REVIEW IN FLUID MECHANICS CE board May 1994 Assuming specific weight of air to be at constant at 12 N/m 3. What is the approximate height of Mount Banahaw if a mercury barometer at the base of the mountain reads 654mm and at the same instant, another barometer at the top of the mountain reads 480mm? Solution: Pressure at the top of the mountain Ptop = whg x hbarometer rdg at the top of the mountain = (9810N/m3 x 13.6)(0.48m) = 64039.68 Pa Pressure at the base of the mountain Pbase = whg x hbarometer rdg at the base = (9810N/m3 x 13.6)(0.654m) = 87254.06 Pa Pbase - Ptop = (wair) (hmountain) 87254.06 Pa - 64039.68 Pa = 12N/m3(hmountain) hm = 1934.53m CE Board November 2000 For the tank shown in the figure, h1=3m and h3=4m. Determine the value of h2. Solution: Note that the pressure at the liquid surface expose to atmosphere is zero. By summing up the pressure heads, we have π2 π1 + 4 − 3 − β2 (0.80) = π€ π€ P1 and P2 are zero, because they are both exposed to atmosphere 0 + 4 − 3 − β2 (0.80) = 0 ππ = π. πππ CE BOARD MAY 1993 In the figure shown, when the funnel is empty, the water surface is at level A and the mercury (s=13.6) shows a deflection of 15cm. Determine the new deflection of mercury when the funnel is filled with water up to level B. Solution: When the water is at level A (Figure A), adding the pressure heads 0 + y – 0.15(13.6) = 0 y=2.04m When the water increases up to level B, the water will push the mercury downward by distance x, as a result the mercury will rise by distance x on the other part of the tube, therefore the new deflection of mercury will be 0.15+2x (refer on Figure B). By summing up the pressure heads, this will lead to 0 + 0.80 + 2.04 + x – x(13.6) – 0.15(13.6) – x(13.6) = 0 x = 0.03m Therefore new deflection = 0.21m or 21cm SAMPLE PROBLEMS 1. A vertical rectangular gate 2m wide and 3m high is submerged in water with its top edge 2.4m below the water surface. Find the total pressure acting on one side of the gate and its location from the water surface. Solution: πΉ = π€βΜ π΄ = 9.81(3.9)(2π₯3) = πππ. πππ²π΅ (answer) π= πΌπ π΄π¦Μ βΜ = π¦Μ = 3.9π πβ3 2(3)3 = = 4.5π4 12 12 4.5 π= = 0.19π 6(3.9) πΌπ = βπ = 3.9 + 0.19 = π. πππ (answer) 2. A rectangular gate 2.4m wide and 3.6mhigh is inclined at 600 with respect to horizontal. It is attached to a hinged support on top of the gate. The water stands 2m above the top of the gate. What force P is required acting horizontally at the bottom of the gate to maintain equilibrium. Solution: b=2.4m h=3.6m A = 2.4(3.6) = 8.64m2 Using the triangle above: π₯ sin 600 = 1.8 π₯ =1.56m βΜ = 1.56π + 2π = 3.56π 3 πΌπ = 3 πβ 2.4(3.6) = = 9.33π4 12 12 = 0.26π Μ β sin 600 = π¦Μ π= πΉ = π€βΜ π΄ = 9.81(3.56)(8.64) = 301.74πΎπ π¦Μ =4.11m πΌπ 9.33 = Μ 8.64(4.11) π΄π¦ By taking summation of moments at hinged: F (0.26+1.8) = P(2)(1.56) 301.74 2.06) = P(3.12) P=199.23KN (answer) 3. A vertical gate 2.6m wide and 4.8m high is subjected to hydrostatic forces on both sides. The gate is supported by hinged on the top of the gate. Water stands 2.2m above the hinged on the right side and 1.2m below the hinged on the left side. A wooden stopper is placed at the bottom of the gate to prevent it from opening. Calculate the stress acting on the wooden stopper if it has a sectional area of 0.01m 2. Solution: A1 = 2.6(4.8) = 12.48m2 βΜ 1 = 2.2 + 2.4 = 4.6π A2 = 2.6(3.6) = 9.36m2 βΜ 2 = 1.8π F1 = (9.81)(4.6)(12.48) F1 = 563.17kN πβ3 2.6(4.8)3 = = 23.96π4 12 12 πΌπ2 = πβ3 2.6(3.6)3 = = 10.11π4 12 12 πΌπ1 23.96 = = 0.42π Μ 1 12.48(4.6) π΄1 π¦ π2 = πΌπ2 10.11 = = 0.60π Μ 2 9.36(1.8) π΄2 π¦ πΌπ1 = π1 = F2 = (9.81)(1.8)(9.36) = 165.28 kN By taking summation of moments at hinged: F1(1.2+1.8+0.60) + Fstopper(4.8)=F2(2.4+0.42) 165.28(3.29) + Fstopper(4.8)=563.17(2.82) Fstopper=206.90 KN Stress on the stopper P = Fstopper / Area of stopper Stress on the stopper P = 206.90KN / 0.01m2 = 20690 KPa 4. The submerged curve gate BC as shown in the figure is a quarter of a circular gate of radius 3.0m. The length of the gate perpendicular to the drawing is 4m. Find the magnitude horizontal and vertical components of the total force acting on the gate and their location from the hinged. Solution: Fh = (9.81KN/m3)( 2m +1.5m)(12m2) = 412.02KN Fv = wV = 9.81KN/m3 [(2m x 3m) + (1/4)(π)(3)2] 4m = 512.81KN For their location from hinged: (distance y and x respectively) y= 1.5 + e πΌπ = πβ3 12 = 4(3)3 12 = 9π4 πΌπ 9 π = π΄π¦Μ = 12(3.5) = 0.21π y = 1.5 + 0.21 = 1.71m By taking summation of moment at the hinged: 412.02 (1.71) = 512.81 (x) x = 1.37m 5. A crest gate BC as shown below is a part of a circle of radius 3.6m and subtended 60 º from the hinged at point D. If the width of the gate is 2.4m, determine the following . a) The magnitude of the horizontal hydrostatic force FH in kN b) The magnitude of the vertical hydrostatic force Fv in kN c) The location of Fh from the hinged in meters d) The location of Fv from the hinged in meters. Solution: Sin 600 = h / 3.6 h = 3.12m Cos 600 = DE / 3.6 DE = 1.8m BE = 3.6 – 1.8 = 1.8m Fh = (9.81KN/m3) (1.56m)(3.12m x 2.4m) = 114.59KN ABCE = ASECTOR BDC - Aβ²CED ABCE = 600 3600 (π)(3.6)2 − 1 2 (3.12)(1.8) = 3.98π2 AACB = AABEC - ABCE AACB = 3.12m (1.8m) – 3.98m2 = 1.64m2 Fv = wV = w (AACB) 2.4m Fv = 9.81KN/m3 (1.64m2) 2.4m Fv = 38.61KN πΌπ = πβ3 2.4(3.12)3 = = 6.07π4 12 12 π= πΌπ 6.07 = = 0.52π Μ (3.12π₯2.4)(1.56) π΄π¦ y = 1.56m – 0.52m y = 1.04m By taking summation of moment at the hinged: Fh (y) = Fv (x) 114.59KN (1.04m) = 38.61KN (x) x = 3.09m