Thin-walled pressure vessel, hoop stress Question

AI Thread Summary
The discussion focuses on the calculations of hoop stress in thin-walled pressure vessels, specifically addressing the force acting on the thin wall, which is represented as p*2πr^2. There is confusion regarding why this area is used and how it relates to the pressure applied to the cross-sectional area of the vessel. Participants clarify that the calculations consider a half-cylinder model, analyzing forces in both axial and hoop directions. For equilibrium, the relationships between pressure, area, and stress are established, demonstrating the balance of forces in the vessel. The conversation emphasizes the importance of understanding these concepts for accurate pressure vessel design.
kidsasd987
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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,
$$2Lt\sigma_{hoop}=p(2R)L$$
 
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