search.noResults

search.searching

saml.title
dataCollection.invalidEmail
note.createNoteMessage

search.noResults

search.searching

orderForm.title

orderForm.productCode
orderForm.description
orderForm.quantity
orderForm.itemPrice
orderForm.price
orderForm.totalPrice
orderForm.deliveryDetails.billingAddress
orderForm.deliveryDetails.deliveryAddress
orderForm.noItems
Flow, level & control Mitigating the effects of


pulsating flow I


t is well known that flowmeters are sensitive to effects such as pulsating flow which can generate errors in flow


measurement. In a pulsating flow system, the velocity profile of the flow undergoes a dramatic change during each cycle of pulsation compared to even flow conditions. So, in electronically sampling flowmeters such as ultrasonic devices, the main source of potential error is the rate of sampling and how it will perceive the real flow passing through it.


How can errors generated by tHe effects of pulsating flow be minimised during sampling? Titan Enterprises offers a range of Ultrasonic small bore flow meters giving high accuracy flow measurement for a wide range of applications. However, as with all flow metering devices, they are sensitive to installation effects that generate variations in the velocity profile of the flow. Where Titan’s flowmeters are installed in a pulsating flow system, the company advises customers to dampen any pulsation as much as possible prior to measurement.


following nyquist tHeorem to increase accuracy of flow measurement The Nyquist Theorem states that in order to adequately reproduce a signal, (in this case the liquid flow), it should be periodically sampled at a rate that is at least twice as fast as its highest frequency component that is being recorded. Therefore, with a pulsating flow scenario the sampling rate of the electronic flow meter needs to be at least double the Hz rate of the pulsations themselves. If the pulsation rate is not taken into account, aliasing of the flow signal will be seen, resulting in erroneous measurement from the flowmeter.


rate is less than twice the rotations of the spokes of the wheel. The visual effect generated is the wheel reversing its direction, even though the cart continues along its original path. With flow measurement, aliasing can be


illustrated graphically. For example, if sampling is much lower than the pulsations, a random scatter of the flow will be observed, seemingly following no pattern at all.


Theoretically, sampling at the same frequency as the pulsation would give a constant but incorrect flow measurement. In practice it is rare to see this and the type of aliasing shown below is more likely, following a cyclic pattern within the peaks and troughs of the pulse.


titan’s ultrasonic flow meters All of Titan’s Ultrasonic flowmeters use time- of-flight acoustic flow measurement. By measuring an acoustic signal upstream and downstream in the liquid measurement tube, the velocity – and thus flow – is accurately measured. For example, the Standard Atrato range will measure to ±one per cent of reading from 2ml/min to 20l/min. Using advanced electronics, Titan’s Atrato and


Metraflow ranges of ultrasonic flowmeters are able to resolve the ultrasonic signals to about 50 picoseconds, with repeat measurements made to ensure stability of measurement. The software samples the flow measured every three milliseconds (ms), but with the downstream processing the reported flow is effectively filtered to about 50ms or 20Hz. So, following the Nyquist theory, Titan’s


Ultrasonic devices can accurately measure pulsating flow that is less than 10Hz. Pulsating above this will likely lead to aliasing, so inline pulse dampening is always recommended for systems using diaphragm, piston or peristaltic pumps for example.


aliasing in flow metering Aliasing can be illustrated in film making with the wagon wheel effect where the camera sampling


52 Titan Enterprises


flowmeters.co.uk/ultrasonic-flow-meter- selection-chart/


June 2021 Instrumentation Monthly


Page 1  |  Page 2  |  Page 3  |  Page 4  |  Page 5  |  Page 6  |  Page 7  |  Page 8  |  Page 9  |  Page 10  |  Page 11  |  Page 12  |  Page 13  |  Page 14  |  Page 15  |  Page 16  |  Page 17  |  Page 18  |  Page 19  |  Page 20  |  Page 21  |  Page 22  |  Page 23  |  Page 24  |  Page 25  |  Page 26  |  Page 27  |  Page 28  |  Page 29  |  Page 30  |  Page 31  |  Page 32  |  Page 33  |  Page 34  |  Page 35  |  Page 36  |  Page 37  |  Page 38  |  Page 39  |  Page 40  |  Page 41  |  Page 42  |  Page 43  |  Page 44  |  Page 45  |  Page 46  |  Page 47  |  Page 48  |  Page 49  |  Page 50  |  Page 51  |  Page 52  |  Page 53  |  Page 54  |  Page 55  |  Page 56  |  Page 57  |  Page 58  |  Page 59  |  Page 60  |  Page 61  |  Page 62  |  Page 63  |  Page 64  |  Page 65  |  Page 66  |  Page 67  |  Page 68  |  Page 69  |  Page 70  |  Page 71  |  Page 72  |  Page 73  |  Page 74  |  Page 75  |  Page 76  |  Page 77  |  Page 78