Torsion constant

From Wikipedia, the free encyclopedia
Jump to: navigation, search

The torsion constant is a geometrical property of a beam's cross-section which is involved in the relationship between angle of twist and applied torque along the axis of the bar, for a homogeneous linear-elastic bar. That is, the torsion constant describes a beam's torsional stiffness.

Contents

[edit] History

In 1820, the French engineer A. Duleau derived analytically that the torsion constant of a beam is identical to the second moment of area normal to the section Jzz, which has an exact analytic equation, by assuming that a plane section before twisting remains plane after twisting, and a diameter remains a straight line. Unfortunately, that assumption is correct only in beams with circular cross-sections, and is incorrect for any other shape.[1]

For non-circular cross-sections, there are no exact analytical equations for finding the torsion constant. However approximate solutions have been found for many shapes. Non-circular cross-section always have warping deformations that require numerical methods to allow the exact calculation of the torsion constant.[2]

[edit] Partial Derivation

For a beam of uniform cross-section along its length:

\theta = \frac{TL}{JG}

where

θ is the angle of twist in radians
T is the applied torque
L is the beam length
J is the torsion constant (also referred to as torsional stiffness)
G is the Modulus of rigidity (shear modulus) of the material

TorsionConstantBar.png

[edit] Examples for specific uniform cross-sectional shapes

[edit] Circle

J = \frac{\pi r^4}{2}[3]

where

r is the radius

This is identical to the second moment of area Jzz and is exact.

[edit] Ellipse

J = \frac{\pi a^3 b^3}{a^2 + b^2}[4][5]

where

a is the major radius
b is the minor radius

[edit] Square

J = \,2.25 a^4[6]

where

2a is the side length

[edit] Thin walled closed tube of uniform thickness

J = \frac{4A^2t}{U}[3]
A is the mean of the areas enclosed by the inner and outer boundaries
t is the wall thickness
U is the length of the median boundary

[edit] Thin walled open tube of uniform thickness

J = \frac{1}{3}U t^3[7]
t is the wall thickness
U is the length of the median boundary

[edit] Circular thin walled open tube of uniform thickness

This is a tube with a slit cut longitudinally through its wall.

J = \frac{2}{3} \pi r t^3[3]
t is the wall thickness
r is the mean radius

This is derived from the above equation for an arbitrary thin walled open tube of uniform thickness.

[edit] Commercial Products

There are a number specialized software tools to calculate the torsion constant using the finite element method.

[edit] References

  1. ^ Archie Higdon et. al. "Mechanics of Materials, 4th edition".
  2. ^ Advanced structural mechanics, 2nd Edition, David Johnson
  3. ^ a b c Roark's Formulas for stress & Strain, 6th Edition, Warren C. Young
  4. ^ Roark's Formulas for stress & Strain, 7th Edition, Warren C. Young & Richard G. Budynas
  5. ^ Continuum Mechanics, Fridtjov Irjens, Springer 2008, p238, ISBN 978-3-540-74297-5
  6. ^ Torsion Equations, Roy Beardmore, http://www.roymech.co.uk/Useful_Tables/Torsion/Torsion.html
  7. ^ Advanced Mechanics of Materials, Boresi, John Wiley & Sons, ISBN 0-471-55157-0
Personal tools
Namespaces
Variants
Actions
Navigation
Interaction
Toolbox
Print/export