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Buckling Calculators







Buckling of Tube

In this calculation, a cylindrical shell with a diameter D and thickness s is considered. Based on the results of calculations, the minimum uniformly distributed critical load of the first form of stability loss P acting on the outer surface of the shell is determined. The edges of the shell are fixed and retain their circular shape when loaded.

For the calculation, the elastic modulus E and Poisson's ratio ν of the tube should be specified.

Buckling of cylindrical shell
Elastic stability of cylindrical shell

INITIAL DATA

D - Tube diameter;


s - Tube wall thickness;


L - Tube length. Tube ends held circular;


E - Young's modulus;


ν - Poisson's ratio.

RESULTS DATA

P - Critical pressure of buckling on the external surface of the shell.

Tube diameter (D)

Wall thickness (s)

Tube length (L)

Young's modulus (E)

Poisson ratio (ν)

Critical pressure (P)

BASIC FORMULAS

Critical pressure P:

P = [1.6Es2 / LD]*[(1 / (1-ν2))3*(s2 / 0.25D2)]0.25

INITIAL DATA

D - Tube diameter;


s - Tube wall thickness;


L - Tube length. Tube ends held circular;


E - Young's modulus;


ν - Poisson's ratio.

RESULTS DATA

P - Critical pressure of buckling on the external surface of the shell.

MATERIALS PROPERTIES

Material

Young’s modulus

Pa (psi)

Poisson’s ratio

Steel

1.86÷2.1×1011 (2.7÷3.05×107)

0.25÷0.33

Cast iron

0.78÷1.47×1011 (1.1÷2.1×107)

0.23÷0.27

Copper

1.0÷1.3×1011 (1.45÷1.9×107)

0.34

Tin bronze

0.74÷1.22×1011 (1.1÷1.8×107)

0.32÷0.35

Brass

0.98÷1.08×1011 (1.4÷1.6×107)

0.32÷0.34

Aluminum alloy

0.7×1011 (1.0×107)

0.33

Magnesium alloy

0.4÷0.44×1011 (5.8÷6.4×106)

0.34

Nickel

2.5×1011 (3.6×107)

0.33

Titanium

1.16×1011 (1.7×107)

0.32

Lead

0.15÷0.2×1011 (2.2÷2.9×106)

0.42

Zinc

0.78×1011 (1.1×107)

0.27

Glass

4.9÷5.9×1010 (7.1÷8.5×106)

0.24÷0.27

Concrete

1.48÷2.25×1010 (2.1÷3.3×106)

0.16÷0.18

Wood (along the grain)

8.8÷15.7×1010 (12.8÷22.8×106)

-

Wood (across the grain)

3.9÷9.8×1010 (5.7÷14.2×106)

-

Nylon

1.03×1010 (1.5×106)

-

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