01 Pressure Measurement (Water Resources I) Dave Morgan Prepared using Lyx, and the Beamer class in LATEX 2ε , on September 12, 2007 01 Pressure Measurement WRI 1/25 Readings for Pressure Measurement Suggested readings for this topic are from Applied Fluid Mechanics by Mott: Read sections: 3.3 - 3.9 Study Example Problems: 3.1 - 3.13 01 Pressure Measurement WRI 2/25 Absolute and Gauge Pressure Pressure measurements are made relative to some reference pressure, usually atmospheric (a.k.a. ambient) pressure 01 Pressure Measurement WRI 3/25 Absolute and Gauge Pressure Pressure measurements are made relative to some reference pressure, usually atmospheric (a.k.a. ambient) pressure Pressure relative to the atmosphere is called gauge pressure 01 Pressure Measurement WRI 3/25 Absolute and Gauge Pressure Pressure measurements are made relative to some reference pressure, usually atmospheric (a.k.a. ambient) pressure Pressure relative to the atmosphere is called gauge pressure Pressure relative to a perfect vacuum is called absolute pressure 01 Pressure Measurement WRI 3/25 Absolute and Gauge Pressure Pressure measurements are made relative to some reference pressure, usually atmospheric (a.k.a. ambient) pressure Pressure relative to the atmosphere is called gauge pressure Pressure relative to a perfect vacuum is called absolute pressure Absolute, atmospheric and gauge pressures are related by the following expression: abs = patm + pgauge p 01 Pressure Measurement WRI 3/25 Absolute and Gauge Pressure When using a tyre-gauge to check the pressure in a car or a bike tyre, the tyre-gauge reports gauge pressure; this is the amount of pressure in the tyre in excess of the pressure of the atmosphere 01 Pressure Measurement WRI 4/25 Absolute and Gauge Pressure When using a tyre-gauge to check the pressure in a car or a bike tyre, the tyre-gauge reports gauge pressure; this is the amount of pressure in the tyre in excess of the pressure of the atmosphere If a tyre-gauge reports a pressure of 275 kPa and the atmospheric pressure is 101.3 kPa(abs), then the absolute pressure inside the tyre is 376.3 kPa 01 Pressure Measurement WRI 4/25 Absolute and Gauge Pressure When using a tyre-gauge to check the pressure in a car or a bike tyre, the tyre-gauge reports gauge pressure; this is the amount of pressure in the tyre in excess of the pressure of the atmosphere If a tyre-gauge reports a pressure of 275 kPa and the atmospheric pressure is 101.3 kPa(abs), then the absolute pressure inside the tyre is 376.3 kPa Normal pressures near the earth's surface are in the range of 95 kPa(abs) to 105 kPa(abs); the average at sea-level is about 101.3 kPa Atmospheric pressure changes with the weather; at 10:00 pm on Tuesday 28th August, 2007, atmospheric pressure at Calgary International Airport was reported by Environment Canada to be 102.4 kPa 01 Pressure Measurement WRI 4/25 Pressure and Elevation Pressure decreases with increased elevation in the atmosphere; the atmospheric pressure in Quito (2850 m above sea-level) is (usually) less than than the atmospheric pressure in Death Valley (86 m below sea-level). Pressure usually decreases about 3.4 kPa for every increase in elevation of 300 m. 01 Pressure Measurement WRI 5/25 Pressure and Elevation Pressure decreases with increased elevation in the atmosphere; the atmospheric pressure in Quito (2850 m above sea-level) is (usually) less than than the atmospheric pressure in Death Valley (86 m below sea-level). Pressure usually decreases about 3.4 kPa for every increase in elevation of 300 m. Weather stations do not normally display this dierence due to elevation; the stations adjust the pressure for elevation. Thus, 101.3 kPa would be the usual reported pressure in both Quito and Death Valley; this enables us to know something about the weather conditions in a particular location without knowing the elevation and making calculations. 01 Pressure Measurement WRI 5/25 Pressure and Elevation Pressure increases with increased depth in a uid. The pressure at the bottom of the deep end in a swimming pool is noticeably greater than just below the surface. 01 Pressure Measurement WRI 6/25 Pressure and Elevation Pressure increases with increased depth in a uid. The pressure at the bottom of the deep end in a swimming pool is noticeably greater than just below the surface. In uid mechanics, elevation refers to the vertical distance from some reference point to a point of interest (Death Valley is 86 m below sea-level). Elevation is usually denoted by z. A dierence in elevation between two points is usually denoted by h. 01 Pressure Measurement WRI 6/25 Pressure and Elevation The change in pressure in a homogeneous liquid at rest due to change in elevation is given by: ∆p = γ h where ∆p = change in pressure γ = specic weight of liquid h = change in elevation 01 Pressure Measurement WRI 7/25 Pressure and Elevation The change in pressure in a homogeneous liquid at rest due to change in elevation is given by: ∆p = γ h where ∆p = change in pressure γ = specic weight of liquid h = change in elevation Note: 1 2 This equation does not apply to gases Points at the same elevation (same horizontal level) have the same pressure (see Pascal's Paradox) 01 Pressure Measurement WRI 7/25 ∆p = γ · h Derivation Derivation: Consider a vertical cylinder of liquid within a body of liquid. Let the cylinder have height h and cross-sectional area A A h 01 Pressure Measurement WRI 8/25 ∆p = γ · h p1 Derivation p1 A h Derivation: Consider a vertical cylinder of liquid within a body of liquid. Let the cylinder have height h and cross-sectional area A The pressure, p1 , on the top surface of the cylinder is uniform since the surface is horizontal 01 Pressure Measurement WRI 8/25 ∆p = γ · h Derivation p1 A A h Derivation: Consider a vertical cylinder of liquid within a body of liquid. Let the cylinder have height h and cross-sectional area A The pressure, p1 , on the top surface of the cylinder is uniform since the surface is horizontal The force exerted on the top surface is Fdown = p1 A 01 Pressure Measurement WRI 8/25 ∆p = γ · h Derivation p1 A A h p2 p2 Derivation: Consider a vertical cylinder of liquid within a body of liquid. Let the cylinder have height h and cross-sectional area A The pressure, p1 , on the top surface of the cylinder is uniform since the surface is horizontal The force exerted on the top surface is Fdown = p1 A Similarly the pressure, p2 , on the bottom surface of the cylinder is uniform... 01 Pressure Measurement WRI 8/25 ∆p = γ · h Derivation p1 A A h p2 A Derivation: Consider a vertical cylinder of liquid within a body of liquid. Let the cylinder have height h and cross-sectional area A The pressure, p1 , on the top surface of the cylinder is uniform since the surface is horizontal The force exerted on the top surface is Fdown = p1 A Similarly the pressure, p2 , on the bottom surface of the cylinder is uniform... ...and Fup = p2 A 01 Pressure Measurement WRI 8/25 ∆p = γ · h Derivation p1 A W Derivation: The other force to be considered is the weight, W , of the cylinder A h p2 A 01 Pressure Measurement WRI 9/25 ∆p = γ · h Derivation p1 A V Derivation: The other force to be considered is the weight, W , of the cylinder Express W as W = γ · V A h p2 A 01 Pressure Measurement WRI 9/25 ∆p = γ · h Derivation p1 A V Derivation: The other force to be considered is the weight, W , of the cylinder Express W as W = γ · V The cylinder is in equilibrium so A h ΣFy = p2 A − γ V − p1 A = 0 p2 A 01 Pressure Measurement WRI 9/25 ∆p = γ · h Derivation p1 A V Derivation: The other force to be considered is the weight, W , of the cylinder Express W as W = γ · V The cylinder is in equilibrium so A ΣFy = p2 A − γ V − p1 A = 0 h V = Ah so p2 A p2 A − γ · Ah − p1 A = 0 p2 − γ h − p1 = 0 p2 − p1 = γ h ∆p = γ h 01 Pressure Measurement WRI 9/25 Pascal's Paradox Pascal's Paradox All three vessels contain the same liquid. The pressure at the bottom of each vessel is the same because pressure is due only to the depth of liquid. 01 Pressure Measurement WRI 10/25 Water Tower 01 Pressure Measurement WRI 11/25 Water Tower 01 Pressure Measurement WRI 12/25 Pressure Measurement Example A tank, open to the atmosphere in the centre, contains medium fuel oil. Atmospheric pressure is 102.1 kPa. Calculate the gauge pressure and the absolute pressure for locations A, B, C, D and E. A 950 mm C 300 mm B 1375 mm D 625 mm E 01 Pressure Measurement WRI 13/25 Pressure Measurement (Example) A 950 mm C Solution B: is open to the atmosphere so PB = 0 and PB (abs ) = P(atm) = 102.1 kPa 300 mm Pressure at B B 1375 mm D 625 mm E 01 Pressure Measurement WRI 14/25 Pressure Measurement (Example) Solution Pressure at P A 950 mm C 300 mm B 1375 mm D 625 mm A = = = = = A: B − ∆p 0−γ ·h −(8.89 kN/m3 )(0.30 m) −2.667 kN/m2 −2.67 kPa P E P A(abs ) = Patm + PA(gauge ) = 102.1 kPa − 2.667 kPa = 99.4 kPa 01 Pressure Measurement WRI 15/25 Pressure Measurement (Example) Solution Pressure at C P A 950 mm = = C = 300 mm B = 1375 mm D 625 mm = C: B − ∆p 0−γ ·h −(8.89 kN/m3 )(0.950 m) −8.4455 kN/m2 −8.45 kPa P E P C (abs ) = Patm + PC (gauge ) = 102.1 kPa − 8.4455 kPa = 93.7 kPa 01 Pressure Measurement WRI 16/25 Pressure Measurement (Example) Solution Pressure at P A 950 mm C 300 mm B 1375 mm D 625 mm D = = = = = D: B + ∆p 0+γ ·h (8.89 kN/m3 )(1.375 m) 12.224 kN/m2 12.2 kPa P E P D (abs ) = Patm + PD (gauge ) = 102.1 kPa + 12.224 kPa = 114.0 kPa 01 Pressure Measurement WRI 17/25 Pressure Measurement (Example) Solution Pressure at P A 950 mm E E: = = C = 300 mm B = 1375 mm D 625 mm = B + ∆p 0+γ ·h (8.89 kN/m3 )(2.0 m) 17.78 kN/m2 17.8 kPa P E P E (abs ) = Patm + PD (gauge ) = 102.1 kPa + 17.78 kPa = 120.0 kPa 01 Pressure Measurement WRI 18/25 Manometers A h A manometer is a pressure-measuring instrument It uses the height of a liquid column, h, to measure the pressure dierence between two locations This manometer is open to the atmosphere at one end; it is used to measure the dierence in pressure between A and the atmosphere (that is, it measures gauge pressure) 01 Pressure Measurement WRI 19/25 Manometer Example Example Determine the pressure at A given that the temperature of the water is 25◦ C. A 47 mm 3 Water 105 mm 1 2 Kerosene, sg = 0.823 01 Pressure Measurement WRI 20/25 Manometer Example Solution A P3 = 0 P2 = 47 mm 3 Water 105 mm 1 Kerosene, sg = 0.823 +γ ·h = 0 + (0.823)(9.81 kN/m3 )(0.105 m) = 0.84773 kPa P1 2 P3 = 0.84773 kPa A = P1 − γ · h = 0.84773 kPa − (9.78)(0.152) kPa = −0.63883 kPa PA = −0.639 kPa P 01 Pressure Measurement WRI 21/25 Manometer Example Note There is not much dierence in pressure for a dierence in levels of 0.105 m. For this reason, a gauge uid with a higher specic gravity, such as mercury, is usually used to measure larger pressure dierences. 01 Pressure Measurement WRI 22/25 Manometers A B h The dierential manometer illustrated is used to measure the dierence in pressure between A and B 01 Pressure Measurement WRI 23/25 Dierential Manometer Example Example Determine the pressure dierence between A and B A 105 mm Water 1 90 mm 150 mm 2 B Oil, sg = 0.90 3 Mercury, sg = 13.54 01 Pressure Measurement WRI 24/25 Dierential Manometer Example Solution P1 = = = A 105 mm Water 1 150 mm 2 Mercury, sg = 13.54 90 mm P2 B Oil, 3 sg = 0.90 = = = P3 = B = = ∆p = P A +γ ·h 3 PA + (9.81 kN/m )(0.195 m) PA +1.913 kPa) 3 P1 +(13.54)(9.81 kN/m )(0.15 m) PA +(1.913 + 19.924) kPa PA +21.837 kPa PA +21.837 kPa 3 P3 −(0.90)(9.81 kN/m )(0.240 m) PA +21.837 kPa − 2.119 kPa 19.718 kPa P The dierence in pressure between A and B is 19.7 kPa 01 Pressure Measurement WRI 25/25
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