How Do You Calculate Work on a pV Diagram When Pressure Varies?

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SUMMARY

The calculation of work done by a gas during a variable pressure process on a pV diagram is determined by integrating the pressure with respect to volume, expressed as W = ∫p dV. This method accounts for non-constant pressure, where pressure is treated as a function of volume. The area under the curve on the pV graph represents the work done, particularly when the graph forms a trapezium shape, simplifying the integration process. The discussion emphasizes the importance of understanding the relationship between pressure and volume in calculating work for ideal gases.

PREREQUISITES
  • Understanding of ideal gas laws
  • Familiarity with calculus, specifically integration
  • Knowledge of pressure-volume (pV) diagrams
  • Concept of work in thermodynamics
NEXT STEPS
  • Study the integration of pressure functions in thermodynamic processes
  • Learn about the area under curves in pV diagrams
  • Explore the implications of non-constant pressure in gas laws
  • Investigate the trapezoidal rule for calculating areas under curves
USEFUL FOR

Students and professionals in physics and engineering, particularly those focusing on thermodynamics and fluid mechanics, will benefit from this discussion on calculating work in variable pressure scenarios.

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W = p*deltaV only holds for the case of constant p, that is true.

What is the general form of the work eqn. that holds for all types of paths? (Hint: It also invloves p and V, and it must reduce to the W = p*deltaV, when p is constant)
 
Is it W = p1V1 - p2V2?
 
No, recall that work done is given by W = F.x, hence dW = F.dx, where dx is a infinitesimal displacement in the direction of the force.

For ideal gases, F = pA, hence dW = pA.dx, or dW = p.dV.

Work is then found from integrating p.dV, with respect to V from Vfinal to Vinitial, which can be interpreted as the area under the pV graph
 
So pV from Vi to Vf, but isn't p still constant in this case?

The graph indicates that p is NOT constant.
 
no, p as indicated in this equation of the general case, is a function of V.
 
okay let's say from 1 to 3, pressure is decreasing from 3p to 2p, how would I apply that to pV| from Vi to Vf?

p(3V) - p(2V)?
 
Integration between two points of a function can be simplified by taking the area under the curve. Because, the graph is linear, it is very easy to find the value of the integral from 1 - 3 - 6, because the area under the curve is a trapezium (or trapezoid).
 

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