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Modern Engineering Thermodynamics

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136 CHAPTER 4: The First Law of <strong>Thermodynamics</strong> and Energy Transport Mechanisms<br />

Now Let us Write a <strong>Thermodynamics</strong> Problem<br />

Step A. We limit it to a closed system and use the energy balance as our primary equation:<br />

<br />

1Q 2 − 1 W 2 = m ðu 2 − u 1 Þ + V2 2 − V2 1<br />

+ gðZ <br />

2 − Z 1 Þ<br />

2g c<br />

g c<br />

Choose the material. Let the system contain an ideal gas. Then auxiliary equations pv = RT and u 2 − u 1 =<br />

c v (T 2 − T 1 ) can be used.<br />

Choose the unknowns. With two independent equations, we can have two unknowns. Let us choose<br />

1Q 2 and p 2 as the unknowns. We can solve for 1 Q 2 from the energy balance and solve for p 2 = RT 2 /v 2 .<br />

If we put the system in a rigid container, then 1 W 2 = m∫pdv = 0, because for a sealed rigid container,<br />

v = constant, then dv = 0. Let us also add the condition that the process must be isothermal, then<br />

T 2 = T 1 and thus u 2 − u 1 = c v (T 2 − T 1 ) = 0. Further, let us also require that V 2 = V 1 , then the energy<br />

balance reduces to<br />

<br />

1Q 2 − 0 = m 0 + 0 + gðZ <br />

2 − Z 1 Þ<br />

g c<br />

system<br />

Now all we need to do is specify m, Z 1 , and Z 2 and we can compute 1 Q 2 .<br />

Step B. The next step is to write a scenario, or a short story, that uses these processes and values to create a<br />

thermodynamic problem. Let us try this:<br />

There are 5.00 kg of hydrogen gas (an ideal gas) at 20.0°C and 0.300 MPa sealed inside a wooden barrel<br />

(a rigid container) at the top of Niagara Falls. The barrel is not insulated and is maintained at a constant<br />

temperature (i.e., isothermal) as it travels over the falls in contact with the water. Determine<br />

a. The heat transfer from the barrel as it travels 50.0 m vertically between the top and bottom of the falls.<br />

b. The final pressure inside the barrel at the bottom of the falls.<br />

Note that the problem scenario does not have to be deadly serious, you can write problem statements<br />

around anything your imagination can conceive.<br />

Step C. Now we must work the problem in the forward direction to see if all the necessary information has<br />

been provided, so let us try it.<br />

Solution<br />

The problem solving technique requires that we start by reading the problem statement carefully.<br />

Step 1 ask us to draw a sketch of the system (the barrel going over the Niagara Falls, see Figure 4.22) and identify<br />

the material in the system, it is the hydrogen in the barrel.<br />

Step 2 asks us to identify the unknowns. Even though we just wrote the problem statement, it is important to<br />

read it again, carefully, to check for errors and completeness. The problem statement should contain clarifying<br />

statements so that the reader need not make any unreasonable assumptions. For example, in our problem statement,<br />

we identified the hydrogen as an ideal gas, because it is not obvious to a beginning thermodynamics student<br />

which materials behave like an ideal gas and<br />

which do not. Also, while it may be obvious to you<br />

when you wrote the problem statement that a barrel<br />

is to be modeled as a sealed, rigid container, itisadvisable<br />

to tell the reader this in clear terms, since the<br />

purpose of the problem should be to test the problem<br />

solving skills of the reader, not his or her ability<br />

to read your mind about how to interpret unfamiliar<br />

things. The unknowns here are clearly specified in<br />

items (a) and (b) at the end of the problem statement.<br />

They are find 1 Q 2 and p 2 .<br />

Step 3 asks us to identify the system’s typeandits<br />

states. The system here is closed (because the barrel is<br />

sealed). We should be able to identify the system states<br />

from the information given in the problem statement:<br />

State 1 State 2<br />

T 1 = 20:0°C T 2 = T 1 = 20:0°C<br />

p 1 = 0:300 Mpa ?<br />

system<br />

5.00 kg of hydrogen gas<br />

at 20.0°C and 0.300 MPa<br />

Niagara falls<br />

50.0 m<br />

State 1 State 2<br />

FIGURE 4.22<br />

A barrel going over Niagara Falls.

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