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Stress Analysis in Thin-Walled Pressure Vessels: Cylindrical and Spherical Vessels, Slides of Fluid Mechanics

This document provides an overview of stress analysis in thin-walled cylindrical and spherical pressure vessels. It details the calculation of tangential and longitudinal stresses in cylindrical vessels, and normal stress in spherical vessels, under internal pressure. Sample problems with detailed solutions illustrate these concepts, making it a useful resource for students and engineers. It aids in understanding the design and analysis of pressure vessels, widely used across industries, offering clear explanations and enhancing educational value through practical application. Concise and focused, it's valuable for those studying pressure vessel behavior.

Typology: Slides

2021/2022

Available from 06/06/2025

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ENGR. BON RYAN ANIBAN
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Download Stress Analysis in Thin-Walled Pressure Vessels: Cylindrical and Spherical Vessels and more Slides Fluid Mechanics in PDF only on Docsity!

ENGR. BON RYAN ANIBAN

Cylindrical and spherical vessels are commonly used in industry to serve as boilers

or tanks. When under pressure, the material of which they are made is subjected to a

loading from all directions. Although this is the case, the vessels can be analyzed in a

simple manner provided it has a thin wall.

In general, โ€œthin wallโ€ refers to a vessel having an inner-

radius-to-wall-thickness ratio of 10 or more ( r / t โ‰ฅ 10 ).

Provided the vessel wall is โ€œthin,โ€ the stress distribution

throughout its thickness will not vary significantly, and so

assumed that it is uniform or constant.

Using this assumption, we will analyze the state of stress in

thin-walled cylindrical and spherical pressure vessels.

t

ฯƒt

ฯƒL

D

a

a

L

The tangential stress ( ฯƒt ) can be determined

by considering the vessel to be cut by plane a-a ,

other common names are circumferential stress, hoop stress, and girth stress.

The tangential stress ( ฯƒt ) can be determined

by considering the vessel to be cut by plane a-a ,

other common names are circumferential stress, hoop stress, and girth stress.

ฯƒt

ฯƒt

t

t

L

D

p

z

y

x

t

ฯƒt

ฯƒL

D

L

The longitudinal stress ( ฯƒL ) can be determined by

considering the vessel to be cut by plane b-b , and isolate

the left portion of plane b-b. As shown in the figure, ฯƒL acts

uniformly throughout the wall, and p acts on the section

of the contained fluid.

t

ฯƒt

ฯƒL

D

L

b

The longitudinal stress ( ฯƒL ) can be determined by

considering the vessel to be cut by plane b-b , and isolate

the left portion of plane b-b. As shown in the figure, ฯƒL acts

uniformly throughout the wall, and p acts on the section

of the contained fluid.

Consider the vessel to have a wall thickness t , inner diameter

D , and subjected to an internal pressure p. A small element of the vessel that is sufficiently removed and oriented as shown, is subjected to normal stress ฯƒS. If the spherical vessel is cut in

half by plane c-c , the resulting free-body diagram is shown.

ฯƒs

ฯƒs

D

t

ฯƒs

ฯƒs

D

t

c

c

Consider the vessel to have a wall thickness t , inner diameter

D , and subjected to an internal pressure p. A small element of the vessel that is sufficiently removed and oriented as shown, is subjected to normal stress ฯƒS. If the spherical vessel is cut in

half by plane c-c , the resulting free-body diagram is shown.

Consider the wooden tank having an inner diameter D , and subjected to an internal pressure p that developed within the vessel by a contained fluid. The staves of wooden tank is bound together by steel hoops having a cross-sectional area AH and allowable stress ฯƒH. The spacing s can be determined by considering the vessel to be sectioned by planes a-a , b-b , and c-c.

c

c

a

a

b

b

s s

D

Consider the wooden tank having an inner diameter D , and subjected to an internal pressure p that developed within the vessel by a contained fluid. The staves of wooden tank is bound together by steel hoops having a cross-sectional area AH and allowable stress ฯƒH. The spacing s can be determined by considering the vessel to be sectioned by planes a-a , b-b , and c-c.

ฯƒH

p D

ฯƒH

AH

AH

s /2 s /

๐ป

๐ป

Where: s = spacing of hoops, mm ฯƒH = allowable hoop stress, MPa AH = cross-sectional area of the hoop, mm^2 p = the internal pressure developed by the contained gas or fluid, MPa D = the inner diameter of the cylindrical vessel, mm

z

y

x

F 1

F 2

= ฯƒH ( AH )

= p^ ( Ds )

F 1 = ฯƒ

H ( AH )

Determine the required thickness of the 450 mm diameter steel pipe to carry a maximum pressure of 5500 kPa if the allowable stress of steel is 124 MPa. Solution ๐œŽ๐‘ก = ๐‘๐ท 2๐‘ก 124 ๐‘€๐‘ƒ๐‘Ž = ( 5. 5 MPa)( 450 mm ) 2 (๐‘ก) ๐‘ก = 9. 980 mm ๐œŽ๐ฟ = ๐‘๐ท 4๐‘ก 124 ๐‘€๐‘ƒ๐‘Ž = ( 5. 5 MPa)( 450 mm ) 4 (๐‘ก) ๐‘ก = 4. 990 mm

A thin walled hallow sphere 3.5 m in diameter holds helium gas at 1700 kPa. Determine the minimum wall thickness of the sphere if the allowable stress is 60 MPa. Solution ๐œŽ๐‘† = ๐‘๐ท 4๐‘ก 60 ๐‘€๐‘ƒ๐‘Ž = ( 1. 7 MPa)( 3500 mm ) 4 (๐‘ก) ๐‘ก = 24. 792 mm