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Modern Engineering Thermodynamics

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6.10 Open System Unsteady State Processes 191<br />

Also, the system has a single-inlet flow stream but no outlet flow stream. To carry out the analysis, we note that<br />

the system does not contain a work mode, so _W = 0: Also, the system is not moving, so<br />

½dðKE + PEÞ/dtŠ system<br />

= 0<br />

Finally, we assume that the tank is filled slowly enough that we can ignore the inlet flow stream’s specific kinetic and<br />

potential energy terms. Under these conditions, the generalized energy rate balance equation becomes<br />

or<br />

_Q − 0 + _m in ðh in + 0 + 0Þ− 0 = ðdU/dt + 0 + 0<br />

_Q + _m in h in = ½dmu<br />

ð Þ/dt<br />

Then, multiplying through by dt and integrating over the filling process gives<br />

1Q 2 +<br />

Z 2<br />

1<br />

Š tank<br />

h in dm in = ðm 2 u 2 − m 1 u 1 Þ tank<br />

where state 1 is the initial state inside the tank and state 2 is the state inside the tank after it has been filled. When<br />

the tank is filled from a pipe of unlimited supply, as shown in Figure 6.14, h in = constant and this equation becomes<br />

1Q 2 + h in m in = ðm 2 u 2 − m 1 u 1 Þ tank<br />

where the conservation of mass law for the filling process gives<br />

Combining the previous two equations, we obtain<br />

m in = ðm 2 − m 1 Þ tank<br />

u 2 = u 1 ðm 1 /m 2 Þ+ 1 Q 2 /m 2 + h in ð1 − m 1 /m 2 Þ (6.33)<br />

where the numerical subscripts refer exclusively to states inside the tank from this point on.<br />

By knowing p 2 from the filling process and calculating u 2 from Eq. (6.33), we have fixed the final thermodynamic<br />

state of the filled tank and can then find the value of any other property we desire, say its final temperature T 2 .To<br />

illustrate this, let us assume the tank is insulated ( 1 Q 2 = 0) and initially evacuated (m 1 = 0). Then, Eq. (6.33)<br />

becomes:<br />

Þ tank<br />

u 2 = h in (6.34)<br />

If we now assume that the tank is filled with an incompressible fluid, then we can utilize Eq. (6.19) and write<br />

u 2 = cT 2 = h in = cT in + vp in<br />

or<br />

T 2<br />

<br />

filling<br />

incomp:<br />

fluid<br />

= T in + ðvp in Þ/c (6.35)<br />

and the compression process of pressurizing the tank would cause T 2 to be greater than T in by an amount ðvp in Þ/c:<br />

EXAMPLE 6.7<br />

A high-pressure water storage system is used to fill initially empty, rigid, insulated tanks with liquid water. The temperature<br />

of the water entering the tank is 20.0°C and the final pressure of the water in the tank is 50.0 MPa. Determine the final temperature<br />

of the water in the tank immediately after it has been filled.<br />

Solution<br />

First, draw a sketch of the system (Figure 6.15).<br />

(Continued )

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