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Question 3
Figure 4 shows a gas strut supporting the lid of a trailer. A fixed mass of nitrogen gas is sealed into the cylinder of the strut. The gas is initially at a pressu... show full transcript
Step 1
Answer
To find the final pressure and temperature of the gas, we can use the adiabatic relations for an ideal gas:
The pressure-volume relation: P_1 V_1^{rac{eta}{eta-1}} = P_2 V_2^{rac{eta}{eta-1}} where ( \beta = \gamma = 1.4 ) for nitrogen.
The temperature-volume relation:
Let's denote:
Now we can calculate the final pressure, ( P_2 ): After computing the above expression, we find:
Next, calculate the final temperature, ( T_2 ): This yields a final temperature of approximately K.
Step 2
Answer
The rapid compression of the gas can be assumed to be an adiabatic process because during the quick closing of the lid, there is not enough time for heat exchange between the gas and its surroundings. In an adiabatic process, by definition, no heat transfer occurs (( Q = 0 )). As the compression happens swiftly, the temperature of the gas increases due to work done on it without any heat lost or gained.
Step 3
Answer
When the lid is closed slowly, the gas has enough time to exchange heat with its surroundings. This means that during compression, the temperature of the gas remains constant, which characterizes an isothermal process. In an isothermal process, the internal energy of the gas remains unchanged, and any work done on the gas is offset by heat transfer into the gas. Therefore, the compression can be treated as isothermal when the lid is closed slowly.
Step 4
Answer
In an adiabatic process, the work done on the gas results in an increase in internal energy and temperature, as there is no heat transfer. Consequently, the work done during adiabatic compression is greater than that done during isothermal compression, where the temperature remains constant and some work is used to transfer heat out of the gas. Thus, while the gas behaves differently in each case, the work done in the adiabatic case is greater due to the inability to dissipate heat.
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