2 Steady Flow of a Liquid through an Adiabatic Duct 16-1Steady Flow of a Liquid through an Adiabatic Duct(fig.16-1)
3 Three States of a Fluid on an h-s Diagram 16-2Three States of a Fluid on an h-s DiagramThe actual state, actual stagnation state, and isentropic stagnation state of a fluid on an h-s diagram(Fig.16-3)
4 16-3Completely Arresting the Flow of an Ideal Gas can Raise its Temperature(Fig.16-5)The temperature of an ideal gas flowing at a velocity V rises by V2/(2CP) when it is brought to a complete stopSTOP
5 Propagation of a Small Pressure Wave Along a Duct 16-4Propagation of a Small Pressure Wave Along a Duct
6 Control Volume Moving With the Small Pressure Wave Along a Duct 16-5Control Volume Moving With the Small Pressure Wave Along a Duct(Fig. 16-8)
7 The Velocity of Sound Changes With Temperature 16-6The Velocity of Sound Changes With Temperature(Fig. 16-9)
8 16-7The Mach Number Can Vary With Different Temperatures Even With Equivalent Velocities(Fig )
9 Throat: The Smallest Flow Area of a Nozzle 16-8Throat: The Smallest Flow Area of a Nozzle
10 16-9Supersonic Velocities Cannot be Obtained by Attaching a Converging SectionWe cannot obtain supersonic velocities by attaching a a converging section to a converging nozzle. Doing so will only move the sonic cross section farther downstream
11 16-10Variation of Flow Properties in Subsonic and Supersonic Nozzles and Diffusers(Fig )
12 16-11Effect of Back Pressure on the Pressure Distribution Along a Converging Nozzle(Fig )
13 16-12Effect of Back Pressure of a Converging Nozzle on Mass Flow Rate and Exit PressureThe effect of back pressure Pb on the mass flow rate m and the exist pressure Pe of a converging nozzle(Fig )
14 16-13Variation of the Mass Flow Rate Through a Nozzle with Inlet Stagnation Properties(Fig )
15 16-14The Effect of Back Pressure on the Flow Through a Converging-Diverging Nozzle(Fig.16-26)
16 The h-s Diagram for Flow Across a Normal Shock 16-15The h-s Diagram for Flow Across a Normal Shock(Fig )
17 Entropy Change Across the Normal Shock 16-16Entropy Change Across the Normal Shock(Fig )
18 Isentropic and Actual (Irreversible) Flow in a Nozzle 16-17Isentropic and Actual (Irreversible) Flow in a NozzleIsentropic and actual flow in a nozzle between the same inlet state and the exit pressure(Fig )
19 16-18Schematic and h-s Diagram for the Definition of the Diffuser Efficiency(Fig )
20 The h-s Diagram for the Isentropic Expansion of Steam in a Nozzle 16-19The h-s Diagram for the Isentropic Expansion of Steam in a Nozzle(Fig )
21 Schematic and h-s Diagram for Example 16-14 16-20Schematic and h-s Diagram for Example 16-14(Fig.16-38)
22 16-21Chapter SummaryIn this chapter the thermodynamic aspects of high-speed fluid flow are examined. For high-speed flows, it is convenient to combine the enthalpy and the kinetic energy of the fluid into a single term called stagnation (or total) enthalpy h0, defined as (kJ/kg) The properties of a fluid at the stagnation state are called stagnation properties and are indicated by the subscript zero.
23 16-22Chapter SummaryThe stagnation temperature of an ideal gas with constant specific heats is which represents the temperature an ideal gas will attain when it is brought to rest adiabatically.
24 16-23Chapter SummaryThe (isentropic) stagnation properties of an ideal gas are related to the static properties of the fluid by
25 16-24Chapter SummaryWhen stagnation enthalpies are used, the conservation of energy equation for a single-stream, steady-flow device can be expressed as where h01 and h02 are the stagnation enthalpies at states 1 and 2, respectively.
26 16-25Chapter SummaryThe velocity at which an infinitesimally small pressure wave travels through a medium is the velocity of sound (or the sonic velocity). It is expressed as
27 16-26Chapter SummaryFor an ideal gas the velocity of sound becomes
28 16-27Chapter SummaryThe Mach number is the ratio of the actual velocity of the fluid to the velocity of sound at the same state:
29 16-28Chapter SummaryThe flow is called sonic when M = 1, subsonic when M < 1, supersonic when M > 1, hypersonic when M >> 1, and transonic when M 1.=~
30 16-29Chapter SummaryThe nozzles whose flow area decreases in the flow direction are called converging nozzles. Nozzles whose flow area first decreases and then increases are called converging-diverging nozzles. The location of the smallest flow area of a nozzle is called the throat.
31 16-30Chapter SummaryThe highest velocity to which a fluid can be accelerated in a convergent nozzle is the sonic velocity. Accelerating a fluid to supersonic velocities is only possible in converging-diverging nozzles. In all supersonic converging-diverging nozzles, the flow velocity at the throat is the velocity of sound.
32 16-31Chapter SummaryThe ratios of the stagnation to static properties for ideal gases with con-stant specific heats can be expressed in terms of the Mach number as
33 16-32Chapter SummaryWhen M = 1, the resulting static-to-stagnation property ratios for the temperature, pressure, and density are called critical ratios and are denoted by the superscript asterisk:
34 16-33Chapter SummaryThe pressure outside the exit plane of a nozzle is called the back pressure. For all back pressures lower than P*, the pressure at the exit plane of the converging nozzle is equal to P*, the Mach number at the exit plane is unity, and the mass flow rate is the maximum (or choked) flow rate.
35 16-34Chapter SummaryUnder steady-flow conditions, the mass flow rate through the nozzle is constant and can be expressed as
36 16-35Chapter SummaryThe variation of flow area A through the nozzle relative to the throat area A* for the same mass flow rate and stagnation properties of a particular ideal gas is
37 16-36Chapter SummaryThe parameter M* is defined as the ratio of the local velocity to the velocity of sound at the throat (M = 1): It can also be expressed as
38 16-37Chapter SummaryIn some range of back pressure, the fluid that achieved a sonic velocity at the throat of a converging-diverging nozzle and is accelerating to supersonic velocities in the diverging section experiences a normal shock, which causes a sudden rise in pressure and temperature and a sudden drop in velocity to subsonic levels. Flow through the shock is highly irreversible, and thus it cannot be approximated as isentropic.
39 16-38Chapter SummaryThe properties of an ideal gas with constant specific heats before (subscript x) and after (subscript y) a shock are related by
40 16-39Chapter SummaryThe entropy change across the shock is obtained by applying the entropy-change equation for an ideal gas across the shock:
41 Chapter Summary Actual kinetic energy at nozzle exit 16-40Chapter SummaryThe deviation of actual nozzles from isentropic ones is expressed in terms of the nozzle efficiency N, nozzle velocity coefficient CV, and the coefficient of discharge CD, which are defined as where h01 is the stagnation enthalpy of the fluid at the nozzle inlet, h2 is the actual enthalpy at the nozzle exit, and h2s is the exit enthalpy under isentropic conditions for the same exit pressure.Actual kinetic energy at nozzle exitKinetic energy at nozzle exit for isentropic flow from the same inlet state to the same exit pressureActual velocity at nozzle exitVelocity at nozzle exit for isentropic flow from the same inlet state to the same exit pressureActual mass flow rate through nozzleMass flow rate through nozzle for isentropic flow from the same inlet state to the same exit pressure=
42 16-41Chapter SummaryThe performance of a diffuser is expressed in terms of the diffuser efficiency D the pressure recovery factor FP, and the pressure rise coefficient CPR. They are defined asActual stagnation pressure at diffuser exitIsentropic stagnation pressureFp==CprActual pressure riseIsentropic pressure rise==
43 16-42Chapter SummarySteam often deviates considerably from ideal-gas behavior, and no simple property relations are available for it. Thus it is often necessary to use steam tables instead of ideal-gas relations. The critical-pressure ratio of steam is often taken to be 0.546, which corresponds to a specific heat ratio of k = 1.3 for superheated steam.
44 16-43Chapter SummaryAt high velocities, steam does not start condensing when it encounters the saturation line, and it exists as a supersaturated substance. Supersaturation states are nonequilibrium (or metastable) states, and care should be exercised in dealing with them.
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