How can we prove the work done by gas expansion in any deformable container?

Click For Summary
SUMMARY

The discussion centers on proving the work done by gas expansion in deformable containers, specifically through the formula W=∫p.dV. The key point is establishing that dV=S.h, where S represents the surface area and h is the small displacement normal to the surface. The mathematical foundation involves using concepts from differential geometry, particularly the introduction of R^n-1 sub-manifolds and their orthogonal complements. This leads to the conclusion that the work done can be expressed as dW=F.h=p.S.h=p.dV for any n-volume.

PREREQUISITES
  • Differential geometry concepts, particularly sub-manifolds
  • Understanding of gas laws and thermodynamics
  • Familiarity with calculus, specifically integration techniques
  • Knowledge of physical principles related to work and energy
NEXT STEPS
  • Study differential geometry and its applications in physics
  • Explore gas laws and their implications in deformable containers
  • Learn advanced calculus techniques, focusing on integration in multiple dimensions
  • Research the principles of work and energy in thermodynamic systems
USEFUL FOR

Physicists, engineers, and students studying thermodynamics and fluid mechanics, particularly those interested in the mathematical modeling of gas behavior in deformable containers.

raopeng
Messages
83
Reaction score
0
In my textbook W=∫p.dV is only proved for a syringe with a piston. This is quite easily done but the book never explains how it extrapolates to the general situation for a gas expanding in any deformable container. It seems the point is to prove dV= S.h where S is the surface area of a given container and h is a small displacement alone the direction of the normal to the surface. I tried in this line of thought but things soon get really mathematical and confusing. How can prove this formula in any deformable containers? Thanks in advance!
 
Physics news on Phys.org
Well the mathematical idea is that since for a (n-1) sub-manifold a R^n-1 can be introduced, the orthogonal complement to the hyperplane R^n-1 becomes after a suitable diffeomorphism the normal to the surface in the space, Hence it is possible to write dV=S.h for any n-volume. Then dW=F.h=p.S.h=p.dV...
 

Similar threads

  • · Replies 15 ·
Replies
15
Views
3K
Replies
1
Views
2K
  • · Replies 8 ·
Replies
8
Views
4K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 5 ·
Replies
5
Views
4K
  • · Replies 11 ·
Replies
11
Views
3K
  • · Replies 14 ·
Replies
14
Views
6K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 33 ·
2
Replies
33
Views
4K