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ME 322: Instrumentation Lecture 33. April 14, 2014 Professor Miles Greiner. Announcements/Reminders. This week: Lab 10 Vibrating Beam Sign up for 1.5-hour Lab 11 periods with your partner in lab Extra-Credit LabVIEW Workshop Friday , April 18, 2014, 2-4 PM, Jot Travis Room 125D
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ME 322: InstrumentationLecture 33 April 14, 2014 Professor Miles Greiner
Announcements/Reminders • This week: Lab 10 Vibrating Beam • Sign up for 1.5-hour Lab 11 periods with your partner in lab • Extra-Credit LabVIEW Workshop • Friday, April 18, 2014, 2-4 PM, Jot Travis Room 125D • Sign-up on WebCampus • If enough interest then we may offer a second session • Noon-2 • Help wanted (see me greiner@unr.edu) • Summer: Help construct a convection heat transfer augmentation experiment • Spring 2015: ME 322r Lab Assistant
Lab 11 Unsteady Speed in a Karman Vortex Street • Nomenclature • U = air speed (instead of V) • VCTA = Constant temperature anemometer voltage • Two steps • Statically calibrate hot film CTA using a Pitot probe • Find frequency, fP with largest URMS downstream from a cylinder of diameter D for a range of air speeds U • Compare to expectations (StD= DfP/U = 0.2-0.21)
Setup myDAQ Variable Speed Blower VCTA Barometer PATM TATM Plexiglas Tube CTA • Same as Lab 6 but add CTA and cylinder, and do not use Venturi tube or Gage Pressure Transducer • Tunnel Air Density DTube Cylinder Static Pitot-Static Probe VC Total PP - + 3 in WC IP
Before Experiment • Construct VI (formula block) • Measure PATM, TATM, and cylinder D • Find m and r for air • Air Viscosity from A.J. Wheeler and A. R. Ganji, Introduction to Engineering Experimentation, 2nd Edition, Pearson Prentice Hall, 2004, p. 430.
Pitot Probe Calibrate CTA using Pitot Probe Hot Film Probe • Remove Cylinder • So air speed is relatively steady • Align hot film and Pitot probes • So both are exposed to same air speed • Careful, hot film probes cost $150 each • Based on physical analysis (last lecture) we expect • For different blower speeds (and outlet covering) measure • VCTA (use myDAQ, average using fS ~ 48,000 Hz, tS ~ 1 sec) • IP (Pitot probe, DMM, “eyeball” average) • In Lab 11 use 8-12 wind speed • including blower off • In Final used fewer if time is an issue Cylinder
Hot Film System Calibration • The fit equation VCTA2 = aU1/2 +b appears to be appropriate for these data. • Using least squares the best values for the dimensional parameters are • a = 2.643 volts2s1/2/m1/2 • b = 4.5742 volts2
Standard Error of the Estimate x x x x VCTA2 x x • Find coefficients of best fit line, a and b • Find Standard Error of the Estimate x x
Measure VCTA to determine and • Invert transfer function • (use this function in VI) • Uncertainty • (68%) • uncertainty in is independent of U • But we want the uncertainty in U, (not uncertainty in ) • Power Product? • But (68%) • (68%) • (68%) • uncertainty in U increases with U
Unsteady Speed Downstream from a Cylinder UA • Enter values of a and b in VI • For each measurement use fS ~ 48,000 Hz, sampling time tT ~ 1 sec • For each blower speed • Remove cylinder to measure average speed approaching cylinder UA • Return cylinder and measure unsteady speed • Determine frequency fP with highest URMS • Eyeball • Uncertainty in fP is larger of • Frequency resolution: ½(1/tT) ~ 1/2 Hz, or • Eyeball range • Repeat for ~5 different blower speeds Hot Film
Fig. 4 Spectral Content in Wake for Highest and Lowest Wind Speed (a) Lowest Speed fp = 751 Hz fp = 2600 Hz (b) Highest Speed • The sampling frequency and period are fS = 48,000 Hz and tT= 1 sec. • The minimum and maximum detectable finite frequencies are 1 and 24,000 Hz. • The frequency resolution is ½ (1/tT) = ½ hz • However, the shape of the peaks are somewhat broad, leading to
Dimensionless Frequency and Uncertainty • UA from LabVIEW VI • fP from LabVIEW VI plot • ½(1/tT) or eyeball uncertainty • Re = UADr/m (power product) • StD = DfP/UA(power product)
Comparison with Expectations • Are the values you get for St within the expected range?
Demo • Construct VI • Formula Block • Convert to Dynamic Data • Perform calculations