Application of the continuity and Bernoulli's equations to either of the above setups will result in the following theoretical formula (ideal flow conditions):
Q
ideal = A
2 √ [(2 g ΔP )/γ / (1- (D
2 / D
1 )^4 ) ]
where:
Qideal is the ideal flow rate (m3/s)
A2 is the area of the orifice or nozzle opening at point 2 (m2)
g is the acceleration of gravity (m/s2)
P1 is the pressure at point 1 (upstream) (kN/m2)
P2 is the pressure at point 2 (downstream) (kN/m2)
γ is the specific weight of the flowing fluid (water) (kN/m3)
D1 is the diameter of the pipe (m)
D2 is the diameter of the orifice or nozzle opening (m)
For non-ideal flow conditions (found in the real world), the correction factor "C" may be used. QReal is the product of the above expression and the "C" factor.
Part 1: Experimental Setup
- Choose two obstructions (orifice and nozzle) and measure the diameter of the openings.
- Measure the inside diameter of the pipe for the experiment.
- Place one of the obstructions between the pipes making sure it is in the correct way (as in pictures, orifice and nozzle are in the upstream section of the pipe)
- Connect the ends of the pipe with the bolts. (Three evenly spaced bolts will work, six are better.)
- Connect the Differential Pressure Gage with the high-pressure side on the portion closer to the pump, and the low-pressure side on the open end.
- Tighten the brass fittings on the pressure gauge by HAND only. (Using a wrench can over-tighten them and damage the compression seal.)
- When the water is not running the (raw) pressure reading should be zero (or less than 0.2). If it is not, click on the Pressure Offset Zero button.
- Click on the Start button and the 4 traces will move across the graph area. You will only see one though because they are all 0 before the pump is turned on.
- On the graph below you will see two thin bumpy traces and two thick smooth traces.
- The thick traces are color coded with the numeric displays. The Filtered Pressure and Filtered Flow are green.
- The pressure reading is in inches of water.
- The flow reading is in US gallons per minute.
Part 2: Pump Control
- Turn the water pump on and make sure there are no leaks before proceeding.
- Set the flow control (valve at table top height) for full flow.
- You will want to take 5 sets of readings for flows that are (more or less) equally spaced from full flow to 3 US GPM.
- Note: The stainless steel pumps have two control valves that need to be adjusted for the full range of flows.
- The two valves being the flow control valve (at the table top) and a bypass valve (the smaller ball-valve underneath with the pump).
- The bypass valve diverts some water back into the pump instead of the obstruction meter.
- Use the bypass valve for course adjustments and the flow control valve for fine adjustments.
- For maximum flow through the obstruction meter the bypass valve must be closed (handle is at a right angle to the pipe)
- For minimum flows, it must be partially or fully open. If it is not open enough for low flows, the pump will cycle on and off.
- This will cause turbulence and not provide a smooth flow of water.
Part 3: Data Collection
- Reset the program filters.
- Record the pressure drop across the obstruction and the flow from the program.
- Adjust the valve on the table to change the flow rate. (Remember you want 5 evenly spaced flows from maximum down to 3 US GPM.)
- Repeat until you have values for the five different flow rates. The flow rate values are not so important as having a range of values to graphically solve later.
- Record the values on the datasheet that you printed off before the lab.
- With the pump off, be sure to tilt the pipe to allow the water to drain from it before opening.
- Repeat with the other obstruction.
- Plot flow rate (US GPM) against pressure drop (inches of water) (use log-log scale) for each obstruction.
- Do a power regression (choose "Power" type trendline in Excel) of your data to obtain an empirical formula.
- This should be in the form Q=a(∆P)b, where a and b are the regression constants.
- Compare QReal and QIdeal and calculate the experimental coefficient of discharge for the orifice and nozzle.
- Explain what cavitation is, and why it would be a concern in pumps and turbines that experience changing flows or pressures.
- Would the theoretical and real flow rates be closer with a denser or lighter fluid? Why?