fluid_mechanics
262 Chapter 5 ■ Finite Control Volume Analysis Section 5.3.4 Application of the Energy Equation to Nonuniform Flows 5.131 Water flows vertically upward in a circular cross-sectional pipe. At section 112, the velocity profile over the cross-sectional area is uniform. At section 122, the velocity profile is V w c a R r 17 R b kˆ where V local velocity vector, w c centerline velocity in the axial direction, R pipe inside radius, and, r radius from pipe axis. Develop an expression for the loss in available energy between sections 112 and 122. 5.132 The velocity profile in a turbulent pipe flow may be approximated with the expression u a R r u c R where u local velocity in the axial direction, u c centerline velocity in the axial direction, R pipe inner radius from pipe axis, r local radius from pipe axis, and n constant. Determine the kinetic energy coefficient, a, for (a) n 5, (b) n 6, (c) n 7, (d) n 8, (e) n 9, (f) n 10. 5.133 A small fan moves air at a mass flowrate of 0.004 lbms. Upstream of the fan, the pipe diameter is 2.5 in., the flow is laminar, the velocity distribution is parabolic, and the kinetic energy coefficient, a 1 , is equal to 2.0. Downstream of the fan, the pipe diameter is 1 in., the flow is turbulent, the velocity profile is quite flat, and the kinetic energy coefficient, a 2 , is equal to 1.08. If the rise in static pressure across the fan is 0.015 psi and the fan shaft draws 0.00024 hp, compare the value of loss calculated: (a) assuming uniform velocity distributions, (b) considering actual velocity distributions. Section 5.3.5 Combination of the Energy Equation and the Moment-of-Momentum Equation 5.134 Air enters a radial blower with zero angular momentum. It leaves with an absolute tangential velocity, V u , of 200 fts. The rotor blade speed at rotor exit is 170 fts. If the stagnation pressure rise across the rotor is 0.4 psi, calculate the loss of available energy across the rotor and the rotor efficiency. 5.135 Water enters a pump impeller radially. It leaves the impeller with a tangential component of absolute velocity of 10 ms. The impeller exit diameter is 60 mm, and the impeller speed is 1800 rpm. If the stagnation pressure rise across the impeller is 45 kPa, determine the loss of available energy across the impeller and the hydraulic efficiency of the pump. 5.136 Water enters an axial-flow turbine rotor with an absolute velocity tangential component, V u , of 15 fts. The corresponding blade velocity, U, is 50 fts. The water leaves the rotor blade row with no angular momentum. If the stagnation pressure drop across the turbine is 12 psi, determine the hydraulic efficiency of the turbine. 5.137 An inward flow radial turbine 1see Fig. P5.1372 involves a nozzle angle, a 1 , of 60° and an inlet rotor tip speed, U 1 , of 30 fts. The ratio of rotor inlet to outlet diameters is 2.0. The radial component of velocity remains constant at 20 fts through the rotor, and the flow leaving the rotor at section 122 is without angular momentum. If the flowing fluid is water and the stagnation pressure drop across the rotor is 16 psi, determine the loss of available energy across the rotor and the hydraulic efficiency involved. 5.138 An inward flow radial turbine 1see Fig. P5.1372 involves a b 1n nozzle angle, a 1 , of 60° and an inlet rotor tip speed of 30 fts. The ratio of rotor inlet to outlet diameters is 2.0. The radial component of velocity remains constant at 20 fts through the rotor, and the U 1 = 30 ft/s V r1 = 20 ft/s 60° r 2 F I G U R E P5.137 2 r 1 flow leaving the rotor at section 122 is without angular momentum. If the flowing fluid is air and the static pressure drop across the rotor is 0.01 psi, determine the loss of available energy across the rotor and the rotor aerodynamic efficiency. Section 5.4 Second Law of Thermodynamics— Irreversible Flow 5.139 Why do all actual fluid flows involve loss of available energy? ■ Lab Problems 5.140 This problem involves the force that a jet of air exerts on a flat plate as the air is deflected by the plate. To proceed with this problem, go to Appendix H which is located on the book’s web site, www.wiley.com/college/munson. 5.141 This problem involves the pressure distribution produced on a flat plate that deflects a jet of air. To proceed with this problem, go to Appendix H which is located on the book’s web site, www. wiley.com/college/munson. 5.142 This problem involves the force that a jet of water exerts on a vane when the vane turns the jet through a given angle. To proceed with this problem, go to Appendix H which is located on the book’s web site, www.wiley.com/college/munson. 5.143 This problem involves the force needed to hold a pipe elbow stationary. To proceed with this problem, go to Appendix H which is located on the book’s web site, www.wiley.com/college/munson. ■ Life Long Learning Problems 5.144 What are typical efficiencies associated with swimming and how can they be improved? 5.145 Explain how local ionization of flowing air can accelerate it. How can this be useful? 5.146 Discuss the main causes of loss of available energy in a turbo-pump and how they can be minimized. What are typical turbo-pump efficiencies? 5.147 Discuss the main causes of loss of available energy in a turbine and how they can be minimized. What are typical turbine efficiencies? ■ FE Exam Problems Sample FE (Fundamentals of Engineering) exam questions for fluid mechanics are provided on the book’s web site, www.wiley.com/ college/munson. 1
6DD ifferential Analysis of Fluid Flow CHAPTER OPENING PHOTO: Flow past an inclined plate: The streamlines of a viscous fluid flowing slowly past a two-dimensional object placed between two closely spaced plates 1a Hele-Shaw cell2 approximate inviscid, irrotational 1potential2 flow. 1Dye in water between glass plates spaced 1 mm apart.2 1Photography courtesy of D. H. Peregrine.2 Learning Objectives After completing this chapter, you should be able to: ■ determine various kinematic elements of the flow given the velocity field. ■ explain the conditions necessary for a velocity field to satisfy the continuity equation. ■ apply the concepts of stream function and velocity potential. ■ characterize simple potential flow fields. ■ analyze certain types of flows using the Navier–Stokes equations. In the previous chapter attention is focused on the use of finite control volumes for the solution of a variety of fluid mechanics problems. This approach is very practical and useful, since it does not generally require a detailed knowledge of the pressure and velocity variations within the control volume. Typically, we found that only conditions on the surface of the control volume were needed, and thus problems could be solved without a detailed knowledge of the flow field. Unfortunately, there are many situations that arise in which the details of the flow are important and the finite control volume approach will not yield the desired information. For example, we may need to know how the velocity varies over the cross section of a pipe, or how the pressure and shear stress vary along the surface of an airplane wing. In these circumstances we need to develop relationships that apply at a point, or at least in a very small infinitesimal region within a given flow field. This approach, which involves an infinitesimal control volume, as distinguished from a finite control volume, is commonly referred to as differential analysis, since 1as we will soon discover2 the governing equations are differential equations. 263
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262 Chapter 5 ■ Finite Control Volume Analysis<br />
Section 5.3.4 Application of the Energy Equation to<br />
Nonuniform Flows<br />
5.131 Water flows vertically upward in a circular cross-sectional<br />
pipe. At section 112, the velocity profile over the cross-sectional area<br />
is uniform. At section 122, the velocity profile is<br />
V w c a R r 17<br />
R<br />
b kˆ<br />
where V local velocity vector, w c centerline velocity in the<br />
axial direction, R pipe inside radius, and, r radius from pipe<br />
axis. Develop an expression for the loss in available energy between<br />
sections 112 and 122.<br />
5.132 The velocity profile in a turbulent pipe flow may be approximated<br />
with the expression<br />
u<br />
a R r<br />
u c R<br />
where u local velocity in the axial direction, u c centerline velocity<br />
in the axial direction, R pipe inner radius from pipe axis,<br />
r local radius from pipe axis, and n constant. Determine the<br />
kinetic energy coefficient, a, for (a) n 5, (b) n 6, (c) n 7,<br />
(d) n 8, (e) n 9, (f) n 10.<br />
5.133 A small fan moves air at a mass flowrate of 0.004 lbms. Upstream<br />
of the fan, the pipe diameter is 2.5 in., the flow is laminar, the<br />
velocity distribution is parabolic, and the kinetic energy coefficient,<br />
a 1 , is equal to 2.0. Downstream of the fan, the pipe diameter is 1 in.,<br />
the flow is turbulent, the velocity profile is quite flat, and the kinetic<br />
energy coefficient, a 2 , is equal to 1.08. If the rise in static pressure<br />
across the fan is 0.015 psi and the fan shaft draws 0.00024 hp, compare<br />
the value of loss calculated: (a) assuming uniform velocity distributions,<br />
(b) considering actual velocity distributions.<br />
Section 5.3.5 Combination of the Energy Equation<br />
and the Moment-of-Momentum Equation<br />
5.134 Air enters a radial blower with zero angular momentum. It<br />
leaves with an absolute tangential velocity, V u , of 200 fts. The rotor<br />
blade speed at rotor exit is 170 fts. If the stagnation pressure<br />
rise across the rotor is 0.4 psi, calculate the loss of available energy<br />
across the rotor and the rotor efficiency.<br />
5.135 Water enters a pump impeller radially. It leaves the impeller<br />
with a tangential component of absolute velocity of 10 ms. The<br />
impeller exit diameter is 60 mm, and the impeller speed is 1800<br />
rpm. If the stagnation pressure rise across the impeller is 45 kPa,<br />
determine the loss of available energy across the impeller and the<br />
hydraulic efficiency of the pump.<br />
5.136 Water enters an axial-flow turbine rotor with an absolute velocity<br />
tangential component, V u , of 15 fts. The corresponding blade<br />
velocity, U, is 50 fts. The water leaves the rotor blade row with no<br />
angular momentum. If the stagnation pressure drop across the turbine<br />
is 12 psi, determine the hydraulic efficiency of the turbine.<br />
5.137 An inward flow radial turbine 1see Fig. P5.1372 involves a<br />
nozzle angle, a 1 , of 60° and an inlet rotor tip speed, U 1 , of 30 fts.<br />
The ratio of rotor inlet to outlet diameters is 2.0. The radial component<br />
of velocity remains constant at 20 fts through the rotor, and<br />
the flow leaving the rotor at section 122 is without angular momentum.<br />
If the flowing <strong>fluid</strong> is water and the stagnation pressure drop<br />
across the rotor is 16 psi, determine the loss of available energy<br />
across the rotor and the hydraulic efficiency involved.<br />
5.138 An inward flow radial turbine 1see Fig. P5.1372 involves a<br />
b<br />
1n<br />
nozzle angle, a 1 , of 60° and an inlet rotor tip speed of 30 fts. The<br />
ratio of rotor inlet to outlet diameters is 2.0. The radial component<br />
of velocity remains constant at 20 fts through the rotor, and the<br />
U 1 =<br />
30 ft/s<br />
V r1 =<br />
20 ft/s<br />
60°<br />
r 2<br />
F I G U R E P5.137<br />
2<br />
r 1<br />
flow leaving the rotor at section 122 is without angular momentum.<br />
If the flowing <strong>fluid</strong> is air and the static pressure drop across the rotor<br />
is 0.01 psi, determine the loss of available energy across the rotor<br />
and the rotor aerodynamic efficiency.<br />
Section 5.4 Second Law of Thermodynamics—<br />
Irreversible Flow<br />
5.139 Why do all actual <strong>fluid</strong> flows involve loss of available energy?<br />
■ Lab Problems<br />
5.140 This problem involves the force that a jet of air exerts on a<br />
flat plate as the air is deflected by the plate. To proceed with this<br />
problem, go to Appendix H which is located on the book’s web site,<br />
www.wiley.com/college/munson.<br />
5.141 This problem involves the pressure distribution produced on<br />
a flat plate that deflects a jet of air. To proceed with this problem, go<br />
to Appendix H which is located on the book’s web site, www.<br />
wiley.com/college/munson.<br />
5.142 This problem involves the force that a jet of water exerts on<br />
a vane when the vane turns the jet through a given angle. To proceed<br />
with this problem, go to Appendix H which is located on the book’s<br />
web site, www.wiley.com/college/munson.<br />
5.143 This problem involves the force needed to hold a pipe elbow<br />
stationary. To proceed with this problem, go to Appendix H which is<br />
located on the book’s web site, www.wiley.com/college/munson.<br />
■ Life Long Learning Problems<br />
5.144 What are typical efficiencies associated with swimming<br />
and how can they be improved?<br />
5.145 Explain how local ionization of flowing air can accelerate<br />
it. How can this be useful?<br />
5.146 Discuss the main causes of loss of available energy in a<br />
turbo-pump and how they can be minimized. What are typical<br />
turbo-pump efficiencies?<br />
5.147 Discuss the main causes of loss of available energy in a<br />
turbine and how they can be minimized. What are typical turbine<br />
efficiencies?<br />
■ FE Exam Problems<br />
Sample FE (Fundamentals of Engineering) exam questions for <strong>fluid</strong><br />
<strong>mechanics</strong> are provided on the book’s web site, www.wiley.com/<br />
college/munson.<br />
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