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The Ultrasonic Flow Measuring Principle — Transcript

by Endress+Hauser · 471 words · 43 segments · language en · Watch on YouTube

Full transcript

  1. 0:16The most diverse substances are transported and  distributed in piping systems every single day.
  2. 0:23They can include solvents and chemicals,  vegetable oils in the food sector,
  3. 0:30coolants in primary industry  or petrochemical products.
  4. 0:36The fluids flowing through pipes often have  completely different properties. Therefore,
  5. 0:42different principles are  required for their measurement.
  6. 0:46One principle is flow measurement based on the  differential transit time method using ultrasound.
  7. 0:55The basic physics of this principle can be traced
  8. 0:57back to the English physicist and  Nobel prize winner Lord Raleigh.
  9. 1:02His book "Theory of Sound“ – published
  10. 1:05in 1877 – describes the propagation  of sound waves in solids and gases.
  11. 1:13Here is how this measurement method works.
  12. 1:20Inside the ultrasonic flowmeter, pairs of sensors
  13. 1:24are fitted across from each  other in the measuring tube.
  14. 1:28Each individual sensor can alternately transmit  and receive an ultrasonic signal. Simultaneously,
  15. 1:35the transit times of these signals are measured.
  16. 1:39The ultrasonic signals are  generated with piezoelectrical
  17. 1:44crystals applying a voltage. Conversely,  a piezoelectric crystal creates a voltage,
  18. 1:50when an ultrasonic signal impacts the sensor.
  19. 1:55By increasing the number of sensor pairs  it is possible to accurately detect and
  20. 2:00mathematically compensate for flow profile  distortions over the entire pipe cross section.
  21. 2:07When there is no flow condition, the signal transit  times are the same – upstream and downstream.
  22. 2:14Once the fluid starts to flow in  the measuring tube, the ultrasonic
  23. 2:18signals are accelerated in the direction  of flow and decelerated against the flow.
  24. 2:24As a result, the ultrasonic signals now  have different transit times – less time
  25. 2:30in the direction of flow and  more time against the flow.
  26. 2:34Therefore, the differential  transit time measured by the
  27. 2:37sensors is directly proportional  to the flow velocity in the pipe.
  28. 2:43Together with the known tube cross-section,  the actual flow volume can then be calculated.
  29. 2:50The greater the flow velocity,
  30. 2:52the greater the measured time difference  between the two ultrasonic signals.
  31. 2:59For ultrasonic flow measurement, the sensors don’t  necessarily have to be fitted into the pipe wall.
  32. 3:07With a clamp-on system, for example, the sensors  are fastened directly onto the outside of the
  33. 3:14pipe. They can be retrofitted at  any time without interrupting the process.
  34. 3:21With clamp-on sensors, the ultrasonic signal  is passed directly through the pipe wall and
  35. 3:27into the fluid. The signal continues through the fluid, is reflected on the opposite pipe
  36. 3:33wall and then measured by the second sensor – in  this example with a two-traverse installation.
  37. 3:40The clamp-on design is unique because flow rates  can be measured in very large pipes up to 4
  38. 3:47meters in diameter. This possibility increases the areas of application,
  39. 3:53for example in the water  and hydroelectric industries.
  40. 4:03Flexible mounting, process  safety and cost-effectiveness
  41. 4:07are the distinctive advantages  of ultrasonic flow measurement.
  42. 4:18For all applications, we have the right solution.
  43. 4:23Endress+Hauser – your single-source  supplier for measurement technology!

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