Thin-walled pressure vessel, hoop stress Question

Click For Summary
SUMMARY

The discussion centers on the calculations of hoop stress in thin-walled pressure vessels, specifically focusing on the forces acting on a cylindrical shell. The internal pressure, denoted as 'p', exerts a force on the cross-sectional area, which is represented as p*2πr² for the vertical slice of the cylinder. The equilibrium equations derived from the axial and hoop directions confirm that the forces balance out, leading to the expressions 2πRtσ_axial = pπR² and 2Ltσ_hoop = p(2R)L. Understanding these principles is crucial for accurate stress analysis in pressure vessel design.

PREREQUISITES
  • Understanding of thin-walled pressure vessel theory
  • Familiarity with hoop stress and axial stress concepts
  • Knowledge of equilibrium equations in mechanics
  • Basic proficiency in mathematical notation and formulas
NEXT STEPS
  • Study the derivation of the thin-walled pressure vessel equations
  • Learn about the differences between axial and hoop stress in cylindrical structures
  • Explore the application of the Mohr's Circle for stress analysis
  • Investigate the design standards for pressure vessels, such as ASME BPVC
USEFUL FOR

Mechanical engineers, structural engineers, and students studying solid mechanics or pressure vessel design will benefit from this discussion, particularly those involved in stress analysis and design optimization of pressure vessels.

kidsasd987
Messages
142
Reaction score
4
Engineering news on Phys.org
kidsasd987 said:
http://www.efunda.com/formulae/solid_mechanics/mat_mechanics/pressure_vessel.cfmaccording to the text above, we assume that force acting on the thin wall is p*2pi*r^2
whcih is the internal area of vertical slice.

But I am not sure why the area has to be 2*pi*r^2. I mean, why pressure on the crossectional area all applied to the thin wall?
I did not see a p*2pi*r^2 anywhere. Is this a case of a cylinder or a sphere?
 
They split the cylinder in half (including the air inside), and determine the forces on half the cylinder, either axially or in the hoop direction. Axially, the forces on the half-cylinder are ##p\pi R^2## and ##2\pi R\sigma_{axial} t##, where ##\sigma_{axial}## is the axial stress in the shell. So, for equilibrium, $$2\pi R t\sigma_{axial}=p\pi R^2$$
Similarly, for the hoop direction, the forces on half the half-cylinder are ##p(2R)L## and ##2Lt\sigma_{hoop}##. So, for equilibrium,
$$2Lt\sigma_{hoop}=p(2R)L$$
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
Replies
6
Views
4K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 6 ·
Replies
6
Views
7K
  • · Replies 10 ·
Replies
10
Views
3K
Replies
8
Views
17K
  • · Replies 9 ·
Replies
9
Views
5K
  • · Replies 11 ·
Replies
11
Views
2K