Drawing a PV Diagram: Solving Homework w/ Work Calculation

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SUMMARY

The discussion focuses on solving a homework problem involving the thermodynamic cycle of one mole of an ideal gas. The cycle consists of four steps: isothermal expansion, isobaric compression, isothermal compression, and isobaric expansion. Key equations referenced include the ideal gas law (PV = nRT) and the calculation of work done via the area under the PV diagram. The participants clarify the relationships between pressure and volume during each step, emphasizing the importance of understanding isothermal and isobaric processes.

PREREQUISITES
  • Understanding of the ideal gas law (PV = nRT)
  • Knowledge of thermodynamic processes: isothermal and isobaric
  • Familiarity with PV diagrams and area calculations
  • Basic concepts of work done in thermodynamics
NEXT STEPS
  • Study the derivation and applications of the ideal gas law (PV = nRT)
  • Learn how to calculate work done in isothermal and isobaric processes
  • Explore the concept of thermodynamic cycles and their significance
  • Practice plotting PV diagrams for various thermodynamic processes
USEFUL FOR

Students studying thermodynamics, physics enthusiasts, and anyone needing to understand the principles of gas behavior in thermodynamic cycles.

imatreyu
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Homework Statement



One mole of an ideal gas at an inital tempreature of 300K and pressure of 4 atm is carried through the following reversible cycle:

a) It expands isothermally until its volume is doubled.
b) It is compressed to its original volume at constant pressure.
c) It is compressed isothermally to a pressure of 4 atm.
d) It expands at constant pressure to its original volume

Make a plot of this cycle process on a PV diagram and calculate the work done by the gas per cycle.

Homework Equations



The Attempt at a Solution



Okay so step a. means that while Vo goes to 2Vo the pressure doubles as well, yes? And step b means that the pressure is the same but the volume goes to Vo. And so then step C should mean that since P is returning to its initial, the gas returns to Vo too, right? But if that's true, then D doesn't make sense since it has already returned to Vo.

Please help! Once I get the diagram correct, I'm just going to use the area to find the work done.
 
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imatreyu said:
Okay so step a. means that while Vo goes to 2Vo the pressure doubles as well, yes?

Take a look at the PV = nRT equation. If T is held constant (isothermal), how must P and V relate to each other?

And step b means that the pressure is the same but the volume goes to Vo. And so then step C should mean that since P is returning to its initial, the gas returns to Vo too, right?

Again, take a look at PV = nRT. What's the current volume and pressure when step C begins? How do P and V vary when the compression (or expansion) is isothermal?
 
Oh okay haha. . .P has to be half. . .

Thank you :)
 

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