by 84-1074663779 » Wed Dec 29, 2004 5:14 pm
Art, it certainly can be confusing until basic operation is understood.
The first thing is that the pressure drop across any orifice increases as the square of the airflow. If it has a certain pressure drop at a certain flow, doubling the flow would cause the pressure drop to increase four times. Tripling the airflow volume causes the pressure to increase nine times. That is the basis of operation of any measurement orifice.
So you have your orifice, and you need a measurement manometer of some sort connected across it to measure pressure differential.
The first thing that needs to be decided is what sort of pressure range is going to be used with that orifice. It could be anything from a couple of inches to tens of inches, it mainly depends on available blower power. Lets say you have decided to operate your flow measurement orifice up to a maximum of 7.5 inches pressure drop, and you know the calibration airflow figure at that pressure.
So full scale flow ( xxx Cfm) can be 100% at 7.5 inches.
Using the square law rule we know that doubling the flow increases pressure four times, so: flow x flow = pressure
We can now mark out a suitable manometer scale going from say 50% flow to 100% flow
50% flow (0.5) 0.5 x 0.5 = 0.25 0.25 of 7.5" is 1.875 inches rise
60% flow (0.6) 0.6 x 0.6 = 0.36 0.36 of 7.5" is 2.700 inches rise
70% flow (0.7) 0.7 x 0.7 = 0.49 0.49 of 7.5" is 3.675 inches rise
100% flow (1.0) 1.0 x 1.0 = 1.0 7.500 inches rise
So we now have a scale that goes from 1.875 inches at 50% flow to 7.5 inches at 100% flow.
This same scale can be used with any sized orifice. If one orifice flows 17 Cfm at 7.5 inches, just read the percentage flow directly off the scale. A much larger orifice might flow 631 Cfm at 7.5 inches, again just read the percentage off the scale and multiply by 631 to get actual Cfm flow.
The problem with this is that the scale length is only 7.5 inches long with a vertical manometer and difficult to read.
The developed air pressure will still raise the water 7.5 inches, but by inclining the manometer it travels further along the scale.
The manometer tube can be any length you want to make it, but as long as the high end is 7.5 inches higher than the well it will work exactly the same.
If you wanted to make the tube 20 inches, 28 inches, or 1000mm, it does not matter. Incidentally, 1000mm is a convenient length and very easy to mark off. It is a lot easier to find 706mm on a steel ruler than 17.93 inches !
Lets suppose you have a manometer scale 1000 mm long and it is marked off in flow increments from say 50% flow at 250mm to 100% flow at 1000mm. That same scale can be used at any desired orifice operating pressure by raising the high end the desired amount.
If you decide to do all your flow measurements at a 100% calibration pressure of fifteen inches of water, just raise the 100% mark on the scale 15 inches above the well height.
The ANGLE of slope is irrelevant, it is only the height of the high end that matters, and you can make the scale length anything that is convenient to construct.
The well is important because as the fluid rises along the manometer tube, it falls in the well. So at zero pressure both fluid levels will be the same. At full pressure the well will always have fallen.
If your manometer rise is say nine inches, and the well falls a quarter inch, the rise may really be nine and a quarter inches, so beware of this error. Fixing it only requires dropping the high end a bit to compensate, or making the well have a larger surface area.
It is all fairly obvious once you have thought it all through. It is all just a bit confusing at the start.
If your test pressure is 28 inches, and your flow manometer operates at 7.5 inches, your blower must provide sufficient air to operate at the combined pressure drop of 35.5 inches. This might be a tall order. It is why lower pressures and sloping manometers are used.
If you have a mighty blower that can operate at 60 inches or more pressure, the flow manometer can be mounted vertical, it does not have to slope.