MCG 3330 FLUID MECHANICS I LABORATORY SESSIONS Professor S. Tavoularis Department of Mechanical Engineering University of Ottawa September 2008 © Copyright Stavros Tavoularis, 2008 MCG 3330 FLUID MECHANICS I / Laboratory Instructions / Prof. S. Tavoularis / p. 1 JET IMPACT - MOMENTUM EQUATION 1. Objective The objective of this laboratory session is to measure the force of a water jet impacting on objects and to compare it to an estimate based on the momentum equation. 2. Apparatus and Instrumentation The experiment is performed using a hydraulics apparatus manufactured by TecQuipment Ltd. Water is supplied in closed loop by a pump. The flow rate is determined with the use of a weighing tank and a stopwatch. The water issues vertically upwards into the air, through a nozzle with a diameter of 9.5 mm. Two objects are available: a flat plate and a hemispherical cup. Each object can be mounted on a horizontal lever above the water jet and receive its impact. The force on the object can be determined with the use of weights that can be hanged at different positions on the lever. Notice that the water jet is under atmospheric pressure; then, one may neglect friction to use Bernoulli’s equation, which shows that the water velocity would be approximately constant along its path, which is tangential to the object surface. A force balance on the zeroed lever is performed on the following page. 3. Instructions for the Experiments Additional details for the use of the apparatus and specifications for the experiments to be conducted will be provided by the instructor. a) Study carefully the layout and components of the apparatus and familiarize yourselves with all controls and measuring instrumentation. Identify the measured properties and their units. b) Conduct the Jet Impact experiment: • level the apparatus and set the lever at its balance position • attach the hemispherical cup and centre the jet by adjusting the three screws at the base to produce axisymmetric flow on the cup • adjust the mass flow rate of water and then measure it; start by adding a certain weight and fill the tank until the lever arm lifts off its cradle; at this time, quickly add another weight and measure the time that it takes for the lever to lift from its cradle for a second time; note that the value given on the weights is the actual weight (in lbf) of water added to the tank • measure the force on the cup by properly positioning the weight (see procedure below) • repeat the test for a second flow rate, as specified • replace the cup by the flat plate and repeat the tests c) Prepare a brief report of your measurements and calculations. All results should be presented in clear tables and graphs, when necessary. Solve the momentum equation for both the cup and the plate, and compare these estimates with the measured forces. Discuss any differences, / p. 2 MCG 3330 FLUID MECHANICS I / Laboratory Instructions / Prof. S. Tavoularis explain possible reasons for them, and list the percent differences in a table. Procedure for measuring the impact force First balance the lever without the jet (Figure 1a) by moving the weight left or right. Balance of moments about the pivot point gives LsFs = LfFw Next activate the jet (Figure 2a) and balance the lever once again. Note that, in both cases, the spring has been stretched by exactly the same amount, so that the spring force and the corresponding moment about the pivot point are the same in both cases. A moment balance on the new system yields LsFs = (Lf + ΔX) Fw - LfFj Equating the right-hand sides of the two equations above gives Fj = Fw ΔX/Lf where Fj and Fw are measured in lbf and ΔX, Lf are measured in inches. It is given that Lf = 6 in and Fw = 1.20 lbf. Figure 1 Sketch of the jet impact force measurement apparatus a) without the jet and b) with the jet. MCG 3330 FLUID MECHANICS I / Laboratory Instructions / Prof. S. Tavoularis / p. 3 CHANNEL FLOW - BERNOULLI’S EQUATION 1. Objective The objective of this laboratory session is to measure the static pressure variation in water flow along a converging-diverging channel and to compare it to estimates based on Bernoulli’s equation. 2. Apparatus and Instrumentation The experiment is conducted in a variable cross-section (convergent-divergent) channel system, manufactured by Armfield Engineering Ltd. The water flow is maintained by a pump and its flow rate is measured by timing the discharge. The channel width is 38 mm. Pressure taps, connected to vertical tubes acting as manometers, are located along the upper wall of the channel as follows (x is the axial distance from the inlet plane of the channel). Tap a b c d e f g h x [mm] 25.4 63.5 88.9 114.3 139.7 165.1 190.5 215.9 Tap i j k l m n o x [mm] 241.3 266.7 292.1 317.5 342.9 368.3 406.4 3. Instructions for the Experiments Additional details for the use of the apparatus and specifications for the experiments to be conducted will be provided by the instructor. a) Study carefully the layout and components of the apparatus and familiarize yourselves with all controls and measuring instrumentation. Identify the measured properties and their units. b) Conduct the Channel Flow experiment: • measure and tabulate the elevation of the top wall of the channel at the locations of the pressure taps; use the flat plate base as a datum • measure and tabulate the corresponding elevations of the bottom wall of the channel • calculate the channel cross sectional areas at the locations of the taps • adjust the flow rate of water and then measure it; start by adding a certain weight and fill the tank until the lever arm lifts off its cradle; at this time, quickly add another weight and measure the time that it takes for the lever to lift from its cradle for a second time; note that the value given on the weights is the actual weight (in lbf) of water added to the tank / p. 4 MCG 3330 FLUID MECHANICS I / Laboratory Instructions / Prof. S. Tavoularis • estimate the average flow velocity and the dynamic pressure at the cross-section of each tap • measure the static pressure at each tap by measuring the height of the water in the corresponding standpipe • apply Bernoulli’s equation along a streamline coinciding with the top wall of the channel to estimate the static pressure pest at the location of each tap, assuming negligible pressure losses in the channel and uniform velocity across each cross-section; use tap “a” as a reference • compare the measured and estimated values of the static pressure at each tap • compute the sum of the total pressure: pmeas + ½DV 2 + Dgz at the locations of the taps, and plot it vs. x • repeat above steps for a different flow rate c) Prepare a brief report of your measurements and calculations. All results should be presented in clear tables and graphs, when necessary. Discuss your findings, identify any differences between measured and estimated values, explain possible reasons for such differences, and list the % differences in a table. MCG 3330 FLUID MECHANICS I / Laboratory Instructions / Prof. S. Tavoularis / p. 5 PRESSURE LOSSES IN INTERNAL FLOWS 1. Objective The objective of this laboratory session is to measure frictional pressure losses in pipes, valves, fittings and simple flow measuring devices. 2. Apparatus and Instrumentation The tests are conducted in a "Fluid Friction Apparatus", manufactured by Armfield Engineering Limited. The geometric specifications for the devices contained in this apparatus are listed in Table 1. Water flow is produced in a closed loop system by a pump. The main water line is divided into several branches, the flow rate in each of which is controlled by individual valves. The flow rate can be measured by timing the filling of a measuring tank. The pressure losses in the 6 mm pipe, which is used for laminar flow tests, is measured using a pressurized water manometer. Pressure differences for all other devices are measured with a mercury manometer. 3. Instructions for the Experiments Further explanations for the use of the apparatus and specifications for the experiments to be conducted will be provided by the instructor. Among the required tasks are the following. a) Study carefully the layout and components of the apparatus and familiarize yourselves with all controls and measuring instrumentation. Identify the appropriate taps to be used (see Table 2) and the direction of flow in each of the pipes. Sketch the apparatus. b) Start the pump. Measure the water flow rate using the stopwatch and one of the two tanks with graduated scales at the system outlet. Note that the scales do not measure the absolute volume in the tank, therefore it is necessary to measure a change in water level. Use the smaller or larger tank, depending on the flow rate. For the laminar flow experiment, measure the flow rate from tap #2 using the 500 ml plastic graduated cylinder. c) Measure the friction coefficients for the specified pipes at the specified flow rate(s), according to Table 2. Verify whether the flow between the two pressure taps used each time is fully developed. Use the format of Table 3 to record your measurements and calculations. Compare your results with values available in your fluid mechanics textbook. d) Measure the loss coefficients and the equivalent pipe lengths for the specified fittings and valves, according to Table 2. Use the format of Table 3 to record your measurements and calculations. Compare your results with values available in your fluid mechanics textbook or other sources. e) Prepare a brief report of your measurements and calculations. All results should be presented / p. 6 MCG 3330 FLUID MECHANICS I / Laboratory Instructions / Prof. S. Tavoularis in clear tables and graphs, when necessary. Determine the percent differences between measured and estimated friction and loss coefficients and explain the possible reasons for such differences. Table 1: Geometrical Specifications for the Different Devices Device Specifications Pipes Smooth pipe (topmost) ID: 22 mm Roughened pipe ID: 19 mm; average roughness height: 0.5 mm Smooth pipe ID: 18 mm Smooth pipe ID: 6 mm All pipes have a length of 2.40 m and are equipped with three pressure taps spaced at 1.00 m Fittings Bend (right angle) ID = 28.5 mm; radius = 106 mm; z39 - z36 = 218 mm Elbow (right angle) ID = 28.5 mm; z37 - z38 = 104 mm Elbow (45) ID = 28.5 mm; z28 - z23 = 64 mm Elbow (45) ID = 28.5 mm; z23 - z20 = 56 mm Valves Globe valve pipe ID = 28.5 mm Gate valve pipe ID = 28.5 mm Butterfly valve (from tables, Le/D•20) pipe ID = 28.5 mm Table 2: Measurements to be Conducted Device(s) Flow Rate(s) Manometer 6 mm pipe Maximum and two others Water 22 mm pipe Maximum and two others 90° bend 90° elbow Both 45° elbows The three valves, fully open Maximum Mercury MCG 3330 FLUID MECHANICS I / Laboratory Instructions / Prof. S. Tavoularis / p. 7 Table 3: Measurements and Calculations Manometer Readings Pressure Hg H2O hA hB PA-PB f, K, or Le/D From Textbook Friction Coefficient etc. Measured Tap B # Pressure Drop Tap A # Re Q Volume Time Device Area Flow Rate / Reynolds No.