fluid_mechanics
62 Chapter 2 ■ Fluid Statics is the weight of the gate and and are the horizontal and vertical reactions of the shaft on the gate. We can now sum moments about the shaft and, therefore, a M c 0 M F R 1y R y c 2 11230 10 3 N210.0866 m2 1.07 10 5 N # m O x O y 0.5 (Ans) y R – y c , m 0.4 0.3 0.2 0.1 (10m, 0.0886 m) 0 0 5 10 15 h c , m 20 25 30 F I G U R E E2.6d E XAMPLE 2.7 Hydrostatic Pressure Force on a Plane Triangular Surface GIVEN An aquarium contains seawater 1g 64.0 lbft 3 2 to a depth of 1 ft as shown in Fig. E2.7a. To repair some damage to one corner of the tank, a triangular section is replaced with a new section as illustrated in Fig. E2.7b. FIND Determine (a) the magnitude of the force of the seawater on this triangular area, and (b) the location of this force. SOLUTION (a) The various distances needed to solve this problem are shown in Fig. E2.7c. Since the surface of interest lies in a vertical plane, y c h c 0.9 ft, and from Eq. 2.18 the magnitude of the force is F R gh c A 164.0 lbft 3 210.9 ft2310.3 ft2 2 24 2.59 lb (Ans) 0.3 ft 1 ft COMMENT Note that this force is independent of the tank length. The result is the same if the tank is 0.25 ft, 25 ft, or 25 miles long. (b) The y coordinate of the center of pressure 1CP2 is found from Eq. 2.19, 0.3 ft 0.9 ft 2.5 ft (b) and from Fig. 2.18 y R I xc y c A y c y x y c Median line y R 1 ft δ A 0.2 ft c c 0.1 ft CP CP x R 0.1 ft 0.15 ft 0.15 ft (c) (d) F I G U R E E2.7b–d F I G U R E E2.7a of Tenecor Tanks, Inc.) (Photograph courtesy
2.9 Pressure Prism 63 so that I xc y R 0.0081 36 ft 4 0.9 ft 10.9 ft210.092 ft 2 2 0.00556 ft 0.9 ft 0.906 ft Similarly, from Eq. 2.20 and from Fig. 2.18 10.3 ft210.3 ft23 36 x R I xyc y c A x c 10.3 ft210.3 ft22 I xyc 72 0.0081 36 ft 4 10.3 ft2 0.0081 72 ft 4 (Ans) so that x R 0.0081 72 ft 4 0 0.00278 ft 10.9 ft210.092 ft 2 2 (Ans) COMMENT Thus, we conclude that the center of pressure is 0.00278 ft to the right of and 0.00556 ft below the centroid of the area. If this point is plotted, we find that it lies on the median line for the area as illustrated in Fig. E2.7d. Since we can think of the total area as consisting of a number of small rectangular strips of area dA 1and the fluid force on each of these small areas acts through its center2, it follows that the resultant of all these parallel forces must lie along the median. 2.9 Pressure Prism An informative and useful graphical interpretation can be made for the force developed by a fluid acting on a plane rectangular area. Consider the pressure distribution along a vertical wall of a tank of constant width b, which contains a liquid having a specific weight g. Since the pressure must vary linearly with depth, we can represent the variation as is shown in Fig. 2.19a, where the pressure is equal to zero at the upper surface and equal to gh at the bottom. It is apparent from this diagram that the average pressure occurs at the depth h2, and therefore the resultant force acting on the rectangular area A bh is F R p av A g a h 2 b A which is the same result as obtained from Eq. 2.18. The pressure distribution shown in Fig. 2.19a applies across the vertical surface so we can draw the three-dimensional representation of the pressure distribution as shown in Fig. 2.19b. The base of this “volume” in pressure-area space is the plane surface of interest, and its altitude at each point is the pressure. This volume is called the pressure prism, and it is clear that the magnitude of the resultant force acting on the rectangular surface is equal to the volume of the pressure prism. Thus, for the prism of Fig. 2.19b the fluid force is The magnitude of the resultant fluid force is equal to the volume of the pressure prism and passes through its centroid. F R volume 1 2 1gh21bh2 g ah 2 b A where bh is the area of the rectangular surface, A. The resultant force must pass through the centroid of the pressure prism. For the volume under consideration the centroid is located along the vertical axis of symmetry of the surface, and at a distance of h3 above the base 1since the centroid of a triangle is located at h3 above its base2. This result can readily be shown to be consistent with that obtained from Eqs. 2.19 and 2.20. h p h h –3 CP F R F R h – 3 (a) γ h γ h (b) b F I G U R E 2.19 Pressure prism for vertical rectangular area.
- Page 36 and 37: 12 Chapter 1 ■ Introduction TABLE
- Page 38 and 39: 14 Chapter 1 ■ Introduction TABLE
- Page 40 and 41: 16 Chapter 1 ■ Introduction Crude
- Page 42 and 43: 18 Chapter 1 ■ Introduction Visco
- Page 44 and 45: 20 Chapter 1 ■ Introduction Kinem
- Page 46 and 47: 22 Chapter 1 ■ Introduction As th
- Page 48 and 49: 24 Chapter 1 ■ Introduction Boili
- Page 50 and 51: 26 Chapter 1 ■ Introduction E XAM
- Page 52 and 53: 28 Chapter 1 ■ Introduction The r
- Page 54 and 55: 30 Chapter 1 ■ Introduction fluid
- Page 56 and 57: 32 Chapter 1 ■ Introduction Secti
- Page 58 and 59: 34 Chapter 1 ■ Introduction avail
- Page 60 and 61: 36 Chapter 1 ■ Introduction compr
- Page 62 and 63: 2 Fluid Statics CHAPTER OPENING PHO
- Page 64 and 65: 40 Chapter 2 ■ Fluid Statics in a
- Page 66 and 67: 42 Chapter 2 ■ Fluid Statics p Fo
- Page 68 and 69: 44 Chapter 2 ■ Fluid Statics the
- Page 70 and 71: 46 Chapter 2 ■ Fluid Statics p 2
- Page 72 and 73: 48 Chapter 2 ■ Fluid Statics wher
- Page 74 and 75: 50 Chapter 2 ■ Fluid Statics F l
- Page 76 and 77: 52 Chapter 2 ■ Fluid Statics E XA
- Page 78 and 79: 54 Chapter 2 ■ Fluid Statics diff
- Page 80 and 81: 56 Chapter 2 ■ Fluid Statics Bour
- Page 82 and 83: 58 Chapter 2 ■ Fluid Statics Free
- Page 84 and 85: 60 Chapter 2 ■ Fluid Statics The
- Page 88 and 89: 64 Chapter 2 ■ Fluid Statics h 1
- Page 90 and 91: 66 Chapter 2 ■ Fluid Statics SOLU
- Page 92 and 93: 68 Chapter 2 ■ Fluid Statics COMM
- Page 94 and 95: 70 Chapter 2 ■ Fluid Statics V2.8
- Page 96 and 97: 72 Chapter 2 ■ Fluid Statics CG
- Page 98 and 99: 74 Chapter 2 ■ Fluid Statics The
- Page 100 and 101: 76 Chapter 2 ■ Fluid Statics z p
- Page 102 and 103: 78 Chapter 2 ■ Fluid Statics dete
- Page 104 and 105: 80 Chapter 2 ■ Fluid Statics Sect
- Page 106 and 107: 82 Chapter 2 ■ Fluid Statics Vapo
- Page 108 and 109: 84 Chapter 2 ■ Fluid Statics heig
- Page 110 and 111: 86 Chapter 2 ■ Fluid Statics h 4
- Page 112 and 113: 88 Chapter 2 ■ Fluid Statics 2.81
- Page 114 and 115: 90 Chapter 2 ■ Fluid Statics h 2
- Page 116 and 117: 92 Chapter 2 ■ Fluid Statics 2.12
- Page 118 and 119: 94 Chapter 3 ■ Elementary Fluid D
- Page 120 and 121: 96 Chapter 3 ■ Elementary Fluid D
- Page 122 and 123: 98 Chapter 3 ■ Elementary Fluid D
- Page 124 and 125: 100 Chapter 3 ■ Elementary Fluid
- Page 126 and 127: 102 Chapter 3 ■ Elementary Fluid
- Page 128 and 129: 104 Chapter 3 ■ Elementary Fluid
- Page 130 and 131: 106 Chapter 3 ■ Elementary Fluid
- Page 132 and 133: 108 Chapter 3 ■ Elementary Fluid
- Page 134 and 135: 110 Chapter 3 ■ Elementary Fluid
62 Chapter 2 ■ Fluid Statics<br />
is the weight of the gate and and are the horizontal and<br />
vertical reactions of the shaft on the gate. We can now sum moments<br />
about the shaft<br />
and, therefore,<br />
a M c 0<br />
M F R 1y R y c 2<br />
11230 10 3 N210.0866 m2<br />
1.07 10 5 N # m<br />
O x O y<br />
0.5<br />
(Ans)<br />
y R – y c , m<br />
0.4<br />
0.3<br />
0.2<br />
0.1<br />
(10m, 0.0886 m)<br />
0<br />
0 5 10 15<br />
h c , m<br />
20 25 30<br />
F I G U R E E2.6d<br />
E XAMPLE 2.7<br />
Hydrostatic Pressure Force on a Plane Triangular Surface<br />
GIVEN An aquarium contains seawater 1g 64.0 lbft 3 2 to a<br />
depth of 1 ft as shown in Fig. E2.7a. To repair some damage to<br />
one corner of the tank, a triangular section is replaced with a new<br />
section as illustrated in Fig. E2.7b.<br />
FIND Determine<br />
(a) the magnitude of the force of the seawater on this triangular<br />
area, and<br />
(b) the location of this force.<br />
SOLUTION<br />
(a) The various distances needed to solve this problem are<br />
shown in Fig. E2.7c. Since the surface of interest lies in a vertical<br />
plane, y c h c 0.9 ft, and from Eq. 2.18 the magnitude<br />
of the force is<br />
F R gh c A<br />
164.0 lbft 3 210.9 ft2310.3 ft2 2 24 2.59 lb<br />
(Ans)<br />
0.3 ft<br />
1 ft<br />
COMMENT Note that this force is independent of the tank<br />
length. The result is the same if the tank is 0.25 ft, 25 ft, or 25 miles<br />
long.<br />
(b) The y coordinate of the center of pressure 1CP2 is found from<br />
Eq. 2.19,<br />
0.3 ft<br />
0.9 ft 2.5 ft<br />
(b)<br />
and from Fig. 2.18<br />
y R I xc<br />
y c A y c<br />
y<br />
x<br />
y c<br />
Median line<br />
y R<br />
1 ft<br />
δ A<br />
0.2 ft<br />
c<br />
c<br />
0.1 ft<br />
CP<br />
CP<br />
x R<br />
0.1 ft 0.15 ft 0.15 ft<br />
(c)<br />
(d)<br />
F I G U R E E2.7b–d<br />
F I G U R E E2.7a<br />
of Tenecor Tanks, Inc.)<br />
(Photograph courtesy