spatial resolution) and also reducing the problems of fading. However, as discussed, they are more expensive, and less amenable to reduction in size and cost. However, the absolute nature of the output enables a much greater array of use cases and they remain the recommended route for most applications.

Single channel spectrogram from SAME location with Quantitative unit

This figure shows a spectrogram from the same section of export cable shown the figure above, but this time taken using a phase coherent DAS. The 150 Hz harmonic is very faint, and in this case real. The low frequency noise from waves is seen at less than 1 Hz, as it should be.

Conclusions

In summary, qualitative units are best used as a cost effective solution for when specific detection of acoustic events is required – e.g. for locating a failure with a thumper or TDR.

For any sort of quantification or measurement of long-term changes, a quantitative device should be installed. We would always recommend the use of a quantitative device to our clients for permament monitoring systems, but we are often asked to look at data from older qualitative units and these can still deliver value but insight must be taken with an understanding of the inaccuracies of the data.