The
torsion constant is a geometrical property of a beam's cross-section which determines the relationship between angle of twist and applied torque.
For a beam of uniform cross-section along its length:
is the angle of twist in radians
T is the applied torque
L is the beam length
J is the torsion constant
G is the modulus of rigidity of the material
For non-circular cross-sections, there are no exact analytical equations for finding J. Approximate solutions have been found for many shapes.
Examples for specific cross-sectional shapes
Circle
r is the radius
This is identical to the
polar moment of inertia and is exact.
Hollow concentric circular tube
is the outer radius
is the inner radius
This is identical to the
polar moment of inertia and is exact.
Square
a is the side length
Rectangle
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 |
Alternatively the following equation can be used with an error of not greater than 4%:
Thin walled closed tube of uniform thickness
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
Thin walled open tube of uniform thickness
t is the wall thickness
U is the length of the median boundary
Circular thin walled open tube of uniform thickness
This is a tube with a slit cut longitudinally through its wall.
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.
References