First Law of Thermodynamics issue

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SUMMARY

The forum discussion addresses a physics problem involving the First Law of Thermodynamics, specifically regarding the behavior of nitrogen gas in a cylinder under two scenarios: constant volume and constant pressure. For part A, the final temperature of the air at constant volume was incorrectly calculated as 1126 K using the equation dU = nCv(Tf - Ti) with Cv = 3/2R. For part B, the correct approach involves using the ideal gas law and recognizing that Cv changes to Cp when the volume is allowed to increase, leading to the equation dU = Q - W, where W is the work done by the gas.

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  • Understanding of the First Law of Thermodynamics
  • Familiarity with the ideal gas law (PV = nRT)
  • Knowledge of specific heat capacities (Cp and Cv) for diatomic gases
  • Ability to manipulate equations involving internal energy (dU)
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  • Study the derivation and application of the ideal gas law in thermodynamic processes
  • Learn about the differences between Cp and Cv for various gases
  • Explore the implications of constant volume vs. constant pressure processes in thermodynamics
  • Practice solving thermodynamic problems involving heat transfer and work done
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Homework Statement


In an experiment to simulate conditions within an automobile engine, 0.155 mol of air at a temperature of 780K and a pressure of 3.20x106 Pa is contained in a cylinder of volume 310 cm3. Then 670 J of heat is transferred to the cylinder.

A) If the volume of the cylinder is constant while the heat is added, what is the final temperature of the air? Assume that the air is essentially nitrogen gas.

B) If instead the volume of the cylinder is allowed to increase while the pressure remains constant, find the final temperature of the air.

Homework Equations


Const P W= pdV Q=nCpdT
Const V W = 0 Q = nCvdT
dU = nCdT
Cp = 5/2R
Cv = 3/2R

The Attempt at a Solution


For part A where Volume is constant, it told me that 670 J of heat is added which would be the Q value for dU. so the overall internal energy is 670 J from that I used the equation dU= nCv(Tf-Ti) which with values came out too 670 = (.155)(3/2*8.314)(Tf-780) which equaled 1126 K. which ended up not being the right answer. I do not know what else to try.

For Part B, I know I need to figure out dU which is Q-W so for this equation it would come out to dU = 670 - pdV or dU = 670 - 3.20E6(Vf-3.1E-4m3). but don't really know where to go from here
 
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  • Nitrogen is a diatomic gas therefore Cv=2.5

    For part B, find Vf as you have been finding and then use the ideal gas relation:

    PV=nRT

 
the Diatomic gas worked, forgot about that tidbit.

but for the Part B I don't fully understand what you mean because I have 2 unknown variables V_f and T_f which is why I am a little lost.
 
Figured it out thanks!, took a good minute though
 
Can you please share the workings of the solution
 
For part b, you use the same equation and everything except that Cv is now Cp, which is just Cv + R.
 

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