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Pitot tube averaging

Differential Pressure Meters Differential pressure meters or head meters measure the change in pressure across a special flow element. The differential pressure increases with increasing flow rate. The pitot tubes described previously work on this principle. Other examples include orifices [see also Eqs. (6-111) and (8-102), and Fig. 10-14], nozzles (Fig. 10-19), targets, venturis (see also Sec. 8 and Fig. 10-17), and elbow meters. Averaging pitot tubes produce a pressure differential that is based on multiple measuring points across the flow path. [Pg.14]

Because of its low pressure drop capability, the pitot tube is gaining popularity in the form of the averaging pitot tube or Annubar which is a variation of the standard pitot tube. This uses multiple sampling points across a pipe or duct in order to provide a representation of the full flow profile. [Pg.439]

The design of a particular averaging Pitot tube. (Courtesy of Dietrich Standard.)... [Pg.421]

Installation of area-averaging Pitot tube ensembles in rectangular duct for metering the flow rate of gases. (Courtesy of Air Monitor Corp.)... [Pg.422]

Air (gas) flow rate Obviously gas flows are another important parameter for proper dryer operation. Pitot tubes are useful when a system has no permanent gas flow sensors. Averaging pitot tubes work well in permanent installations. The devices work best in straight sections of ductwork which are sometimes difficult to find and make accurate measurement a challenge. [Pg.1430]

When the veloeity pressure is more than 5% of the pressure rise, it should be determined by a pitot-tube traverse of two stations. For each station, the traverse consists of 10 readings at positions representing equal areas of the pipe cross section, as shown in Figure 20-2. The average velocity pressure Py is given by... [Pg.697]

The Prosser was calibrated by measuring the air flows using a laminar flow meter (1% accuracy) for the odorous sample and a pitot tube with a micromanometer for the fan-blown air (3). The pitot pressures were converted to air velocities (4) and hence, from the cross sectional area of the tube, to volumetric flow rates. Since flow near the tube wall was slower than the centre, the tube was traversed by the pitot head and the average value calculated. A rotameter was also tried but it induced a back-pressure of 250 N/m2 and, as the manufacturer states that the maximum permissible back-pressure is 60 N/m for calibration to be accurate, its use was not pursued. [Pg.135]

Measurement of flow can be based on the measurement of velocity in ducts or pipes by using devices such as pitot tubes and hot wire anemometers. The local velocity is measured at various sections of a conduit and then averaged for the area under consideration. [Pg.11]

In these equations pt is the mass density (g. cm.-3) of the fth chemical species, fc is the rate of production of the fth chemical species by chemical reaction (g. cm.-3 sec.-1), and Fi is the external body force per unit mass acting on the ith species. The velocity v is the local mass average velocity (that velocity measured by a Pitot tube), p is the over-all density of the fluid, and U is the local thermodynamic internal energy (per unit mass) of the mixture. The j, are the fluxes of the various chemical species in g. cm.-2 sec.-1 with respect to the local mass average velocity, v. It should be noted that 2j, = 0, 2/c,- = 0, and = p these relations are used in deriving the over-all equation of continuity [Eq. (4)] by adding up the individual equations of continuity given in Eq. (24). [Pg.166]

The principle of operation of a pitot tube is discussed in Section 6.3.1. It should be emphasised that the pitot tube measures the point velocity of a flowing fluid and not the average velocity so that in order to find the average velocity, a traverse across the duct is necessary. Treatment of typical results is illustrated in Problem 6.16. The point velocity is given by u = (2gh) where h is the difference of head expressed in terms of the flowing fluid. [Pg.93]

Determining average linear velocity and air flow through ducts with standard pitot tube equipment, finding sample point, measurement technique, data collection, and calculation procedures. [Pg.197]

Vg = average stack gas velocity (ft/s) fCp = velocity equation constant Cp = Pitot tube probe constant... [Pg.160]


See other pages where Pitot tube averaging is mentioned: [Pg.61]    [Pg.245]    [Pg.81]    [Pg.439]    [Pg.245]    [Pg.185]    [Pg.61]    [Pg.245]    [Pg.81]    [Pg.439]    [Pg.245]    [Pg.185]    [Pg.61]    [Pg.299]    [Pg.248]    [Pg.301]    [Pg.29]    [Pg.299]    [Pg.429]    [Pg.421]    [Pg.213]    [Pg.213]    [Pg.814]    [Pg.155]    [Pg.1897]    [Pg.51]    [Pg.97]    [Pg.230]    [Pg.233]    [Pg.149]    [Pg.160]    [Pg.673]    [Pg.11]    [Pg.1887]    [Pg.474]    [Pg.248]   
See also in sourсe #XX -- [ Pg.439 ]




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