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Modern Engineering Thermodynamics

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674 CHAPTER 16: Compressible Fluid Flow<br />

where ∑ net F ext g c is the net sum of all the external forces acting on the system. Note that, for a closed system,<br />

_m = 0andm closed system = constant. Then, Eq. (16.32) reduces to Newton’s second law for a fixed mass closed<br />

system:<br />

d<br />

dt ðmVÞ closed<br />

system<br />

<br />

= m dV <br />

= ma<br />

dt closed closed<br />

system system<br />

= ∑ F ext g c<br />

net<br />

Also, the external forces are normally divided into two categories: surface forces, such as pressure and contact<br />

forces, and body forces, such as gravity and magnetic forces. That is,<br />

∑F ext = ∑F surface +∑F body<br />

For a steady state, steady flow, single-inlet, single-outlet open system, Eq. (16.32) further reduces to<br />

Linear momentum rate balance (SS, SF, SI, SO):<br />

∑F ext = _mðV out − V in Þ/g c (16.33)<br />

EXAMPLE 16.10<br />

An air jet is used to levitate a 5.00 × 10 –3 kg sheet of paper, as shown in Figure 16.20. The diameter of the jet at the nozzle<br />

exit is 3.00 × 10 –3 m and it is at atmospheric pressure at 20.0°C. Determine the velocity of the jet.<br />

Solution<br />

W<br />

Assume the flow is steady state and steady flow. Then, the y<br />

Paper<br />

component of Eq. (16.33) is<br />

F y = −W = _mðV out − V in Þ y<br />

/g c<br />

where W is the weight of the paper, given by<br />

W = mg/g c = ð5:00 × 10 −3 kgÞð9:81 m=s 2 Þ/ð1Þ = 0:0491 N<br />

y<br />

0.003 m in diameter<br />

and<br />

ðV out Þ y<br />

= 0<br />

Nozzle<br />

Also, _m = ρAV = ρπ D 2 V/4, where<br />

Then,<br />

So,<br />

ρ =<br />

p<br />

RT = 101:3 × 10 3 kg/ðm.s 2 Þ<br />

½286 m 2 /ðs 2 . = 1:21 kg/m3<br />

KÞŠð293:15 KÞ<br />

W = _mðV in Þ y<br />

/g c = ρAV 2 in /g c = ρπ D 2 V 2 in /4g c<br />

FIGURE 16.20<br />

Example 16.10.<br />

x<br />

Air flow<br />

<br />

V in =<br />

4g " # 1/2<br />

cW<br />

4ð1Þð0:0491 kg.m=s 2 1/2<br />

Þ<br />

=<br />

ρπ D 2 ð1:21 kg=m 3 ÞðπÞð3:00 × 10 − 3 mÞ 2 = 75:7m=s<br />

Exercises<br />

25. The nozzle diameter in Example 16.10 is to be reduced from 3.00 × 10 –3 m to 1.50 × 10 –3 m. Determine the velocity of<br />

the resulting jet required to levitate the sheet of paper, assuming all the other variables remain unchanged. Answer:<br />

V jet = 151 m/s.<br />

26. Suppose the sheet of paper in Example 16.10 is replaced by a sheet of cardboard with a mass of 5 × 10 –2 kg. Determine<br />

the velocity of the jet required to levitate the cardboard, assuming all the other variables remain unchanged. Answer:<br />

V jet = 239 m/s.<br />

27. If the air jet in Example 16.10 is at 0.00°C rather than 20.0°C, determine the velocity of the jet required to levitate the<br />

sheet of paper assuming all the other variables remain unchanged. Answer: V jet = 73.1 m/s.

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