\nThe probes used for taking the measurements can be external (clamp-on) or intrusive.
\nClamp-on probes<\/strong> are designed for temporary measurements but can also be used for permanent measurements because they are safe and easy to install.
\nIntrusive probes<\/strong> can be divided into two categories: fixed probes, which are installed where there is an absence of pressure, and probes that can be removed under pressure.<\/p>\n–> These categories of probes can be used to take mono-chord<\/strong> or multi-chord<\/strong> measurements.<\/p>\n<\/div><\/div><\/div>\nMono-chord system<\/div>
\nA measuring point in the mono-chord system is made up of:<\/p>\n
\n- 1 converter<\/li>\n
- 1 chord = 2 probes (marked as A and B on the diagram)<\/li>\n<\/ul>\n
\n\n\n\u00a0<\/td>\n | <\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n A and B probes<\/strong> are both transmitters<\/strong> and receivers<\/strong>. They alternately<\/strong> transmit to one other. The acoustic signal that spreads through the fluid is collected by the opposite probe. \nThe Upstream\/Downstream and Downstream\/Upstream propagation times<\/strong> are precisely measured (typically 0.2 ns). \nThe average speed<\/strong> along the acoustic path can be calculated using these times<\/strong> and the geometric position<\/strong> of the probes.<\/p>\n<\/div><\/div><\/div>\nMulti-chord system<\/div> \nMono-chord measurements can be used in the assumption that the velocity profile at the measuring point is symmetrical relative to the axis of the pipe.\u00a0Using multi-chord<\/strong> measurements makes it easier to integrate speed profile irregularities<\/strong>.\u00a0As such, multi-chord measurements<\/strong> can be used on straight lengths that are shorter<\/strong> than those required for mono-chord measurements.<\/p>\n\n\n\n<\/td>\n | <\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n \n<\/div><\/div><\/div>\n Calculation method<\/div> \n<\/p>\n \n\n\n<\/td>\n | <\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n With<\/span>:<\/p>\nTAB<\/sub><\/strong>:\u00a0propagation time of the ultrasonic wave from probe A to probe B \nC<\/strong>: speed of sound \nVUS<\/sub><\/strong>: velocity or\u00a0average speed on the ultrasonic path \nKh<\/strong>:\u00a0hydraulic coefficient \nQ<\/strong>: flow \nD<\/strong>: Axial distance or Daxe<\/sub>\u00a0(projected acoustic path along the pipe axis) \nS<\/strong>: Section<\/p>\n\n<\/div><\/div><\/div>\n \nDiscover our products for full pipes: \nFlow meters for liquids<\/a> & flow meters for gas<\/a>.<\/em><\/span><\/p>\n<\/div>\n","protected":false},"excerpt":{"rendered":"","protected":false},"author":3,"featured_media":0,"parent":5588,"menu_order":10,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"acf":[],"yoast_head":"\nFull pipe flow rate measurement | Ultraflux - flow meters<\/title>\n\n\n\n\n\n\n\n\n\n\n\n\n\t\n | | |