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ME 322: Instrumentation Lecture 15 February 22, 2016 Professor Miles Greiner Relating speed and flowrate, Lab 6 equipment, Presso flow coefficient, linear sum uncertainty

ME 322: Instrumentation Lecture 15

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ME 322: Instrumentation Lecture 15. February 27, 2012 Professor Miles Greiner. Announcements/Reminders. HW 6 due Friday No lab this week Career Fair, Thursday , February 27, 2014 Internships Prepare for permanent employment next year www.unr.edu/engineering/careerfair. - PowerPoint PPT Presentation

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Page 1: ME 322: Instrumentation Lecture 15

ME 322: InstrumentationLecture 15

February 22, 2016Professor Miles Greiner

Relating speed and flowrate, Lab 6 equipment, Presso flow coefficient, linear sum uncertainty

Page 2: ME 322: Instrumentation Lecture 15

Announcements/Reminders

• HW 6 due Friday• Lab today (Lab 5) but not the rest of this week

Page 3: ME 322: Instrumentation Lecture 15

Regional Science Olympiad• Tests middle and high school teams on various science

topics and engineering abilities• Will be held 8 am to 4 pm Saturday, March 5th 2016

– On campus: SEM, PE and DMS• ME 322 students who participate in observing and judging

the events for at least two hours (as reported) will earn 1% extra credit.

• To sign up, contact Rebecca Fisher, [email protected], (775) 682-7741 – by Wednesday, February 24

• Details– You cannot get extra-credit in two courses for the same work. – If you sign-up but don’t show-up you will loose 1%!

Page 4: ME 322: Instrumentation Lecture 15

Pipe Speed and Volume Flow Rate

• Centerline speed increases in the entrance region– Even though mass (and volume) flow rate is constant

• In fully-developed flow, speed profile V(r) is– Parabolic in laminar flow (Re <~2000), and develops slowly– Flatter in Turbulent flow (Re > 104), and develops rapidly

Page 5: ME 322: Instrumentation Lecture 15

Speed and Flow Rate Consistency

• Does the centerline speed increase with flow rate? Yes or No?

• Is there a unique centerline speed for every volume flow rate and every location? Yes or No?

• What does this “relationship” dependent on?• For a given volume flow rate, what is the range

of centerline speeds in which we expect to be?

Page 6: ME 322: Instrumentation Lecture 15

Possible Centerline Speeds• At the pipe entrance and for fully-developed turbulent flow,

the velocity profile is relatively flat compared to fully-developed laminar flow–

• For fully-developed laminar flow, we expect the velocity profile to be parabolic– where

• is the pipe inner radius, and • is the centerline velocity (for a parabolic profile).

– Relationship between speed and volume flow rate

• In HW show that

• It’s reasonable to expect () < < ()• In Lab 6 measure and in a small wind tunnel

Page 7: ME 322: Instrumentation Lecture 15

Lab 6 Air Volume Flow Rate and Centerline Speed in a Wind Tunnel

• Plexiglas Tube and Schedule-40 Pipe have different diameters• We control flow rate using a variable-speed blower

– Also cover blower exit for very low speeds• For a range of flow rates, measure

– Volume flow rate using a Presso Venturi Tube (in pipe) – Centerline speed using a Pitot-Static Tube (in Plexiglas tube)

• For both measure pressures difference using calibrated transmitters/digital multimeters

• Both and increase with blower flow rate– Check to see if < <

Page 8: ME 322: Instrumentation Lecture 15

Venturi Tube

• Inverted transfer function: – Need , (throat), – These are all characteristics of the venture tube.

• But is based on knowing d and D.

• Presso Formulation: – = = – : Given by manufacturer – Only need D (pipe) and KPresso (not ~1, but don’t need )

Page 9: ME 322: Instrumentation Lecture 15

In Lab 6 use a Presso Venturi Tube

• In Lab 6 use 2-inch schedule 40 Pipe, ID = 2.067 inch– Presso Data Sheet – Page 10, Venturi # 38

• http://wolfweb.unr.edu/homepage/greiner/teaching/MECH322Instrumentation/Labs/Lab%2006%20Fluid%20Flow/Lab%20Index.htm

• = 0.3810 ± 2% (b = 0.6652, but don’t need to this)• Valid for 54,000 < < 137,000 (ReD or Red?)

• – Easier to use than

Page 10: ME 322: Instrumentation Lecture 15

How to find and (and uncertainties)?• Pitot-Static Probe– (power product?)

• Presso Venturi Tube– (power product?)

• Both need air-density– (power product?) • RAir = 0.2870 kPa-m3/kg-K

• Need to measure– Pressure differences PP (pitot), PV (volume), and PStat – Air Temperature, T

Page 11: ME 322: Instrumentation Lecture 15

Instrument Schematic

• To measure PATM and TATM – Use hand-held digital-barometer

• Is PStat <, = or > than PATM?– Use 40-in-WC transmitter to find Gage Pressure PG = PATM – PStat (IG)– PStat = PATM - PG

• To measure PP (Pitot)– Use 3-in-WC transmitter (IP)

• To measure PV (Volume)– Use 40-in-WC transmitter (IV)

DTubeDPipe

PP PG

PV Static

Total+ +--IV

IP IG

+-

Variable SpeedBlower Pipe

PlexiglasTube

Pitot-Static Probe VC

Venturi TubeQ

Atm40 in WC

3 in WC 40 in WC

BarometerPATM TATM

Page 12: ME 322: Instrumentation Lecture 15

Inlet Pressure and Temperature

• Fisher Scientific™ Traceable™ Hand-Held Digital Barometer• Barometric pressure, PATM

– Uncertainty: = 5 mbar = 0.5 kPa = 500 Pa (assume 95%?)• Units: 1 bar = 105 Pa; so 1 mbar = 100 Pa = 0.1 kPa

• Atmospheric Temperature, TATM

– Assume: = 1°C (assume 95%?)– T[K] = T[°C] + 273.15– Assume tunnel and atmospheric temperatures are the same

Page 13: ME 322: Instrumentation Lecture 15

Pressure Transmitter Uncertainty• Pressure

• = 998.7 kg/m3, g = 9.81 m/s2

• FS = (3 or 40 inch)

• Manufacturer stated uncertainty: 0.25% Full Scale– (68%?)– For FS = 3 inch WC

• PFS = rWghFS = (998.7 kg/m3)(9.81 m/s2) (3 inch) = 746.6 Pa• wP = 0.0025 PFS = 1.9 Pa

– For FS = 40 inch WC• PFS = rWghFS = (998.7 kg/m3)(9.81 m/s2) (40 inch) = 9954 Pa• wP = 0.0025 PFS = 25 Pa

Page 14: ME 322: Instrumentation Lecture 15

Static Pressure• PStat = PATM – PG – Use for , RAir = 0.2870 kPa-m3/kg-K–Want kPa

• Inputs– PATM • Measure using barometer• = 500 Pa = 0.5 kPa (68%)

– PGAGE • Measure using 40 inch WC gage• = 25 Pa = 0.025 kPa (68%)

Page 15: ME 322: Instrumentation Lecture 15

Static Pressure Uncertainty

• PStat = PATM – PG (power product?) – Need to use general formula for likely uncertainty:

• Square of absolute uncertainty in result is sum of squares of absolute uncertainty in inputs times coefficient.

Page 16: ME 322: Instrumentation Lecture 15

General Expression Likely Error of “Linear Sums”

Page 17: ME 322: Instrumentation Lecture 15

Summary

• Before Experiment• Use hand held barometer to measure– PATM

– TATM • °C

DTubeDPipe

PP PG

PV Static

Total+ +--IV

IP IG

+-

Variable SpeedBlower Pipe

PlexiglasTube

Pitot-Static Probe VC

Venturi TubeQ

Atm40 in WC

3 in WC 40 in WC

BarometerPATM TATM

Page 18: ME 322: Instrumentation Lecture 15

During Experiment• For each blower setting find the value and

uncertainty of the– Static Pressure, PStat = PATM – Pgage (Power product, linear

sum, other?) • Work on Board

– Air density (Power product, linear sum, other?)

– Centerline speed (Power product, linear sum, other?)

– Volume flow rate (PP, LS, other?)

Page 19: ME 322: Instrumentation Lecture 15

Consistency Check

• For eac volume flow rate (show calculations next time)– –

• What area should we use– APipe or ATube ?

Page 20: ME 322: Instrumentation Lecture 15
Page 21: ME 322: Instrumentation Lecture 15

During Experiment• For each blower setting find the value and

uncertainty of the – Static Pressure, PStat = PATM – Pgage

– Air density

– Centerline speed

– Volume flow rate

Page 22: ME 322: Instrumentation Lecture 15

Wind Tunnel Schematic

DTubeDPipe

PP PG

PV Static

Total+ +--IV

IP IG

+-

Variable SpeedBlower Pipe

PlexiglasTube

Pitot-StaticProbe, VC

VenturiTube, Q

Atm40 in WC

3 in WC 40 in WC