Heat and internal energy of gas

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The discussion focuses on the internal energy change and heat transfer of one mole of an ideal diatomic gas transitioning from point a to c. The change in internal energy during this transition is calculated as -4987 J. For the indirect path abc, the required heat is determined to be 5013 J, highlighting that the heat added varies depending on the path taken. The calculations reveal that the heat added along path abc differs from that of the direct path ac, confirming that heat is path-dependent. Understanding these principles is crucial for analyzing thermodynamic processes in gases.
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One mole of an ideal diatomic gas at room temperature undergoes a transition from a to c along the diagonal path in Figure 19-23.
hrw7_19-23.gif

(a) During the transition, what is the change in internal energy of the gas?
-4987 J
(b) How much energy is added to the gas as heat?
____ J
(c) How much heat is required if the gas goes from a to c along the indirect path abc?
5013 J

I got part a and c right. I found the energies for path abc and added them together, because I couldn't find a way with path ac. Does the path I took matter for the heat? How do I find it using path ac?
 

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For path ac, ##\Delta (PV)=nR\Delta T$=-2000J##. The change in internal energy is ##\Delta U=nC_v\Delta T=n\frac{5}{2}R\Delta T=\frac{5}{2}(-2000)=-5000J##

The work in going from a to c is ##\int{PdV}=7000J##, so from the first law, ##Q=\Delta U+W=-5000+7000=2000J##

Along path ab, the expansion is at constant pressure, so ##Q=\Delta H=nC_p\delta T=n\frac{7}{2}R\Delta T=\frac{7}{2}\Delta (PV)=10000=35000J##

Along path bc, the change is at constant volume, so ##Q=nC_v\Delta T=n\frac{5}{2}R\Delta T=\frac{5}{2}\Delta (PV)=\frac{5}{2}(-12000)=-30000J##

So the heat added along path abc is Q = (35000)-(30000)=5000J

So the heat added along path abc is different from that for the direct path ac. Of course, this confirms that heat added is a function of path.
 
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