Torsion constant

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The torsion constant is a geometrical property of a bar'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. The torsion constant, together with material properties and length, describes a bar's torsional stiffness. The SI unit for torsion constant is m4.

History[edit]

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 planar 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 where warping takes place.[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-sections always have warping deformations that require numerical methods to allow for the exact calculation of the torsion constant.[2]

The torsional stiffness of beams with non-circular cross sections is significantly increased if the warping of the end sections is restrained by, for example, stiff end blocks.[3]

Partial Derivation[edit]

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

where

is the angle of twist in radians
T is the applied torque
L is the beam length
J is the torsional constant
G is the Modulus of rigidity (shear modulus) of the material

TorsionConstantBar.svg

Examples for specific uniform cross-sectional shapes[edit]

Circle[edit]

[4]

where

r is the radius

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

alternatively write: [4] where

D is the Diameter

Ellipse[edit]

[5][6]

where

a is the major radius
b is the minor radius

Square[edit]

[7]

where

a is half the side length

Rectangle[edit]

where

a is the length of the long side
b is the length of the short side
is found from the following table:
a/b
1.0 0.141
1.5 0.196
2.0 0.229
2.5 0.249
3.0 0.263
4.0 0.281
5.0 0.291
6.0 0.299
10.0 0.312
0.333

[8]

Alternatively the following equation can be used with an error of not greater than 4%:

[5]

Thin walled open tube of uniform thickness[edit]

[9]
t is the wall thickness
U is the length of the median boundary (perimeter of median cross section)

Circular thin walled open tube of uniform thickness (approximation)[edit]

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

[10]
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.

Commercial Products[edit]

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

References[edit]

  1. ^ Archie Higdon et al. "Mechanics of Materials, 4th edition".
  2. ^ Advanced structural mechanics, 2nd Edition, David Johnson
  3. ^ The Influence and Modelling of Warping Restraint on Beams
  4. ^ a b "Area Moment of Inertia." From MathWorld--A Wolfram Web Resource. http://mathworld.wolfram.com/AreaMomentofInertia.html
  5. ^ a b Roark's Formulas for stress & Strain, 7th Edition, Warren C. Young & Richard G. Budynas
  6. ^ Continuum Mechanics, Fridtjov Irjens, Springer 2008, p238, ISBN 978-3-540-74297-5
  7. ^ Torsion Equations, Roy Beardmore, http://www.roymech.co.uk/Useful_Tables/Torsion/Torsion.html
  8. ^ Advanced Strength and Applied Elasticity, Ugural & Fenster, Elsevier, ISBN 0-444-00160-3
  9. ^ Advanced Mechanics of Materials, Boresi, John Wiley & Sons, ISBN 0-471-55157-0
  10. ^ Roark's Formulas for stress & Strain, 6th Edition, Warren C. Young