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3Thin Walled
Pressure Vessels
ASEN 3112 - Structures
ASEN 3112 Lecture 3 – Slide 1
Spherical and Cylindrical Pressure Vessels
ASEN 3112 - Structures
ASEN 3112 Lecture 3 – Slide 2
Thin Wall Cylindrical Pressure Vessel:Wall Stress Assumptions
ASEN 3112 - Structures
θx xθ
Free surface: σ = 0, τ = 0, τ = 0rθrr rx Wall thickness t
xr rx
rrσ inside body neglected since it varies from −p to 0 over wall, which is << σ & << σ
Zero because of thin body and τ = τ
θr rθ
Zero becauseτ = τ Zero
becauseτ = τ
Zero because of axisymmetry and no torque
rθ rx
No tangential forcesbecause τ = 0 & τ =0
θrΑ
Βτxr
xxσ : axial stress
xx
τxθ
θxτ
θrτ
θθσ : hoop (a.k.a. circumferential) stress
θθ
C
D
2Rx
ASEN 3112 Lecture 3 – Slide 3
Thin Wall Cylindrical Pressure Vessel:Free Body Diagrams for Hoop and Axial Stress
ASEN 3112 - Structures
t σ (2πR t)xx
dx
(a) (b) (c)
p(πR )2
σ θθ
σ θθ
σ xxσ xx
θrx
~2Rσ t dxθθ
σ t dxθθ
p 2R dx
Both interior and exterior vessel radii can be taken as R, since t << R
ASEN 3112 Lecture 3 – Slide 4
Thin Wall Cylindrical Pressure Vessel:Result for Wall Stress Distribution
Stress matrix at any wall point in cylidrical coordinates (x , θ, r ):
Nonzero wall stress component in terms of the data (p,R,t)
Hoop stress is twice axial stress, and will control the design
[σxx 0 00 σ
θθ
θθ 00 0 0
]Note: this is a plane stressstate
σθθ = p R
tσxx = p R
2t= 1
2 σ
ASEN 3112 - Structures
ASEN 3112 Lecture 3 – Slide 5
σ (2πR t)
p (πR )2
t
~2R
x
y
z
rφ
θ
σ θθσ φφ
σ φφ
σ θθ
Thin Wall Spherical Pressure Vessel:Free Body Diagram for Wall Stress
ASEN 3112 - Structures
ASEN 3112 Lecture 3 – Slide 6
[σ 0 00 σ 00 0 0
]
σ = p R
2t
Thin Wall Spherical Pressure Vessel:Result for Wall Stress Distribution
Stress matrix at any wall point in spherical coordinates
Nonzero wall stress component in terms of the data (p,R,t)
ASEN 3112 - Structures
ASEN 3112 Lecture 3 – Slide 7
Why A Spherical Pressure Vessel is MoreStructurally Efficient Than A Cylindrical One
ASEN 3112 - Structures
pp
σ
σ
σ
σ
σ
(a) Spherical vessel wall (b) Cylindrical vessel wall
σ (axial)xxσxx
θθ
σ (hoop, a.k.a.circumferential)
θθ
ASEN 3112 Lecture 3 – Slide 8
Thin Wall Cylindrical Pressure Vessel:Watch Out For End Cap Effects
ASEN 3112 - Structures
0.35 mm
0.15 mm
t
t
0.20 mm
0.35 mm
(a) Deformed shape
(b) Detail A
(c) Deformation of the same cylindrical pressure vessel at a flat head
A
R = 1000 mm
ASEN 3112 Lecture 3 – Slide 9
Gap
t 45
Joining Vessel Wall Pieces By Welds
Fair (eccentricity disturbsmembrane state) but cheap
Better but more expensive
ASEN 3112 - Structures
ASEN 3112 Lecture 3 – Slide 10
N = σ A = π σ /4bolt bolt bolt bolt
N = p π Rlid2
Design of Lid-Bolted Thin-Wall Cylindrical TankExample Worked Out in Vable's Book and Lecture Text
ASEN 3112 - Structures
ASEN 3112 Lecture 3 – Slide 11